function Out=XSteam(fun,In1,In2) // Water and steam properties according to IAPWS IF-97 * //*********************************************************************************************************** //* Water and steam properties according to IAPWS IF-97 * //* By Magnus Holmgren, www.x-eng.com * //* The steam tables are free and provided as is. * //* We take no responsibilities for any errors in the code or damage thereby. * //* You are free to use, modify and distribute the code as long as authorship is properly acknowledged. * //* Please notify me at magnus@x-eng.com if the code is used in commercial applications * //*********************************************************************************************************** //------------------------------------------------------------------------------// // Translated to Scilab format from XSteam.m using m2sci.pl at 21:24 15/8/2006. // Torbjørn Pettersen, torbjorn.pettersen.at.broadpark.no //------------------------------------------------------------------------------// // // XSteam provides accurate steam and water properties from 0 - 1000 bar and from 0 - 2000 deg C according to // the standard IAPWS IF-97. For accuracy of the functions in different regions see IF-97 (www.iapws.org) // // *** Using XSteam ***************************************************************************************** //XSteam take 2 or 3 arguments. The first argument must always be the steam table function you want to use. //The other arguments are the inputs to that function. //Example: XSteam('h_pt',1,20) Returns the enthalpy of water at 1 bar and 20 degC //Example: XSteam('TSat_p',1) Returns the saturation temperature of water at 1 bar. //For a list of valid Steam Table functions se bellow or the XSteam macros for MS Excel. // //*** Nomenclature ****************************************************************************************** // First the wanted property then a _ then the wanted input properties. // Example. T_ph is temperature as a function of pressure and enthalpy. // For a list of valid functions se bellow or XSteam for MS Excel. // T Temperature (deg C) // p Pressure (bar) // h Enthalpy (kJ/kg) // v Specific volume (m3/kg) // rho Density // s Specific entropy // u Specific internal energy // Cp Specific isobaric heat capacity // Cv Specific isochoric heat capacity // w Speed of sound // my Viscosity // tc Thermal Conductivity // st Surface Tension // x Vapour fraction // vx Vapour Volume Fraction // //*** Valid Steam table functions. **************************************************************************** // //Temperature //Tsat_p Saturation temperature //T_ph Temperture as a function of pressure and enthalpy //T_ps Temperture as a function of pressure and entropy //T_hs Temperture as a function of enthalpy and entropy // //Pressure //psat_T Saturation pressure //p_hs Pressure as a function of h and s. //p_hrho Pressure as a function of h and rho. Very unaccurate for solid water region since it's almost incompressible! // //Enthalpy //hV_p Saturated vapour enthalpy //hL_p Saturated liquid enthalpy //hV_T Saturated vapour enthalpy //hL_T Saturated liquid enthalpy //h_pT Entalpy as a function of pressure and temperature. //h_ps Entalpy as a function of pressure and entropy. //h_px Entalpy as a function of pressure and vapour fraction //h_prho Entalpy as a function of pressure and density. Observe for low temperatures (liquid) this equation has 2 solutions. //h_Tx Entalpy as a function of temperature and vapour fraction // //Specific volume //vV_p Saturated vapour volume //vL_p Saturated liquid volume //vV_T Saturated vapour volume //vL_T Saturated liquid volume //v_pT Specific volume as a function of pressure and temperature. //v_ph Specific volume as a function of pressure and enthalpy //v_ps Specific volume as a function of pressure and entropy. // //Density //rhoV_p Saturated vapour density //rhoL_p Saturated liquid density //rhoV_T Saturated vapour density //rhoL_T Saturated liquid density //rho_pT Density as a function of pressure and temperature. //rho_ph Density as a function of pressure and enthalpy //rho_ps Density as a function of pressure and entropy. // //Specific entropy //sV_p Saturated vapour entropy //sL_p Saturated liquid entropy //sV_T Saturated vapour entropy //sL_T Saturated liquid entropy //s_pT Specific entropy as a function of pressure and temperature (Returns saturated vapour entalpy if mixture.) //s_ph Specific entropy as a function of pressure and enthalpy // //Specific internal energy //uV_p Saturated vapour internal energy //uL_p Saturated liquid internal energy //uV_T Saturated vapour internal energy //uL_T Saturated liquid internal energy //u_pT Specific internal energy as a function of pressure and temperature. //u_ph Specific internal energy as a function of pressure and enthalpy //u_ps Specific internal energy as a function of pressure and entropy. // //Specific isobaric heat capacity //CpV_p Saturated vapour heat capacity //CpL_p Saturated liquid heat capacity //CpV_T Saturated vapour heat capacity //CpL_T Saturated liquid heat capacity //Cp_pT Specific isobaric heat capacity as a function of pressure and temperature. //Cp_ph Specific isobaric heat capacity as a function of pressure and enthalpy //Cp_ps Specific isobaric heat capacity as a function of pressure and entropy. // //Specific isochoric heat capacity //CvV_p Saturated vapour isochoric heat capacity //CvL_p Saturated liquid isochoric heat capacity //CvV_T Saturated vapour isochoric heat capacity //CvL_T Saturated liquid isochoric heat capacity //Cv_pT Specific isochoric heat capacity as a function of pressure and temperature. //Cv_ph Specific isochoric heat capacity as a function of pressure and enthalpy //Cv_ps Specific isochoric heat capacity as a function of pressure and entropy. // //Speed of sound //wV_p Saturated vapour speed of sound //wL_p Saturated liquid speed of sound //wV_T Saturated vapour speed of sound //wL_T Saturated liquid speed of sound //w_pT Speed of sound as a function of pressure and temperature. //w_ph Speed of sound as a function of pressure and enthalpy //w_ps Speed of sound as a function of pressure and entropy. // //Viscosity //Viscosity is not part of IAPWS Steam IF97. Equations from //"Revised Release on the IAPWS Formulation 1985 for the Viscosity of Ordinary Water Substance", 2003 are used. //Viscosity in the mixed region (4) is interpolated according to the density. This is not true since it will be two fases. //my_pT Viscosity as a function of pressure and temperature. //my_ph Viscosity as a function of pressure and enthalpy //my_ps Viscosity as a function of pressure and entropy. // //Thermal Conductivity //Revised release on the IAPS Formulation 1985 for the Thermal Conductivity of ordinary water substance (IAPWS 1998) //tcL_p Saturated vapour thermal conductivity //tcV_p Saturated liquid thermal conductivity //tcL_T Saturated vapour thermal conductivity //tcV_T Saturated liquid thermal conductivity //tc_pT Thermal conductivity as a function of pressure and temperature. //tc_ph Thermal conductivity as a function of pressure and enthalpy //tc_hs Thermal conductivity as a function of enthalpy and entropy // //Surface tension //st_T Surface tension for two phase water/steam as a function of T //st_p Surface tension for two phase water/steam as a function of T //Vapour fraction //x_ph Vapour fraction as a function of pressure and enthalpy //x_ps Vapour fraction as a function of pressure and entropy. // //Vapour volume fraction //vx_ph Vapour volume fraction as a function of pressure and enthalpy //vx_ps Vapour volume fraction as a function of pressure and entropy. //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// //*Contents. //*1 Calling functions //*1.1 //*1.2 Temperature (T) //*1.3 Pressure (p) //*1.4 Enthalpy (h) //*1.5 Specific Volume (v) //*1.6 Density (rho) //*1.7 Specific entropy (s) //*1.8 Specific internal energy (u) //*1.9 Specific isobaric heat capacity (Cp) //*1.10 Specific isochoric heat capacity (Cv) //*1.11 Speed of sound //*1.12 Viscosity //*1.13 Prandtl //*1.14 Kappa //*1.15 Surface tension //*1.16 Heat conductivity //*1.17 Vapour fraction //*1.18 Vapour Volume Fraction // //*2 IAPWS IF 97 Calling functions //*2.1 Functions for region 1 //*2.2 Functions for region 2 //*2.3 Functions for region 3 //*2.4 Functions for region 4 //*2.5 Functions for region 5 // //*3 Region Selection //*3.1 Regions as a function of pT //*3.2 Regions as a function of ph //*3.3 Regions as a function of ps //*3.4 Regions as a function of hs // //4 Region Borders //4.1 Boundary between region 1 and 3. //4.2 Region 3. pSat_h and pSat_s //4.3 Region boundary 1to3 and 3to2 as a functions of s // //5 Transport properties //5.1 Viscosity (IAPWS formulation 1985) //5.2 Thermal Conductivity (IAPWS formulation 1985) //5.3 Surface Tension // //6 Units // //7 Verification //7.1 Verifiy region 1 //7.2 Verifiy region 2 //7.3 Verifiy region 3 //7.4 Verifiy region 4 //7.5 Verifiy region 5 //*********************************************************************************************************** //*1 Calling functions * //*********************************************************************************************************** //*********************************************************************************************************** //*1.1 fun=mtlb_lower(fun); select fun //*********************************************************************************************************** //*1.2 Temperature case 'tsat_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 Out = fromSIunit_T(T4_p(p)); else Out = %nan; end case 'tsat_s' s = toSIunit_s(In1); if s > -0.0001545495919 & s < 9.155759395 ps = p4_s(s); Out = fromSIunit_T(T4_p(ps)); else Out = %nan; end case 't_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 Out = fromSIunit_T(T1_ph(p, h)); case 2 Out = fromSIunit_T(T2_ph(p, h)); case 3 Out = fromSIunit_T(T3_ph(p, h)); case 4 Out = fromSIunit_T(T4_p(p)); case 5 Out = fromSIunit_T(T5_ph(p, h)); else Out = %nan; end case 't_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); Region = region_ps(p, s); select Region case 1 Out = fromSIunit_T(T1_ps(p, s)); case 2 Out = fromSIunit_T(T2_ps(p, s)); case 3 Out = fromSIunit_T(T3_ps(p, s)); case 4 Out = fromSIunit_T(T4_p(p)); case 5 Out = fromSIunit_T(T5_ps(p, s)); else Out = %nan; end case 't_hs' h = toSIunit_h(In1); s = toSIunit_s(In2); Region = region_hs(h, s); select Region case 1 p1 = p1_hs(h, s); Out = fromSIunit_T(T1_ph(p1, h)); case 2 p2 = p2_hs(h, s); Out = fromSIunit_T(T2_ph(p2, h)); case 3 p3 = p3_hs(h, s); Out = fromSIunit_T(T3_ph(p3, h)); case 4 Out = fromSIunit_T(T4_hs(h, s)); case 5 error('functions of hs is not avlaible in region 5'); else Out = %nan; end //*********************************************************************************************************** //*1.3 Pressure (p) case 'psat_t' T = toSIunit_T(In1); if T < 647.096 & T > 273.15 Out = fromSIunit_p(p4_T(T)); else Out = %nan; end case 'psat_s' s = toSIunit_s(In1); if s > -0.0001545495919 & s < 9.155759395 Out = fromSIunit_p(p4_s(s)); else Out = %nan; end case 'p_hs' h = toSIunit_h(In1); s = toSIunit_s(In2); Region = region_hs(h, s); select Region case 1 Out = fromSIunit_p(p1_hs(h, s)); case 2 Out = fromSIunit_p(p2_hs(h, s)); case 3 Out = fromSIunit_p(p3_hs(h, s)); case 4 tSat = T4_hs(h, s); Out = fromSIunit_p(p4_T(tSat)); case 5 error('functions of hs is not avlaible in region 5'); else Out = %nan; end case 'p_hrho' h=In1; rho=In2; //Not valid for water or sumpercritical since water rho does not change very much with p. //Uses iteration to find p. High_Bound = fromSIunit_p(100); Low_Bound = fromSIunit_p(0.000611657); ps = fromSIunit_p(10); rhos = 1 / XSteam('v_ph',ps, h); while abs(rho - rhos) > 0.0000001 rhos = 1 / XSteam('v_ph',ps, h); if rhos >= rho High_Bound = ps; else Low_Bound = ps; end ps = (Low_Bound + High_Bound) / 2; end Out = ps; //*********************************************************************************************************** //*1.4 Enthalpy (h) case 'hv_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 Out = fromSIunit_h(h4V_p(p)); else Out = %nan; end case 'hl_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 Out = fromSIunit_h(h4L_p(p)); else Out = %nan; end case 'hv_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 p = p4_T(T); Out = fromSIunit_h(h4V_p(p)); else Out = %nan; end case 'hl_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 p = p4_T(T); Out = fromSIunit_h(h4L_p(p)); else Out = %nan; end case 'h_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 1 Out = fromSIunit_h(h1_pT(p, T)); case 2 Out = fromSIunit_h(h2_pT(p, T)); case 3 Out = fromSIunit_h(h3_pT(p, T)); case 4 Out = %nan; case 5 Out = fromSIunit_h(h5_pT(p, T)); else Out = %nan; end case 'h_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); Region = region_ps(p, s); select Region case 1 Out = fromSIunit_h(h1_pT(p, T1_ps(p, s))); case 2 Out = fromSIunit_h(h2_pT(p, T2_ps(p, s))); case 3 Out = fromSIunit_h(h3_rhoT(1 / v3_ps(p, s), T3_ps(p, s))); case 4 xs = x4_ps(p, s); Out = xs * h4V_p(p) + (1 - xs) * h4L_p(p); case 5 Out = fromSIunit_h(h5_pT(p, T5_ps(p, s))); else Out = %nan; end case 'h_px' p = toSIunit_p(In1); x = toSIunit_x(In2); if x > 1 | x < 0 | p >= 22.064 Out = %nan; return end hL = h4L_p(p); hV = h4V_p(p); Out = hL + x * (hV - hL); case 'h_prho' p = toSIunit_p(In1); rho = 1 / toSIunit_v(1 / In2); Region = Region_prho(p, rho); select Region case 1 Out = fromSIunit_h(h1_pT(p, T1_prho(p, rho))); case 2 Out = fromSIunit_h(h2_pT(p, T2_prho(p, rho))); case 3 Out = fromSIunit_h(h3_rhoT(rho, T3_prho(p, rho))); case 4 if p < 16.529 vV = v2_pT(p, T4_p(p)); vL = v1_pT(p, T4_p(p)); else vV = v3_ph(p, h4V_p(p)); vL = v3_ph(p, h4L_p(p)); end hV = h4V_p(p); hL = h4L_p(p); x = (1 / rho - vL) / (vV - vL); Out = fromSIunit_h((1 - x) * hL + x * hV); case 5 Out = fromSIunit_h(h5_pT(p, T5_prho(p, rho))); else Out = %nan; end case 'h_tx' T = toSIunit_T(In1); x = toSIunit_x(In2); if x > 1 | x < 0 | T >= 647.096 Out = %nan; return end p = p4_T(T); hL = h4L_p(p); hV = h4V_p(p); Out = hL + x * (hV - hL); //*********************************************************************************************************** //*1.5 Specific Volume (v) case 'vv_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_v(v2_pT(p, T4_p(p))); else Out = fromSIunit_v(v3_ph(p, h4V_p(p))); end else Out = %nan; end // if fun(1)=='r' // Out=1/Out; // end case 'rhov_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 then if p < 16.529 then Out = fromSIunit_v(v2_pT(p, T4_p(p))); else Out = fromSIunit_v(v3_ph(p, h4V_p(p))); end else Out = %nan; end // if fun(1)=='r' Out=1/Out; // end case 'vl_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_v(v1_pT(p, T4_p(p))); else Out = fromSIunit_v(v3_ph(p, h4L_p(p))); end else Out = %nan; end // if fun(1)=='r' // Out=1/Out; // end case 'rhol_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_v(v1_pT(p, T4_p(p))); else Out = fromSIunit_v(v3_ph(p, h4L_p(p))); end else Out = %nan; end // if fun(1)=='r' Out=1/Out; // end case 'vv_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_v(v2_pT(p4_T(T), T)); else Out = fromSIunit_v(v3_ph(p4_T(T), h4V_p(p4_T(T)))); end else Out = %nan; end // if fun(1)=='r' // Out=1/Out; // end case 'rhov_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_v(v2_pT(p4_T(T), T)); else Out = fromSIunit_v(v3_ph(p4_T(T), h4V_p(p4_T(T)))); end else Out = %nan; end // if fun(1)=='r' Out=1/Out; // end case 'vl_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_v(v1_pT(p4_T(T), T)); else Out = fromSIunit_v(v3_ph(p4_T(T), h4L_p(p4_T(T)))); end else Out = %nan; end // if fun(1)=='r' // Out=1/Out; // end case 'rhol_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_v(v1_pT(p4_T(T), T)); else Out = fromSIunit_v(v3_ph(p4_T(T), h4L_p(p4_T(T)))); end else Out = %nan; end // if fun(1)=='r' Out=1/Out; // end case 'rho_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 1 Out = fromSIunit_v(v1_pT(p, T)); case 2 Out = fromSIunit_v(v2_pT(p, T)); case 3 Out = fromSIunit_v(v3_ph(p, h3_pT(p, T))); case 4 Out = %nan; case 5 Out = fromSIunit_v(v5_pT(p, T)); else Out = %nan; end // if fun(1)=='r' Out=1/Out; // end case 'v_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 1 Out = fromSIunit_v(v1_pT(p, T)); case 2 Out = fromSIunit_v(v2_pT(p, T)); case 3 Out = fromSIunit_v(v3_ph(p, h3_pT(p, T))); case 4 Out = %nan; case 5 Out = fromSIunit_v(v5_pT(p, T)); else Out = %nan; end // if fun(1)=='r' // Out=1/Out; // end case 'rho_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 Out = fromSIunit_v(v1_pT(p, T1_ph(p, h))); case 2 Out = fromSIunit_v(v2_pT(p, T2_ph(p, h))); case 3 Out = fromSIunit_v(v3_ph(p, h)); case 4 xs = x4_ph(p, h); if p < 16.529 v4v = v2_pT(p, T4_p(p)); v4L = v1_pT(p, T4_p(p)); else v4v = v3_ph(p, h4V_p(p)); v4L = v3_ph(p, h4L_p(p)); end Out = fromSIunit_v((xs * v4v + (1 - xs) * v4L)); case 5 Ts = T5_ph(p, h); Out = fromSIunit_v(v5_pT(p, Ts)); else Out = %nan; end // if fun(1)=='r' Out=1/Out; // end case 'v_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 Out = fromSIunit_v(v1_pT(p, T1_ph(p, h))); case 2 Out = fromSIunit_v(v2_pT(p, T2_ph(p, h))); case 3 Out = fromSIunit_v(v3_ph(p, h)); case 4 xs = x4_ph(p, h); if p < 16.529 v4v = v2_pT(p, T4_p(p)); v4L = v1_pT(p, T4_p(p)); else v4v = v3_ph(p, h4V_p(p)); v4L = v3_ph(p, h4L_p(p)); end Out = fromSIunit_v((xs * v4v + (1 - xs) * v4L)); case 5 Ts = T5_ph(p, h); Out = fromSIunit_v(v5_pT(p, Ts)); else Out = %nan; end // if fun(1)=='r' // Out=1/Out; // end case 'v_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); Region = region_ps(p, s); select Region case 1 Out = fromSIunit_v(v1_pT(p, T1_ps(p, s))); case 2 Out = fromSIunit_v(v2_pT(p, T2_ps(p, s))); case 3 Out = fromSIunit_v(v3_ps(p, s)); case 4 xs = x4_ps(p, s); if p < 16.529 v4v = v2_pT(p, T4_p(p)); v4L = v1_pT(p, T4_p(p)); else v4v = v3_ph(p, h4V_p(p)); v4L = v3_ph(p, h4L_p(p)); end Out = fromSIunit_v((xs * v4v + (1 - xs) * v4L)); case 5 Ts = T5_ps(p, s); Out = fromSIunit_v(v5_pT(p, Ts)); else Out = %nan; end // if fun(1)=='r' // Out=1/Out; // end case 'rho_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); Region = region_ps(p, s); select Region case 1 Out = fromSIunit_v(v1_pT(p, T1_ps(p, s))); case 2 Out = fromSIunit_v(v2_pT(p, T2_ps(p, s))); case 3 Out = fromSIunit_v(v3_ps(p, s)); case 4 xs = x4_ps(p, s); if p < 16.529 v4v = v2_pT(p, T4_p(p)); v4L = v1_pT(p, T4_p(p)); else v4v = v3_ph(p, h4V_p(p)); v4L = v3_ph(p, h4L_p(p)); end Out = fromSIunit_v((xs * v4v + (1 - xs) * v4L)); case 5 Ts = T5_ps(p, s); Out = fromSIunit_v(v5_pT(p, Ts)); else Out = %nan; end // if fun(1)=='r' Out=1/Out; // end //*********************************************************************************************************** //*1.6 Density (rho) // Density is calculated as 1/v. Se section 1.5 Volume //*********************************************************************************************************** //*1.7 Specific entropy (s) case 'sv_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_s(s2_pT(p, T4_p(p))); else Out = fromSIunit_s(s3_rhoT(1 / (v3_ph(p, h4V_p(p))), T4_p(p))); end else Out = %nan; end case 'sl_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_s(s1_pT(p, T4_p(p))); else Out = fromSIunit_s(s3_rhoT(1 / (v3_ph(p, h4L_p(p))), T4_p(p))); end else Out = %nan; end case 'sv_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_s(s2_pT(p4_T(T), T)); else Out = fromSIunit_s(s3_rhoT(1 / (v3_ph(p4_T(T), h4V_p(p4_T(T)))), T)); end else Out = %nan; end case 'sl_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_s(s1_pT(p4_T(T), T)); else Out = fromSIunit_s(s3_rhoT(1 / (v3_ph(p4_T(T), h4L_p(p4_T(T)))), T)); end else Out = %nan; end case 's_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 1 Out = fromSIunit_s(s1_pT(p, T)); case 2 Out = fromSIunit_s(s2_pT(p, T)); case 3 hs = h3_pT(p, T); rhos = 1 / v3_ph(p, hs); Out = fromSIunit_s(s3_rhoT(rhos, T)); case 4 Out = %nan; case 5 Out = fromSIunit_s(s5_pT(p, T)); else Out = %nan; end case 's_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 T = T1_ph(p, h); Out = fromSIunit_s(s1_pT(p, T)); case 2 T = T2_ph(p, h); Out = fromSIunit_s(s2_pT(p, T)); case 3 rhos = 1 / v3_ph(p, h); Ts = T3_ph(p, h); Out = fromSIunit_s(s3_rhoT(rhos, Ts)); case 4 Ts = T4_p(p); xs = x4_ph(p, h); if p < 16.529 s4v = s2_pT(p, Ts); s4L = s1_pT(p, Ts); else v4v = v3_ph(p, h4V_p(p)); s4v = s3_rhoT(1 / v4v, Ts); v4L = v3_ph(p, h4L_p(p)); s4L = s3_rhoT(1 / v4L, Ts); end Out = fromSIunit_s((xs * s4v + (1 - xs) * s4L)); case 5 T = T5_ph(p, h); Out = fromSIunit_s(s5_pT(p, T)); else Out = %nan; end //*********************************************************************************************************** //*1.8 Specific internal energy (u) case 'uv_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_u(u2_pT(p, T4_p(p))); else Out = fromSIunit_u(u3_rhoT(1 / (v3_ph(p, h4V_p(p))), T4_p(p))); end else Out = %nan; end case 'ul_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_u(u1_pT(p, T4_p(p))); else Out = fromSIunit_u(u3_rhoT(1 / (v3_ph(p, h4L_p(p))), T4_p(p))); end else Out = %nan; end case 'uv_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_u(u2_pT(p4_T(T), T)); else Out = fromSIunit_u(u3_rhoT(1 / (v3_ph(p4_T(T), h4V_p(p4_T(T)))), T)); end else Out = %nan; end case 'ul_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_u(u1_pT(p4_T(T), T)); else Out = fromSIunit_u(u3_rhoT(1 / (v3_ph(p4_T(T), h4L_p(p4_T(T)))), T)); end else Out = %nan; end case 'u_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 1 Out = fromSIunit_u(u1_pT(p, T)); case 2 Out = fromSIunit_u(u2_pT(p, T)); case 3 hs = h3_pT(p, T); rhos = 1 / v3_ph(p, hs); Out = fromSIunit_u(u3_rhoT(rhos, T)); case 4 Out = %nan; case 5 Out = fromSIunit_u(u5_pT(p, T)); else Out = %nan; end case 'u_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 Ts = T1_ph(p, h); Out = fromSIunit_u(u1_pT(p, Ts)); case 2 Ts = T2_ph(p, h); Out = fromSIunit_u(u2_pT(p, Ts)); case 3 rhos = 1 / v3_ph(p, h); Ts = T3_ph(p, h); Out = fromSIunit_u(u3_rhoT(rhos, Ts)); case 4 Ts = T4_p(p); xs = x4_ph(p, h); if p < 16.529 u4v = u2_pT(p, Ts); u4L = u1_pT(p, Ts); else v4v = v3_ph(p, h4V_p(p)); u4v = u3_rhoT(1 / v4v, Ts); v4L = v3_ph(p, h4L_p(p)); u4L = u3_rhoT(1 / v4L, Ts); end Out = fromSIunit_u((xs * u4v + (1 - xs) * u4L)); case 5 Ts = T5_ph(p, h); Out = fromSIunit_u(u5_pT(p, Ts)); else Out = %nan; end case 'u_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); Region = region_ps(p, s); select Region case 1 Ts = T1_ps(p, s); Out = fromSIunit_u(u1_pT(p, Ts)); case 2 Ts = T2_ps(p, s); Out = fromSIunit_u(u2_pT(p, Ts)); case 3 rhos = 1 / v3_ps(p, s); Ts = T3_ps(p, s); Out = fromSIunit_u(u3_rhoT(rhos, Ts)); case 4 if p < 16.529 uLp = u1_pT(p, T4_p(p)); uVp = u2_pT(p, T4_p(p)); else uLp = u3_rhoT(1 / (v3_ph(p, h4L_p(p))), T4_p(p)); uVp = u3_rhoT(1 / (v3_ph(p, h4V_p(p))), T4_p(p)); end xs = x4_ps(p, s); Out = fromSIunit_u((xs * uVp + (1 - xs) * uLp)); case 5 Ts = T5_ps(p, s); Out = fromSIunit_u(u5_pT(p, Ts)); else Out = %nan; end //*********************************************************************************************************** //*1.9 Specific isobaric heat capacity (Cp) case 'cpv_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_Cp(Cp2_pT(p, T4_p(p))); else Out = fromSIunit_Cp(Cp3_rhoT(1 / (v3_ph(p, h4V_p(p))), T4_p(p))); end else Out = %nan; end case 'cpl_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_Cp(Cp1_pT(p, T4_p(p))); else Out = fromSIunit_Cp(Cp3_rhoT(1 / (v3_ph(p, h4L_p(p))), T4_p(p))); end else Out = %nan; end case 'cpv_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_Cp(Cp2_pT(p4_T(T), T)); else Out = fromSIunit_Cp(Cp3_rhoT(1 / (v3_ph(p4_T(T), h4V_p(p4_T(T)))), T)); end else Out = %nan; end case 'cpl_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_Cp(Cp1_pT(p4_T(T), T)); else Out = fromSIunit_Cp(Cp3_rhoT(1 / (v3_ph(p4_T(T), h4L_p(p4_T(T)))), T)); end else Out = %nan; end case 'cp_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 1 Out = fromSIunit_Cp(Cp1_pT(p, T)); case 2 Out = fromSIunit_Cp(Cp2_pT(p, T)); case 3 hs = h3_pT(p, T); rhos = 1 / v3_ph(p, hs); Out = fromSIunit_Cp(Cp3_rhoT(rhos, T)); case 4 Out = %nan; case 5 Out = fromSIunit_Cp(Cp5_pT(p, T)); else Out = %nan; end case 'cp_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 Ts = T1_ph(p, h); Out = fromSIunit_Cp(Cp1_pT(p, Ts)); case 2 Ts = T2_ph(p, h); Out = fromSIunit_Cp(Cp2_pT(p, Ts)); case 3 rhos = 1 / v3_ph(p, h); Ts = T3_ph(p, h); Out = fromSIunit_Cp(Cp3_rhoT(rhos, Ts)); case 4 Out = %nan; case 5 Ts = T5_ph(p, h); Out = fromSIunit_Cp(Cp5_pT(p, Ts)); else Out = %nan; end case 'cp_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); Region = region_ps(p, s); select Region case 1 Ts = T1_ps(p, s); Out = fromSIunit_Cp(Cp1_pT(p, Ts)); case 2 Ts = T2_ps(p, s); Out = fromSIunit_Cp(Cp2_pT(p, Ts)); case 3 rhos = 1 / v3_ps(p, s); Ts = T3_ps(p, s); Out = fromSIunit_Cp(Cp3_rhoT(rhos, Ts)); case 4 Out = %nan; case 5 Ts = T5_ps(p, s); Out = fromSIunit_Cp(Cp5_pT(p, Ts)); else Out = %nan end //*********************************************************************************************************** //*1.10 Specific isochoric heat capacity (Cv) case 'cvv_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_Cv(Cv2_pT(p, T4_p(p))); else Out = fromSIunit_Cv(Cv3_rhoT(1 / (v3_ph(p, h4V_p(p))), T4_p(p))); end else Out = %nan; end case 'cvl_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_Cv(Cv1_pT(p, T4_p(p))); else Out = fromSIunit_Cv(Cv3_rhoT(1 / (v3_ph(p, h4L_p(p))), T4_p(p))); end else Out = %nan; end case 'cvv_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_Cv(Cv2_pT(p4_T(T), T)); else Out = fromSIunit_Cv(Cv3_rhoT(1 / (v3_ph(p4_T(T), h4V_p(p4_T(T)))), T)); end else Out = %nan; end case 'cvl_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_Cv(Cv1_pT(p4_T(T), T)); else Out = fromSIunit_Cv(Cv3_rhoT(1 / (v3_ph(p4_T(T), h4L_p(p4_T(T)))), T)); end else Out = %nan; end case 'cv_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 1 Out = fromSIunit_Cv(Cv1_pT(p, T)); case 2 Out = fromSIunit_Cv(Cv2_pT(p, T)); case 3 hs = h3_pT(p, T); rhos = 1 / v3_ph(p, hs); Out = fromSIunit_Cv(Cv3_rhoT(rhos, T)); case 4 Out = %nan; case 5 Out = fromSIunit_Cv(Cv5_pT(p, T)); else Out = %nan; end case 'cv_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 Ts = T1_ph(p, h); Out = fromSIunit_Cv(Cv1_pT(p, Ts)); case 2 Ts = T2_ph(p, h); Out = fromSIunit_Cv(Cv2_pT(p, Ts)); case 3 rhos = 1 / v3_ph(p, h); Ts = T3_ph(p, h); Out = fromSIunit_Cv(Cv3_rhoT(rhos, Ts)); case 4 Out = %nan; case 5 Ts = T5_ph(p, h); Out = fromSIunit_Cv(Cv5_pT(p, Ts)); else Out = %nan; end case 'cv_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); Region = region_ps(p, s); select Region case 1 Ts = T1_ps(p, s); Out = fromSIunit_Cv(Cv1_pT(p, Ts)); case 2 Ts = T2_ps(p, s); Out = fromSIunit_Cv(Cv2_pT(p, Ts)); case 3 rhos = 1 / v3_ps(p, s); Ts = T3_ps(p, s); Out = fromSIunit_Cv(Cv3_rhoT(rhos, Ts)); case 4 Out = %nan; //(xs * CvVp + (1 - xs) * CvLp) / Cv_scale - Cv_offset case 5 Ts = T5_ps(p, s); Out = fromSIunit_Cv(Cv5_pT(p, Ts)); else Out = CVErr(xlErrValue); end //*********************************************************************************************************** //*1.11 Speed of sound case 'wv_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_w(w2_pT(p, T4_p(p))); else Out = fromSIunit_w(w3_rhoT(1 / (v3_ph(p, h4V_p(p))), T4_p(p))); end else Out = %nan; end case 'wl_p' p = toSIunit_p(In1); if p > 0.000611657 & p < 22.06395 if p < 16.529 Out = fromSIunit_w(w1_pT(p, T4_p(p))); else Out = fromSIunit_w(w3_rhoT(1 / (v3_ph(p, h4L_p(p))), T4_p(p))); end else Out = %nan; end case 'wv_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_w(w2_pT(p4_T(T), T)); else Out = fromSIunit_w(w3_rhoT(1 / (v3_ph(p4_T(T), h4V_p(p4_T(T)))), T)); end else Out = %nan; end case 'wl_t' T = toSIunit_T(In1); if T > 273.15 & T < 647.096 if T <= 623.15 Out = fromSIunit_w(w1_pT(p4_T(T), T)); else Out = fromSIunit_w(w3_rhoT(1 / (v3_ph(p4_T(T), h4L_p(p4_T(T)))), T)); end else Out = %nan; end case 'w_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 1 Out = fromSIunit_w(w1_pT(p, T)); case 2 Out = fromSIunit_w(w2_pT(p, T)); case 3 hs = h3_pT(p, T); rhos = 1 / v3_ph(p, hs); Out = fromSIunit_w(w3_rhoT(rhos, T)); case 4 Out = %nan; case 5 Out = fromSIunit_w(w5_pT(p, T)); else Out = %nan; end case 'w_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 Ts = T1_ph(p, h); Out = fromSIunit_w(w1_pT(p, Ts)); case 2 Ts = T2_ph(p, h); Out = fromSIunit_w(w2_pT(p, Ts)); case 3 rhos = 1 / v3_ph(p, h); Ts = T3_ph(p, h); Out = fromSIunit_w(w3_rhoT(rhos, Ts)); case 4 Out = %nan; case 5 Ts = T5_ph(p, h); Out = fromSIunit_w(w5_pT(p, Ts)); else Out = %nan; end case 'w_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); Region = region_ps(p, s); select Region case 1 Ts = T1_ps(p, s); Out = fromSIunit_w(w1_pT(p, Ts)); case 2 Ts = T2_ps(p, s); Out = fromSIunit_w(w2_pT(p, Ts)); case 3 rhos = 1 / v3_ps(p, s); Ts = T3_ps(p, s); Out = fromSIunit_w(w3_rhoT(rhos, Ts)); case 4 Out = %nan; //(xs * wVp + (1 - xs) * wLp) / w_scale - w_offset case 5 Ts = T5_ps(p, s); Out = fromSIunit_w(w5_pT(p, Ts)); else Out = %nan; end //*********************************************************************************************************** //*1.12 Viscosity case 'my_pt' p = toSIunit_p(In1); T = toSIunit_T(In2); Region = region_pT(p, T); select Region case 4 Out = %nan; case 1 Out = fromSIunit_my(my_AllRegions_pT(p, T)); case 2 Out = fromSIunit_my(my_AllRegions_pT(p, T)); case 3 Out = fromSIunit_my(my_AllRegions_pT(p, T)); case 5 Out = fromSIunit_my(my_AllRegions_pT(p, T)); else Out = %nan; end case 'my_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); Region = region_ph(p, h); select Region case 1 Out = fromSIunit_my(my_AllRegions_ph(p, h)); case 2 Out = fromSIunit_my(my_AllRegions_ph(p, h)); case 3 Out = fromSIunit_my(my_AllRegions_ph(p, h)); case 5 Out = fromSIunit_my(my_AllRegions_ph(p, h)); case 4 Out = %nan; else Out = %nan; end case 'my_ps' h = XSteam('h_ps',In1, In2); Out = XSteam('my_ph',In1, h); //*********************************************************************************************************** //*1.13 Prandtl case 'pr_pt' Cp = toSIunit_Cp(XSteam('Cp_pT',In1, In2)); my = toSIunit_my(XSteam('my_pT',In1,In2)); tc = toSIunit_tc(XSteam('tc_pT',In1,In2)); Out = Cp * 1000 * my / tc; case 'pr_ph' Cp = toSIunit_Cp(XSteam('Cp_ph',In1, In2)); my = toSIunit_my(XSteam('my_ph',In1,In2)); tc = toSIunit_tc(XSteam('tc_ph',In1,In2)); Out = Cp * 1000 * my / tc; //*********************************************************************************************************** //*1.14 Kappa //*********************************************************************************************************** //*********************************************************************************************************** //*1.15 Surface tension case 'st_t' T = toSIunit_T(In1); Out = fromSIunit_st(Surface_Tension_T(T)); case 'st_p' T = XSteam('Tsat_p',In1); T = toSIunit_T(T); Out = fromSIunit_st(Surface_Tension_T(T)); //*********************************************************************************************************** //*1.16 Thermal conductivity case 'tcl_p' T = XSteam('Tsat_p',In1); v = XSteam('vL_p',In1); p = toSIunit_p(In1); T = toSIunit_T(T); v = toSIunit_v(v); rho = 1 / v; Out = fromSIunit_tc(tc_ptrho(p, T, rho)); case 'tcv_p' ps = In1; T = XSteam('Tsat_p',ps); v = XSteam('vV_p',ps); p = toSIunit_p(In1); T = toSIunit_T(T); v = toSIunit_v(v); rho = 1 / v; Out = fromSIunit_tc(tc_ptrho(p, T, rho)); case 'tcl_t' Ts = In1; p = XSteam('psat_T',Ts); v = XSteam('vL_T',Ts); p = toSIunit_p(p); T = toSIunit_T(Ts); v = toSIunit_v(v); rho = 1 / v; Out = fromSIunit_tc(tc_ptrho(p, T, rho)); case 'tcv_t' Ts = In1; p = XSteam('psat_T',Ts); v = XSteam('vV_T',Ts); p = toSIunit_p(p); T = toSIunit_T(Ts); v = toSIunit_v(v); rho = 1 / v; Out = fromSIunit_tc(tc_ptrho(p, T, rho)); case 'tc_pt' Ts = In2; ps = In1; v = XSteam('v_pT',ps, Ts); p = toSIunit_p(ps); T = toSIunit_T(Ts); v = toSIunit_v(v); rho = 1 / v; Out = fromSIunit_tc(tc_ptrho(p, T, rho)); case 'tc_ph' hs = In2; ps = In1; v = XSteam('v_ph',ps, hs); T = XSteam('T_ph',ps, hs); p = toSIunit_p(ps); T = toSIunit_T(T); v = toSIunit_v(v); rho = 1 / v; Out = fromSIunit_tc(tc_ptrho(p, T, rho)); case 'tc_hs' hs = In1; p = XSteam('p_hs',hs, In2); ps = p; v = XSteam('v_ph',ps, hs); T = XSteam('T_ph',ps, hs); p = toSIunit_p(p); T = toSIunit_T(T); v = toSIunit_v(v); rho = 1 / v; Out = fromSIunit_tc(tc_ptrho(p, T, rho)); //*********************************************************************************************************** //*1.17 Vapour fraction case 'x_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); if p > 0.000611657 & p < 22.06395 Out = fromSIunit_x(x4_ph(p, h)); else Out = %nan; end case 'x_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); if p > 0.000611657 & p < 22.06395 Out = fromSIunit_x(x4_ps(p, s)); else Out = %nan; end //*********************************************************************************************************** //*1.18 Vapour Volume Fraction case 'vx_ph' p = toSIunit_p(In1); h = toSIunit_h(In2); if p > 0.000611657 & p < 22.06395 if p < 16.529 vL = v1_pT(p, T4_p(p)); vV = v2_pT(p, T4_p(p)); else vL = v3_ph(p, h4L_p(p)); vV = v3_ph(p, h4V_p(p)); end xs = x4_ph(p, h); Out = fromSIunit_vx((xs * vV / (xs * vV + (1 - xs) * vL))); else Out = %nan; end case 'vx_ps' p = toSIunit_p(In1); s = toSIunit_s(In2); if p > 0.000611657 & p < 22.06395 if p < 16.529 vL = v1_pT(p, T4_p(p)); vV = v2_pT(p, T4_p(p)); else vL = v3_ph(p, h4L_p(p)); vV = v3_ph(p, h4V_p(p)); end xs = x4_ps(p, s); Out = fromSIunit_vx((xs * vV / (xs * vV + (1 - xs) * vL))); else Out = %nan; end case 'check' err=check(); else error(['Unknown calling function to XSteam, ',fun, ' See help XSteam for valid calling functions']); end //*********************************************************************************************************** //*2 IAPWS IF 97 Calling functions * //*********************************************************************************************************** // //*********************************************************************************************************** //*2.1 Functions for region 1 endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function v1_pT = v1_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation //Eqution 7, Table 3, Page 6 I1 = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 4, 4, 4, 5, 8, 8, 21, 23, 29, 30, 31, 32]; J1 = [-2, -1, 0, 1, 2, 3, 4, 5, -9, -7, -1, 0, 1, 3, -3, 0, 1, 3, 17, -4, 0, 6, -5, -2, 10, -8, -11, -6, -29, -31, -38, -39, -40, -41]; n1 = [0.14632971213167, -0.84548187169114, -3.756360367204, 3.3855169168385, -0.95791963387872, 0.15772038513228, -0.016616417199501, 8.1214629983568E-04, 2.8319080123804E-04, -6.0706301565874E-04, -0.018990068218419, -0.032529748770505, -0.021841717175414, -5.283835796993E-05, -4.7184321073267E-04, -3.0001780793026E-04, 4.7661393906987E-05, -4.4141845330846E-06, -7.2694996297594E-16, -3.1679644845054E-05, -2.8270797985312E-06, -8.5205128120103E-10, -2.2425281908E-06, -6.5171222895601E-07, -1.4341729937924E-13, -4.0516996860117E-07, -1.2734301741641E-09, -1.7424871230634E-10, -6.8762131295531E-19, 1.4478307828521E-20, 2.6335781662795E-23, -1.1947622640071E-23, 1.8228094581404E-24, -9.3537087292458E-26]; R = 0.461526; //kJ/(kg K) Pi = p / 16.53; tau = 1386 / T; gamma_der_pi = 0; for i = 1 : 34 gamma_der_pi = gamma_der_pi - n1(i) * I1(i) * (7.1 - Pi) ^ (I1(i) - 1) * (tau - 1.222) ^ J1(i); end v1_pT = R * T / p * Pi * gamma_der_pi / 1000; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function h1_pT = h1_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation //Eqution 7, Table 3, Page 6 I1 = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 4, 4, 4, 5, 8, 8, 21, 23, 29, 30, 31, 32]; J1 = [-2, -1, 0, 1, 2, 3, 4, 5, -9, -7, -1, 0, 1, 3, -3, 0, 1, 3, 17, -4, 0, 6, -5, -2, 10, -8, -11, -6, -29, -31, -38, -39, -40, -41]; n1 = [0.14632971213167, -0.84548187169114, -3.756360367204, 3.3855169168385, -0.95791963387872, 0.15772038513228, -0.016616417199501, 8.1214629983568E-04, 2.8319080123804E-04, -6.0706301565874E-04, -0.018990068218419, -0.032529748770505, -0.021841717175414, -5.283835796993E-05, -4.7184321073267E-04, -3.0001780793026E-04, 4.7661393906987E-05, -4.4141845330846E-06, -7.2694996297594E-16, -3.1679644845054E-05, -2.8270797985312E-06, -8.5205128120103E-10, -2.2425281908E-06, -6.5171222895601E-07, -1.4341729937924E-13, -4.0516996860117E-07, -1.2734301741641E-09, -1.7424871230634E-10, -6.8762131295531E-19, 1.4478307828521E-20, 2.6335781662795E-23, -1.1947622640071E-23, 1.8228094581404E-24, -9.3537087292458E-26]; R = 0.461526; //kJ/(kg K) Pi = p / 16.53; tau = 1386 / T; gamma_der_tau = 0; for i = 1 : 34 gamma_der_tau = gamma_der_tau + (n1(i) * (7.1 - Pi) ^ I1(i) * J1(i) * (tau - 1.222) ^ (J1(i) - 1)); end h1_pT = R * T * tau * gamma_der_tau; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function u1_pT = u1_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation //Eqution 7, Table 3, Page 6 I1 = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 4, 4, 4, 5, 8, 8, 21, 23, 29, 30, 31, 32]; J1 = [-2, -1, 0, 1, 2, 3, 4, 5, -9, -7, -1, 0, 1, 3, -3, 0, 1, 3, 17, -4, 0, 6, -5, -2, 10, -8, -11, -6, -29, -31, -38, -39, -40, -41]; n1 = [0.14632971213167, -0.84548187169114, -3.756360367204, 3.3855169168385, -0.95791963387872, 0.15772038513228, -0.016616417199501, 8.1214629983568E-04, 2.8319080123804E-04, -6.0706301565874E-04, -0.018990068218419, -0.032529748770505, -0.021841717175414, -5.283835796993E-05, -4.7184321073267E-04, -3.0001780793026E-04, 4.7661393906987E-05, -4.4141845330846E-06, -7.2694996297594E-16, -3.1679644845054E-05, -2.8270797985312E-06, -8.5205128120103E-10, -2.2425281908E-06, -6.5171222895601E-07, -1.4341729937924E-13, -4.0516996860117E-07, -1.2734301741641E-09, -1.7424871230634E-10, -6.8762131295531E-19, 1.4478307828521E-20, 2.6335781662795E-23, -1.1947622640071E-23, 1.8228094581404E-24, -9.3537087292458E-26]; R = 0.461526; //kJ/(kg K) Pi = p / 16.53; tau = 1386 / T; gamma_der_tau = 0; gamma_der_pi = 0; for i = 1 : 34 gamma_der_pi = gamma_der_pi - n1(i) * I1(i) * (7.1 - Pi) ^ (I1(i) - 1) * (tau - 1.222) ^ J1(i); gamma_der_tau = gamma_der_tau + (n1(i) * (7.1 - Pi) ^ I1(i) * J1(i) * (tau - 1.222) ^ (J1(i) - 1)); end u1_pT = R * T * (tau * gamma_der_tau - Pi * gamma_der_pi); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function s1_pT = s1_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation //Eqution 7, Table 3, Page 6 I1 = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 4, 4, 4, 5, 8, 8, 21, 23, 29, 30, 31, 32]; J1 = [-2, -1, 0, 1, 2, 3, 4, 5, -9, -7, -1, 0, 1, 3, -3, 0, 1, 3, 17, -4, 0, 6, -5, -2, 10, -8, -11, -6, -29, -31, -38, -39, -40, -41]; n1 = [0.14632971213167, -0.84548187169114, -3.756360367204, 3.3855169168385, -0.95791963387872, 0.15772038513228, -0.016616417199501, 8.1214629983568E-04, 2.8319080123804E-04, -6.0706301565874E-04, -0.018990068218419, -0.032529748770505, -0.021841717175414, -5.283835796993E-05, -4.7184321073267E-04, -3.0001780793026E-04, 4.7661393906987E-05, -4.4141845330846E-06, -7.2694996297594E-16, -3.1679644845054E-05, -2.8270797985312E-06, -8.5205128120103E-10, -2.2425281908E-06, -6.5171222895601E-07, -1.4341729937924E-13, -4.0516996860117E-07, -1.2734301741641E-09, -1.7424871230634E-10, -6.8762131295531E-19, 1.4478307828521E-20, 2.6335781662795E-23, -1.1947622640071E-23, 1.8228094581404E-24, -9.3537087292458E-26]; R = 0.461526; //kJ/(kg K) Pi = p / 16.53; tau = 1386 / T; Gamma = 0; gamma_der_tau = 0; for i = 1 : 34 gamma_der_tau = gamma_der_tau + (n1(i) * (7.1 - Pi) ^ I1(i) * J1(i) * (tau - 1.222) ^ (J1(i) - 1)); Gamma = Gamma + n1(i) * (7.1 - Pi) ^ I1(i) * (tau - 1.222) ^ J1(i); end s1_pT = R * tau * gamma_der_tau - R * Gamma; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Cp1_pT = Cp1_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation //Eqution 7, Table 3, Page 6 I1 = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 4, 4, 4, 5, 8, 8, 21, 23, 29, 30, 31, 32]; J1 = [-2, -1, 0, 1, 2, 3, 4, 5, -9, -7, -1, 0, 1, 3, -3, 0, 1, 3, 17, -4, 0, 6, -5, -2, 10, -8, -11, -6, -29, -31, -38, -39, -40, -41]; n1 = [0.14632971213167, -0.84548187169114, -3.756360367204, 3.3855169168385, -0.95791963387872, 0.15772038513228, -0.016616417199501, 8.1214629983568E-04, 2.8319080123804E-04, -6.0706301565874E-04, -0.018990068218419, -0.032529748770505, -0.021841717175414, -5.283835796993E-05, -4.7184321073267E-04, -3.0001780793026E-04, 4.7661393906987E-05, -4.4141845330846E-06, -7.2694996297594E-16, -3.1679644845054E-05, -2.8270797985312E-06, -8.5205128120103E-10, -2.2425281908E-06, -6.5171222895601E-07, -1.4341729937924E-13, -4.0516996860117E-07, -1.2734301741641E-09, -1.7424871230634E-10, -6.8762131295531E-19, 1.4478307828521E-20, 2.6335781662795E-23, -1.1947622640071E-23, 1.8228094581404E-24, -9.3537087292458E-26]; R = 0.461526; //kJ/(kg K) Pi = p / 16.53; tau = 1386 / T; gamma_der_tautau = 0; for i = 1 :34 gamma_der_tautau = gamma_der_tautau + (n1(i) * (7.1 - Pi) ^ I1(i) * J1(i) * (J1(i) - 1) * (tau - 1.222) ^ (J1(i) - 2)); end Cp1_pT = -R * tau ^ 2 * gamma_der_tautau; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Cv1_pT = Cv1_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation //Eqution 7, Table 3, Page 6 I1 = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 4, 4, 4, 5, 8, 8, 21, 23, 29, 30, 31, 32]; J1 = [-2, -1, 0, 1, 2, 3, 4, 5, -9, -7, -1, 0, 1, 3, -3, 0, 1, 3, 17, -4, 0, 6, -5, -2, 10, -8, -11, -6, -29, -31, -38, -39, -40, -41]; n1 = [0.14632971213167, -0.84548187169114, -3.756360367204, 3.3855169168385, -0.95791963387872, 0.15772038513228, -0.016616417199501, 8.1214629983568E-04, 2.8319080123804E-04, -6.0706301565874E-04, -0.018990068218419, -0.032529748770505, -0.021841717175414, -5.283835796993E-05, -4.7184321073267E-04, -3.0001780793026E-04, 4.7661393906987E-05, -4.4141845330846E-06, -7.2694996297594E-16, -3.1679644845054E-05, -2.8270797985312E-06, -8.5205128120103E-10, -2.2425281908E-06, -6.5171222895601E-07, -1.4341729937924E-13, -4.0516996860117E-07, -1.2734301741641E-09, -1.7424871230634E-10, -6.8762131295531E-19, 1.4478307828521E-20, 2.6335781662795E-23, -1.1947622640071E-23, 1.8228094581404E-24, -9.3537087292458E-26]; R = 0.461526; //kJ/(kg K) Pi = p / 16.53; tau = 1386 / T; gamma_der_pi = 0; gamma_der_pipi = 0; gamma_der_pitau = 0; gamma_der_tautau = 0; for i = 1 : 34 gamma_der_pi = gamma_der_pi - n1(i) * I1(i) * (7.1 - Pi) ^ (I1(i) - 1) * (tau - 1.222) ^ J1(i); gamma_der_pipi = gamma_der_pipi + n1(i) * I1(i) * (I1(i) - 1) * (7.1 - Pi) ^ (I1(i) - 2) * (tau - 1.222) ^ J1(i); gamma_der_pitau = gamma_der_pitau - n1(i) * I1(i) * (7.1 - Pi) ^ (I1(i) - 1) * J1(i) * (tau - 1.222) ^ (J1(i) - 1); gamma_der_tautau = gamma_der_tautau + n1(i) * (7.1 - Pi) ^ I1(i) * J1(i) * (J1(i) - 1) * (tau - 1.222) ^ (J1(i) - 2); end Cv1_pT = R * (-tau ^ 2 * gamma_der_tautau + (gamma_der_pi - tau * gamma_der_pitau) ^ 2 / gamma_der_pipi); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function w1_pT = w1_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation //Eqution 7, Table 3, Page 6 I1 = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 4, 4, 4, 5, 8, 8, 21, 23, 29, 30, 31, 32]; J1 = [-2, -1, 0, 1, 2, 3, 4, 5, -9, -7, -1, 0, 1, 3, -3, 0, 1, 3, 17, -4, 0, 6, -5, -2, 10, -8, -11, -6, -29, -31, -38, -39, -40, -41]; n1 = [0.14632971213167, -0.84548187169114, -3.756360367204, 3.3855169168385, -0.95791963387872, 0.15772038513228, -0.016616417199501, 8.1214629983568E-04, 2.8319080123804E-04, -6.0706301565874E-04, -0.018990068218419, -0.032529748770505, -0.021841717175414, -5.283835796993E-05, -4.7184321073267E-04, -3.0001780793026E-04, 4.7661393906987E-05, -4.4141845330846E-06, -7.2694996297594E-16, -3.1679644845054E-05, -2.8270797985312E-06, -8.5205128120103E-10, -2.2425281908E-06, -6.5171222895601E-07, -1.4341729937924E-13, -4.0516996860117E-07, -1.2734301741641E-09, -1.7424871230634E-10, -6.8762131295531E-19, 1.4478307828521E-20, 2.6335781662795E-23, -1.1947622640071E-23, 1.8228094581404E-24, -9.3537087292458E-26]; R = 0.461526; //kJ/(kg K) Pi = p / 16.53; tau = 1386 / T; gamma_der_pi = 0; gamma_der_pipi = 0; gamma_der_pitau = 0; gamma_der_tautau = 0; for i = 1 : 34 gamma_der_pi = gamma_der_pi - n1(i) * I1(i) * (7.1 - Pi) ^ (I1(i) - 1) * (tau - 1.222) ^ J1(i); gamma_der_pipi = gamma_der_pipi + n1(i) * I1(i) * (I1(i) - 1) * (7.1 - Pi) ^ (I1(i) - 2) * (tau - 1.222) ^ J1(i); gamma_der_pitau = gamma_der_pitau - n1(i) * I1(i) * (7.1 - Pi) ^ (I1(i) - 1) * J1(i) * (tau - 1.222) ^ (J1(i) - 1); gamma_der_tautau = gamma_der_tautau + n1(i) * (7.1 - Pi) ^ I1(i) * J1(i) * (J1(i) - 1) * (tau - 1.222) ^ (J1(i) - 2); end w1_pT = (1000 * R * T * gamma_der_pi ^ 2 / ((gamma_der_pi - tau * gamma_der_pitau) ^ 2 / (tau ^ 2 * gamma_der_tautau) - gamma_der_pipi)) ^ 0.5; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T1_ph = T1_ph(p, h) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation, 5.2.1 The Backward Equation T ( p,h ) //Eqution 11, Table 6, Page 10 I1 = [0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 1, 2, 2, 3, 3, 4, 5, 6]; J1 = [0, 1, 2, 6, 22, 32, 0, 1, 2, 3, 4, 10, 32, 10, 32, 10, 32, 32, 32, 32]; n1 = [-238.72489924521, 404.21188637945, 113.49746881718, -5.8457616048039, -1.528548241314E-04, -1.0866707695377E-06, -13.391744872602, 43.211039183559, -54.010067170506, 30.535892203916, -6.5964749423638, 9.3965400878363E-03, 1.157364750534E-07, -2.5858641282073E-05, -4.0644363084799E-09, 6.6456186191635E-08, 8.0670734103027E-11, -9.3477771213947E-13, 5.8265442020601E-15, -1.5020185953503E-17]; Pi = p / 1; eta = h / 2500; T = 0; for i = 1 : 20 T = T + n1(i) * Pi ^ I1(i) * (eta + 1) ^ J1(i); end T1_ph = T; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T1_ps = T1_ps(p, s) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //5 Equations for Region 1, Section. 5.1 Basic Equation, 5.2.2 The Backward Equation T ( p, s ) //Eqution 13, Table 8, Page 11 I1 = [0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 4]; J1 = [0, 1, 2, 3, 11, 31, 0, 1, 2, 3, 12, 31, 0, 1, 2, 9, 31, 10, 32, 32]; n1 = [174.78268058307, 34.806930892873, 6.5292584978455, 0.33039981775489, -1.9281382923196E-07, -2.4909197244573E-23, -0.26107636489332, 0.22592965981586, -0.064256463395226, 7.8876289270526E-03, 3.5672110607366E-10, 1.7332496994895E-24, 5.6608900654837E-04, -3.2635483139717E-04, 4.4778286690632E-05, -5.1322156908507E-10, -4.2522657042207E-26, 2.6400441360689E-13, 7.8124600459723E-29, -3.0732199903668E-31]; Pi = p / 1; Sigma = s / 1; T = 0; for i = 1 : 20 T = T + n1(i) * Pi ^ I1(i) * (Sigma + 2) ^ J1(i); end T1_ps = T; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function p1_hs = p1_hs(h, s) //Supplementary Release on Backward Equations for Pressure as a Function of Enthalpy and Entropy p(h,s) to the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //5 Backward Equation p(h,s) for Region 1 //Eqution 1, Table 2, Page 5 I1 = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 3, 4, 4, 5]; J1 = [0, 1, 2, 4, 5, 6, 8, 14, 0, 1, 4, 6, 0, 1, 10, 4, 1, 4, 0]; n1 = [-0.691997014660582, -18.361254878756, -9.28332409297335, 65.9639569909906, -16.2060388912024, 450.620017338667, 854.68067822417, 6075.23214001162, 32.6487682621856, -26.9408844582931, -319.9478483343, -928.35430704332, 30.3634537455249, -65.0540422444146, -4309.9131651613, -747.512324096068, 730.000345529245, 1142.84032569021, -436.407041874559]; eta = h / 3400; Sigma = s / 7.6; p = 0; for i = 1 : 19 p = p + n1(i) * (eta + 0.05) ^ I1(i) * (Sigma + 0.05) ^ J1(i); end p1_hs = p * 100; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T1_prho = T1_prho(p ,rho) //Solve by iteration. Observe that for low temperatures this equation has 2 solutions. //Solve with half interval method Low_Bound = 273.15; High_Bound = T4_p(p); rhos=-1000; while abs(rho - rhos) > 0.00001 Ts = (Low_Bound + High_Bound) / 2; rhos = 1 / v1_pT(p, Ts); if rhos < rho High_Bound = Ts; else Low_Bound = Ts; end end T1_prho = Ts; //*********************************************************************************************************** //*2.2 functions for region 2 endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function v2_pT = v2_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2, Section. 6.1 Basic Equation //Table 11 and 12, Page 14 and 15 J0 = [0, 1, -5, -4, -3, -2, -1, 2, 3]; n0 = [-9.6927686500217, 10.086655968018, -0.005608791128302, 0.071452738081455, -0.40710498223928, 1.4240819171444, -4.383951131945, -0.28408632460772, 0.021268463753307]; Ir = [1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 5, 6, 6, 6, 7, 7, 7, 8, 8, 9, 10, 10, 10, 16, 16, 18, 20, 20, 20, 21, 22, 23, 24, 24, 24]; Jr = [0, 1, 2, 3, 6, 1, 2, 4, 7, 36, 0, 1, 3, 6, 35, 1, 2, 3, 7, 3, 16, 35, 0, 11, 25, 8, 36, 13, 4, 10, 14, 29, 50, 57, 20, 35, 48, 21, 53, 39, 26, 40, 58]; nr = [-1.7731742473213E-03, -0.017834862292358, -0.045996013696365, -0.057581259083432, -0.05032527872793, -3.3032641670203E-05, -1.8948987516315E-04, .. -3.9392777243355E-03, -0.043797295650573, -2.6674547914087E-05, 2.0481737692309E-08, 4.3870667284435E-07, -3.227767723857E-05, -1.5033924542148E-03, .. -0.040668253562649, -7.8847309559367E-10, 1.2790717852285E-08, 4.8225372718507E-07, 2.2922076337661E-06, -1.6714766451061E-11, -2.1171472321355E-03, .. -23.895741934104, -5.905956432427E-18, -1.2621808899101E-06, -0.038946842435739, 1.1256211360459E-11, -8.2311340897998, 1.9809712802088E-08, .. 1.0406965210174E-19, -1.0234747095929E-13, -1.0018179379511E-09, -8.0882908646985E-11, 0.10693031879409, -0.33662250574171, 8.9185845355421E-25, .. 3.0629316876232E-13, -4.2002467698208E-06, -5.9056029685639E-26, 3.7826947613457E-06, -1.2768608934681E-15, 7.3087610595061E-29, 5.5414715350778E-17, .. -9.436970724121E-07]; R = 0.461526; //kJ/(kg K) Pi = p; tau = 540 / T; g0_pi = 1 / Pi; gr_pi = 0; for i = 1:43, gr_pi = gr_pi + nr(i) * Ir(i) * Pi ^ (Ir(i) - 1) * (tau - 0.5) ^ Jr(i); end v2_pT = R * T / p * Pi * (g0_pi + gr_pi) / 1000; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function h2_pT = h2_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2, Section. 6.1 Basic Equation //Table 11 and 12, Page 14 and 15 J0 = [0, 1, -5, -4, -3, -2, -1, 2, 3]; n0 = [-9.6927686500217, 10.086655968018, -0.005608791128302, 0.071452738081455, -0.40710498223928, 1.4240819171444, -4.383951131945, -0.28408632460772, 0.021268463753307]; Ir = [1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 5, 6, 6, 6, 7, 7, 7, 8, 8, 9, 10, 10, 10, 16, 16, 18, 20, 20, 20, 21, 22, 23, 24, 24, 24]; Jr = [0, 1, 2, 3, 6, 1, 2, 4, 7, 36, 0, 1, 3, 6, 35, 1, 2, 3, 7, 3, 16, 35, 0, 11, 25, 8, 36, 13, 4, 10, 14, 29, 50, 57, 20, 35, 48, 21, 53, 39, 26, 40, 58]; nr = [-1.7731742473213E-03, -0.017834862292358, -0.045996013696365, -0.057581259083432, -0.05032527872793, -3.3032641670203E-05, -1.8948987516315E-04, -3.9392777243355E-03, -0.043797295650573, -2.6674547914087E-05, 2.0481737692309E-08, 4.3870667284435E-07, -3.227767723857E-05, -1.5033924542148E-03, -0.040668253562649, -7.8847309559367E-10, 1.2790717852285E-08, 4.8225372718507E-07, 2.2922076337661E-06, -1.6714766451061E-11, -2.1171472321355E-03, -23.895741934104, -5.905956432427E-18, -1.2621808899101E-06, -0.038946842435739, 1.1256211360459E-11, -8.2311340897998, 1.9809712802088E-08, 1.0406965210174E-19, -1.0234747095929E-13, -1.0018179379511E-09, -8.0882908646985E-11, 0.10693031879409, -0.33662250574171, 8.9185845355421E-25, 3.0629316876232E-13, -4.2002467698208E-06, -5.9056029685639E-26, 3.7826947613457E-06, -1.2768608934681E-15, 7.3087610595061E-29, 5.5414715350778E-17, -9.436970724121E-07]; R = 0.461526; //kJ/(kg K) Pi = p; tau = 540 / T; g0_tau = 0; for i = 1 : 9 g0_tau = g0_tau + n0(i) * J0(i) * tau ^ (J0(i) - 1); end gr_tau = 0; for i = 1 : 43 gr_tau = gr_tau + nr(i) * Pi ^ Ir(i) * Jr(i) * (tau - 0.5) ^ (Jr(i) - 1); end h2_pT = R * T * tau * (g0_tau + gr_tau); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function u2_pT = u2_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2, Section. 6.1 Basic Equation //Table 11 and 12, Page 14 and 15 J0 = [0, 1, -5, -4, -3, -2, -1, 2, 3]; n0 = [-9.6927686500217, 10.086655968018, -0.005608791128302, 0.071452738081455, -0.40710498223928, 1.4240819171444, -4.383951131945, -0.28408632460772, 0.021268463753307]; Ir = [1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 5, 6, 6, 6, 7, 7, 7, 8, 8, 9, 10, 10, 10, 16, 16, 18, 20, 20, 20, 21, 22, 23, 24, 24, 24]; Jr = [0, 1, 2, 3, 6, 1, 2, 4, 7, 36, 0, 1, 3, 6, 35, 1, 2, 3, 7, 3, 16, 35, 0, 11, 25, 8, 36, 13, 4, 10, 14, 29, 50, 57, 20, 35, 48, 21, 53, 39, 26, 40, 58]; nr = [-1.7731742473213E-03, -0.017834862292358, -0.045996013696365, -0.057581259083432, -0.05032527872793, -3.3032641670203E-05, -1.8948987516315E-04, -3.9392777243355E-03, -0.043797295650573, -2.6674547914087E-05, 2.0481737692309E-08, 4.3870667284435E-07, -3.227767723857E-05, -1.5033924542148E-03, -0.040668253562649, -7.8847309559367E-10, 1.2790717852285E-08, 4.8225372718507E-07, 2.2922076337661E-06, -1.6714766451061E-11, -2.1171472321355E-03, -23.895741934104, -5.905956432427E-18, -1.2621808899101E-06, -0.038946842435739, 1.1256211360459E-11, -8.2311340897998, 1.9809712802088E-08, 1.0406965210174E-19, -1.0234747095929E-13, -1.0018179379511E-09, -8.0882908646985E-11, 0.10693031879409, -0.33662250574171, 8.9185845355421E-25, 3.0629316876232E-13, -4.2002467698208E-06, -5.9056029685639E-26, 3.7826947613457E-06, -1.2768608934681E-15, 7.3087610595061E-29, 5.5414715350778E-17, -9.436970724121E-07]; R = 0.461526; //kJ/(kg K) Pi = p; tau = 540 / T; g0_pi = 1 / Pi; g0_tau = 0; for i = 1 : 9 g0_tau = g0_tau + n0(i) * J0(i) * tau ^ (J0(i) - 1); end gr_pi = 0; gr_tau = 0; for i = 1 : 43 gr_pi = gr_pi + nr(i) * Ir(i) * Pi ^ (Ir(i) - 1) * (tau - 0.5) ^ Jr(i); gr_tau = gr_tau + nr(i) * Pi ^ Ir(i) * Jr(i) * (tau - 0.5) ^ (Jr(i) - 1); end u2_pT = R * T * (tau * (g0_tau + gr_tau) - Pi * (g0_pi + gr_pi)); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function s2_pT = s2_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2, Section. 6.1 Basic Equation //Table 11 and 12, Page 14 and 15 J0 = [0, 1, -5, -4, -3, -2, -1, 2, 3]; n0 = [-9.6927686500217, 10.086655968018, -0.005608791128302, 0.071452738081455, -0.40710498223928, 1.4240819171444, -4.383951131945, -0.28408632460772, 0.021268463753307]; Ir = [1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 5, 6, 6, 6, 7, 7, 7, 8, 8, 9, 10, 10, 10, 16, 16, 18, 20, 20, 20, 21, 22, 23, 24, 24, 24]; Jr = [0, 1, 2, 3, 6, 1, 2, 4, 7, 36, 0, 1, 3, 6, 35, 1, 2, 3, 7, 3, 16, 35, 0, 11, 25, 8, 36, 13, 4, 10, 14, 29, 50, 57, 20, 35, 48, 21, 53, 39, 26, 40, 58]; nr = [-1.7731742473213E-03, -0.017834862292358, -0.045996013696365, -0.057581259083432, -0.05032527872793, -3.3032641670203E-05, -1.8948987516315E-04, -3.9392777243355E-03, -0.043797295650573, -2.6674547914087E-05, 2.0481737692309E-08, 4.3870667284435E-07, -3.227767723857E-05, -1.5033924542148E-03, -0.040668253562649, -7.8847309559367E-10, 1.2790717852285E-08, 4.8225372718507E-07, 2.2922076337661E-06, -1.6714766451061E-11, -2.1171472321355E-03, -23.895741934104, -5.905956432427E-18, -1.2621808899101E-06, -0.038946842435739, 1.1256211360459E-11, -8.2311340897998, 1.9809712802088E-08, 1.0406965210174E-19, -1.0234747095929E-13, -1.0018179379511E-09, -8.0882908646985E-11, 0.10693031879409, -0.33662250574171, 8.9185845355421E-25, 3.0629316876232E-13, -4.2002467698208E-06, -5.9056029685639E-26, 3.7826947613457E-06, -1.2768608934681E-15, 7.3087610595061E-29, 5.5414715350778E-17, -9.436970724121E-07]; R = 0.461526; //kJ/(kg K) Pi = p; tau = 540 / T; g0 = log(Pi); g0_tau = 0; for i = 1 : 9 g0 = g0 + n0(i) * tau ^ J0(i); g0_tau = g0_tau + n0(i) * J0(i) * tau ^ (J0(i) - 1); end gr = 0; gr_tau = 0; for i = 1 : 43 gr = gr + nr(i) * Pi ^ Ir(i) * (tau - 0.5) ^ Jr(i); gr_tau = gr_tau + nr(i) * Pi ^ Ir(i) * Jr(i) * (tau - 0.5) ^ (Jr(i) - 1); end s2_pT = R * (tau * (g0_tau + gr_tau) - (g0 + gr)); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Cp2_pT = Cp2_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2, Section. 6.1 Basic Equation //Table 11 and 12, Page 14 and 15 J0 = [0, 1, -5, -4, -3, -2, -1, 2, 3]; n0 = [-9.6927686500217, 10.086655968018, -0.005608791128302, 0.071452738081455, -0.40710498223928, 1.4240819171444, -4.383951131945, -0.28408632460772, 0.021268463753307]; Ir = [1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 5, 6, 6, 6, 7, 7, 7, 8, 8, 9, 10, 10, 10, 16, 16, 18, 20, 20, 20, 21, 22, 23, 24, 24, 24]; Jr = [0, 1, 2, 3, 6, 1, 2, 4, 7, 36, 0, 1, 3, 6, 35, 1, 2, 3, 7, 3, 16, 35, 0, 11, 25, 8, 36, 13, 4, 10, 14, 29, 50, 57, 20, 35, 48, 21, 53, 39, 26, 40, 58]; nr = [-1.7731742473213E-03, -0.017834862292358, -0.045996013696365, -0.057581259083432, -0.05032527872793, -3.3032641670203E-05, -1.8948987516315E-04, -3.9392777243355E-03, -0.043797295650573, -2.6674547914087E-05, 2.0481737692309E-08, 4.3870667284435E-07, -3.227767723857E-05, -1.5033924542148E-03, -0.040668253562649, -7.8847309559367E-10, 1.2790717852285E-08, 4.8225372718507E-07, 2.2922076337661E-06, -1.6714766451061E-11, -2.1171472321355E-03, -23.895741934104, -5.905956432427E-18, -1.2621808899101E-06, -0.038946842435739, 1.1256211360459E-11, -8.2311340897998, 1.9809712802088E-08, 1.0406965210174E-19, -1.0234747095929E-13, -1.0018179379511E-09, -8.0882908646985E-11, 0.10693031879409, -0.33662250574171, 8.9185845355421E-25, 3.0629316876232E-13, -4.2002467698208E-06, -5.9056029685639E-26, 3.7826947613457E-06, -1.2768608934681E-15, 7.3087610595061E-29, 5.5414715350778E-17, -9.436970724121E-07]; R = 0.461526; //kJ/(kg K) Pi = p; tau = 540 / T; g0_tautau = 0; for i = 1 : 9 g0_tautau = g0_tautau + n0(i) * J0(i) * (J0(i) - 1) * tau ^ (J0(i) - 2); end gr_tautau = 0; for i = 1 : 43 gr_tautau = gr_tautau + nr(i) * Pi ^ Ir(i) * Jr(i) * (Jr(i) - 1) * (tau - 0.5) ^ (Jr(i) - 2); end Cp2_pT = -R * tau ^ 2 * (g0_tautau + gr_tautau); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Cv2_pT = Cv2_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2, Section. 6.1 Basic Equation //Table 11 and 12, Page 14 and 15 J0 = [0, 1, -5, -4, -3, -2, -1, 2, 3]; n0 = [-9.6927686500217, 10.086655968018, -0.005608791128302, 0.071452738081455, -0.40710498223928, 1.4240819171444, -4.383951131945, -0.28408632460772, 0.021268463753307]; Ir = [1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 5, 6, 6, 6, 7, 7, 7, 8, 8, 9, 10, 10, 10, 16, 16, 18, 20, 20, 20, 21, 22, 23, 24, 24, 24]; Jr = [0, 1, 2, 3, 6, 1, 2, 4, 7, 36, 0, 1, 3, 6, 35, 1, 2, 3, 7, 3, 16, 35, 0, 11, 25, 8, 36, 13, 4, 10, 14, 29, 50, 57, 20, 35, 48, 21, 53, 39, 26, 40, 58]; nr = [-1.7731742473213E-03, -0.017834862292358, -0.045996013696365, -0.057581259083432, -0.05032527872793, -3.3032641670203E-05, -1.8948987516315E-04, -3.9392777243355E-03, -0.043797295650573, -2.6674547914087E-05, 2.0481737692309E-08, 4.3870667284435E-07, -3.227767723857E-05, -1.5033924542148E-03, -0.040668253562649, -7.8847309559367E-10, 1.2790717852285E-08, 4.8225372718507E-07, 2.2922076337661E-06, -1.6714766451061E-11, -2.1171472321355E-03, -23.895741934104, -5.905956432427E-18, -1.2621808899101E-06, -0.038946842435739, 1.1256211360459E-11, -8.2311340897998, 1.9809712802088E-08, 1.0406965210174E-19, -1.0234747095929E-13, -1.0018179379511E-09, -8.0882908646985E-11, 0.10693031879409, -0.33662250574171, 8.9185845355421E-25, 3.0629316876232E-13, -4.2002467698208E-06, -5.9056029685639E-26, 3.7826947613457E-06, -1.2768608934681E-15, 7.3087610595061E-29, 5.5414715350778E-17, -9.436970724121E-07]; R = 0.461526; //kJ/(kg K) Pi = p; tau = 540 / T; g0_tautau = 0; for i = 1 : 9 g0_tautau = g0_tautau + n0(i) * J0(i) * (J0(i) - 1) * tau ^ (J0(i) - 2); end gr_pi = 0; gr_pitau = 0; gr_pipi = 0; gr_tautau = 0; for i = 1 : 43 gr_pi = gr_pi + nr(i) * Ir(i) * Pi ^ (Ir(i) - 1) * (tau - 0.5) ^ Jr(i); gr_pipi = gr_pipi + nr(i) * Ir(i) * (Ir(i) - 1) * Pi ^ (Ir(i) - 2) * (tau - 0.5) ^ Jr(i); gr_pitau = gr_pitau + nr(i) * Ir(i) * Pi ^ (Ir(i) - 1) * Jr(i) * (tau - 0.5) ^ (Jr(i) - 1); gr_tautau = gr_tautau + nr(i) * Pi ^ Ir(i) * Jr(i) * (Jr(i) - 1) * (tau - 0.5) ^ (Jr(i) - 2); end Cv2_pT = R * (-tau ^ 2 * (g0_tautau + gr_tautau) - (1 + Pi * gr_pi - tau * Pi * gr_pitau) ^ 2 / (1 - Pi ^ 2 * gr_pipi)); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function w2_pT = w2_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2, Section. 6.1 Basic Equation //Table 11 and 12, Page 14 and 15 J0 = [0, 1, -5, -4, -3, -2, -1, 2, 3]; n0 = [-9.6927686500217, 10.086655968018, -0.005608791128302, 0.071452738081455, -0.40710498223928, 1.4240819171444, -4.383951131945, -0.28408632460772, 0.021268463753307]; Ir = [1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 5, 6, 6, 6, 7, 7, 7, 8, 8, 9, 10, 10, 10, 16, 16, 18, 20, 20, 20, 21, 22, 23, 24, 24, 24]; Jr = [0, 1, 2, 3, 6, 1, 2, 4, 7, 36, 0, 1, 3, 6, 35, 1, 2, 3, 7, 3, 16, 35, 0, 11, 25, 8, 36, 13, 4, 10, 14, 29, 50, 57, 20, 35, 48, 21, 53, 39, 26, 40, 58]; nr = [-1.7731742473213E-03, -0.017834862292358, -0.045996013696365, -0.057581259083432, -0.05032527872793, -3.3032641670203E-05, -1.8948987516315E-04, -3.9392777243355E-03, -0.043797295650573, -2.6674547914087E-05, 2.0481737692309E-08, 4.3870667284435E-07, -3.227767723857E-05, -1.5033924542148E-03, -0.040668253562649, -7.8847309559367E-10, 1.2790717852285E-08, 4.8225372718507E-07, 2.2922076337661E-06, -1.6714766451061E-11, -2.1171472321355E-03, -23.895741934104, -5.905956432427E-18, -1.2621808899101E-06, -0.038946842435739, 1.1256211360459E-11, -8.2311340897998, 1.9809712802088E-08, 1.0406965210174E-19, -1.0234747095929E-13, -1.0018179379511E-09, -8.0882908646985E-11, 0.10693031879409, -0.33662250574171, 8.9185845355421E-25, 3.0629316876232E-13, -4.2002467698208E-06, -5.9056029685639E-26, 3.7826947613457E-06, -1.2768608934681E-15, 7.3087610595061E-29, 5.5414715350778E-17, -9.436970724121E-07]; R = 0.461526; //kJ/(kg K) Pi = p; tau = 540 / T; g0_tautau = 0; for i = 1 : 9 g0_tautau = g0_tautau + n0(i) * J0(i) * (J0(i) - 1) * tau ^ (J0(i) - 2); end gr_pi = 0; gr_pitau = 0; gr_pipi = 0; gr_tautau = 0; for i = 1 : 43 gr_pi = gr_pi + nr(i) * Ir(i) * Pi ^ (Ir(i) - 1) * (tau - 0.5) ^ Jr(i); gr_pipi = gr_pipi + nr(i) * Ir(i) * (Ir(i) - 1) * Pi ^ (Ir(i) - 2) * (tau - 0.5) ^ Jr(i); gr_pitau = gr_pitau + nr(i) * Ir(i) * Pi ^ (Ir(i) - 1) * Jr(i) * (tau - 0.5) ^ (Jr(i) - 1); gr_tautau = gr_tautau + nr(i) * Pi ^ Ir(i) * Jr(i) * (Jr(i) - 1) * (tau - 0.5) ^ (Jr(i) - 2); end w2_pT = (1000 * R * T * (1 + 2 * Pi * gr_pi + Pi ^ 2 * gr_pi ^ 2) / ((1 - Pi ^ 2 * gr_pipi) + (1 + Pi * gr_pi - tau * Pi * gr_pitau) ^ 2 / (tau ^ 2 * (g0_tautau + gr_tautau)))) ^ 0.5; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T2_ph = T2_ph(p, h) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2,6.3.1 The Backward Equations T( p, h ) for Subregions 2a, 2b, and 2c if p < 4 sub_reg = 1; else if p < (905.84278514723 - 0.67955786399241 * h + 1.2809002730136E-04 * h ^ 2) sub_reg = 2; else sub_reg = 3; end end select sub_reg case 1 //Subregion A //Table 20, Eq 22, page 22 Ji = [0, 1, 2, 3, 7, 20, 0, 1, 2, 3, 7, 9, 11, 18, 44, 0, 2, 7, 36, 38, 40, 42, 44, 24, 44, 12, 32, 44, 32, 36, 42, 34, 44, 28]; Ii = [0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 2, 2, 2, 3, 3, 4, 4, 4, 5, 5, 5, 6, 6, 7]; ni = [1089.8952318288, 849.51654495535, -107.81748091826, 33.153654801263, -7.4232016790248, 11.765048724356, 1.844574935579, -4.1792700549624, 6.2478196935812, -17.344563108114, -200.58176862096, 271.96065473796, -455.11318285818, 3091.9688604755, 252266.40357872, -6.1707422868339E-03, -0.31078046629583, 11.670873077107, 128127984.04046, -985549096.23276, 2822454697.3002, -3594897141.0703, 1722734991.3197, -13551.334240775, 12848734.66465, 1.3865724283226, 235988.32556514, -13105236.545054, 7399.9835474766, -551966.9703006, 3715408.5996233, 19127.72923966, -415351.64835634, -62.459855192507]; Ts = 0; hs = h / 2000; for i = 1 : 34 Ts = Ts + ni(i) * p ^ (Ii(i)) * (hs - 2.1) ^ Ji(i); end T2_ph = Ts; case 2 //Subregion B //Table 21, Eq 23, page 23 Ji = [0, 1, 2, 12, 18, 24, 28, 40, 0, 2, 6, 12, 18, 24, 28, 40, 2, 8, 18, 40, 1, 2, 12, 24, 2, 12, 18, 24, 28, 40, 18, 24, 40, 28, 2, 28, 1, 40]; Ii = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 1, 1, 2, 2, 2, 2, 3, 3, 3, 3, 4, 4, 4, 4, 4, 4, 5, 5, 5, 6, 7, 7, 9, 9]; ni = [1489.5041079516, 743.07798314034, -97.708318797837, 2.4742464705674, -0.63281320016026, 1.1385952129658, -0.47811863648625, 8.5208123431544E-03, 0.93747147377932, 3.3593118604916, 3.3809355601454, 0.16844539671904, 0.73875745236695, -0.47128737436186, 0.15020273139707, -0.002176411421975, -0.021810755324761, -0.10829784403677, -0.046333324635812, 7.1280351959551E-05, 1.1032831789999E-04, 1.8955248387902E-04, 3.0891541160537E-03, 1.3555504554949E-03, 2.8640237477456E-07, -1.0779857357512E-05, -7.6462712454814E-05, 1.4052392818316E-05, -3.1083814331434E-05, -1.0302738212103E-06, 2.821728163504E-07, 1.2704902271945E-06, 7.3803353468292E-08, -1.1030139238909E-08, -8.1456365207833E-14, -2.5180545682962E-11, -1.7565233969407E-18, 8.6934156344163E-15]; Ts = 0; hs = h / 2000; for i = 1 : 38 Ts = Ts + ni(i) * (p - 2) ^ (Ii(i)) * (hs - 2.6) ^ Ji(i); end T2_ph = Ts; else //Subregion C //Table 22, Eq 24, page 24 Ji = [0, 4, 0, 2, 0, 2, 0, 1, 0, 2, 0, 1, 4, 8, 4, 0, 1, 4, 10, 12, 16, 20, 22]; Ii = [-7, -7, -6, -6, -5, -5, -2, -2, -1, -1, 0, 0, 1, 1, 2, 6, 6, 6, 6, 6, 6, 6, 6]; ni = [-3236839855524.2, 7326335090218.1, 358250899454.47, -583401318515.9, -10783068217.47, 20825544563.171, 610747.83564516, 859777.2253558, -25745.72360417, 31081.088422714, 1208.2315865936, 482.19755109255, 3.7966001272486, -10.842984880077, -0.04536417267666, 1.4559115658698E-13, 1.126159740723E-12, -1.7804982240686E-11, 1.2324579690832E-07, -1.1606921130984E-06, 2.7846367088554E-05, -5.9270038474176E-04, 1.2918582991878E-03]; Ts = 0; hs = h / 2000; for i = 1 : 23 Ts = Ts + ni(i) * (p + 25) ^ (Ii(i)) * (hs - 1.8) ^ Ji(i); end T2_ph = Ts; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T2_ps = T2_ps(p, s) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //6 Equations for Region 2,6.3.2 The Backward Equations T( p, s ) for Subregions 2a, 2b, and 2c //Page 26 if p < 4 sub_reg = 1; else if s < 5.85 sub_reg = 3; else sub_reg = 2; end end select sub_reg case 1 //Subregion A //Table 25, Eq 25, page 26 Ii = [-1.5, -1.5, -1.5, -1.5, -1.5, -1.5, -1.25, -1.25, -1.25, -1, -1, -1, -1, -1, -1, -0.75, -0.75, -0.5, -0.5, -0.5, -0.5, -0.25, -0.25, -0.25, -0.25, 0.25, 0.25, 0.25, 0.25, 0.5, 0.5, 0.5, 0.5, 0.5, 0.5, 0.5, 0.75, 0.75, 0.75, 0.75, 1, 1, 1.25, 1.25, 1.5, 1.5]; Ji = [-24, -23, -19, -13, -11, -10, -19, -15, -6, -26, -21, -17, -16, -9, -8, -15, -14, -26, -13, -9, -7, -27, -25, -11, -6, 1, 4, 8, 11, 0, 1, 5, 6, 10, 14, 16, 0, 4, 9, 17, 7, 18, 3, 15, 5, 18]; ni = [-392359.83861984, 515265.7382727, 40482.443161048, -321.93790923902, 96.961424218694, -22.867846371773, -449429.14124357, -5011.8336020166, 0.35684463560015, 44235.33584819, -13673.388811708, 421632.60207864, 22516.925837475, 474.42144865646, -149.31130797647, -197811.26320452, -23554.39947076, -19070.616302076, 55375.669883164, 3829.3691437363, -603.91860580567, 1936.3102620331, 4266.064369861, -5978.0638872718, -704.01463926862, 338.36784107553, 20.862786635187, 0.033834172656196, -4.3124428414893E-05, 166.53791356412, -139.86292055898, -0.78849547999872, 0.072132411753872, -5.9754839398283E-03, -1.2141358953904E-05, 2.3227096733871E-07, -10.538463566194, 2.0718925496502, -0.072193155260427, 2.074988708112E-07, -0.018340657911379, 2.9036272348696E-07, 0.21037527893619, 2.5681239729999E-04, -0.012799002933781, -8.2198102652018E-06]; Pi = p; Sigma = s / 2; teta = 0; for i = 1 : 46 teta = teta + ni(i) * Pi ^ Ii(i) * (Sigma - 2) ^ Ji(i); end T2_ps = teta; case 2 //Subregion B //Table 26, Eq 26, page 27 Ii = [-6, -6, -5, -5, -4, -4, -4, -3, -3, -3, -3, -2, -2, -2, -2, -1, -1, -1, -1, -1, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 3, 3, 3, 4, 4, 5, 5, 5]; Ji = [0, 11, 0, 11, 0, 1, 11, 0, 1, 11, 12, 0, 1, 6, 10, 0, 1, 5, 8, 9, 0, 1, 2, 4, 5, 6, 9, 0, 1, 2, 3, 7, 8, 0, 1, 5, 0, 1, 3, 0, 1, 0, 1, 2]; ni = [316876.65083497, 20.864175881858, -398593.99803599, -21.816058518877, 223697.85194242, -2784.1703445817, 9.920743607148, -75197.512299157, 2970.8605951158, -3.4406878548526, 0.38815564249115, 17511.29508575, -1423.7112854449, 1.0943803364167, 0.89971619308495, -3375.9740098958, 471.62885818355, -1.9188241993679, 0.41078580492196, -0.33465378172097, 1387.0034777505, -406.63326195838, 41.72734715961, 2.1932549434532, -1.0320050009077, 0.35882943516703, 5.2511453726066E-03, 12.838916450705, -2.8642437219381, 0.56912683664855, -0.099962954584931, -3.2632037778459E-03, 2.3320922576723E-04, -0.1533480985745, 0.029072288239902, 3.7534702741167E-04, 1.7296691702411E-03, -3.8556050844504E-04, -3.5017712292608E-05, -1.4566393631492E-05, 5.6420857267269E-06, 4.1286150074605E-08, -2.0684671118824E-08, 1.6409393674725E-09]; Pi = p; Sigma = s / 0.7853; teta = 0; for i = 1 : 44 teta = teta + ni(i) * Pi ^ Ii(i) * (10 - Sigma) ^ Ji(i); end T2_ps = teta; else //Subregion C //Table 27, Eq 27, page 28 Ii = [-2, -2, -1, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 3, 3, 3, 4, 4, 4, 5, 5, 5, 6, 6, 7, 7, 7, 7, 7]; Ji = [0, 1, 0, 0, 1, 2, 3, 0, 1, 3, 4, 0, 1, 2, 0, 1, 5, 0, 1, 4, 0, 1, 2, 0, 1, 0, 1, 3, 4, 5]; ni = [909.68501005365, 2404.566708842, -591.6232638713, 541.45404128074, -270.98308411192, 979.76525097926, -469.66772959435, 14.399274604723, -19.104204230429, 5.3299167111971, -21.252975375934, -0.3114733441376, 0.60334840894623, -0.042764839702509, 5.8185597255259E-03, -0.014597008284753, 5.6631175631027E-03, -7.6155864584577E-05, 2.2440342919332E-04, -1.2561095013413E-05, 6.3323132660934E-07, -2.0541989675375E-06, 3.6405370390082E-08, -2.9759897789215E-09, 1.0136618529763E-08, 5.9925719692351E-12, -2.0677870105164E-11, -2.0874278181886E-11, 1.0162166825089E-10, -1.6429828281347E-10]; Pi = p; Sigma = s / 2.9251; teta = 0; for i = 1 : 30 teta = teta + ni(i) * Pi ^ Ii(i) * (2 - Sigma) ^ Ji(i); end T2_ps = teta; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function p2_hs = p2_hs(h, s) //Supplementary Release on Backward Equations for Pressure as a function of Enthalpy and Entropy p(h,s) to the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //Chapter 6:Backward Equations p(h,s) for Region 2 if h < (-3498.98083432139 + 2575.60716905876 * s - 421.073558227969 * s ^ 2 + 27.6349063799944 * s ^ 3) sub_reg = 1; else if s < 5.85 sub_reg = 3; else sub_reg = 2; end end select sub_reg case 1 //Subregion A //Table 6, Eq 3, page 8 Ii = [0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 2, 2, 2, 3, 3, 3, 3, 3, 4, 5, 5, 6, 7]; Ji = [1, 3, 6, 16, 20, 22, 0, 1, 2, 3, 5, 6, 10, 16, 20, 22, 3, 16, 20, 0, 2, 3, 6, 16, 16, 3, 16, 3, 1]; ni = [-1.82575361923032E-02, -0.125229548799536, 0.592290437320145, 6.04769706185122, 238.624965444474, -298.639090222922, 0.051225081304075, -0.437266515606486, 0.413336902999504, -5.16468254574773, -5.57014838445711, 12.8555037824478, 11.414410895329, -119.504225652714, -2847.7798596156, 4317.57846408006, 1.1289404080265, 1974.09186206319, 1516.12444706087, 1.41324451421235E-02, 0.585501282219601, -2.97258075863012, 5.94567314847319, -6236.56565798905, 9659.86235133332, 6.81500934948134, -6332.07286824489, -5.5891922446576, 4.00645798472063E-02]; eta = h / 4200; Sigma = s / 12; Pi = 0; for i = 1 : 29 Pi = Pi + ni(i) * (eta - 0.5) ^ Ii(i) * (Sigma - 1.2) ^ Ji(i); end p2_hs = Pi ^ 4 * 4; case 2 //Subregion B //Table 7, Eq 4, page 9 Ii = [0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 1, 2, 2, 2, 3, 3, 3, 3, 4, 4, 5, 5, 6, 6, 6, 7, 7, 8, 8, 8, 8, 12, 14]; Ji = [0, 1, 2, 4, 8, 0, 1, 2, 3, 5, 12, 1, 6, 18, 0, 1, 7, 12, 1, 16, 1, 12, 1, 8, 18, 1, 16, 1, 3, 14, 18, 10, 16]; ni = [8.01496989929495E-02, -0.543862807146111, 0.337455597421283, 8.9055545115745, 313.840736431485, 0.797367065977789, -1.2161697355624, 8.72803386937477, -16.9769781757602, -186.552827328416, 95115.9274344237, -18.9168510120494, -4334.0703719484, 543212633.012715, 0.144793408386013, 128.024559637516, -67230.9534071268, 33697238.0095287, -586.63419676272, -22140322476.9889, 1716.06668708389, -570817595.806302, -3121.09693178482, -2078413.8463301, 3056059461577.86, 3221.57004314333, 326810259797.295, -1441.04158934487, 410.694867802691, 109077066873.024, -24796465425889.3, 1888019068.65134, -123651009018773]; eta = h / 4100; Sigma = s / 7.9; Pi = 0; for i = 1 : 33 Pi = Pi + ni(i) * (eta - 0.6) ^ Ii(i) * (Sigma - 1.01) ^ Ji(i); end p2_hs = Pi ^ 4 * 100; else //Subregion C //Table 8, Eq 5, page 10 Ii = [0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 1, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 5, 5, 5, 5, 6, 6, 10, 12, 16]; Ji = [0, 1, 2, 3, 4, 8, 0, 2, 5, 8, 14, 2, 3, 7, 10, 18, 0, 5, 8, 16, 18, 18, 1, 4, 6, 14, 8, 18, 7, 7, 10]; ni = [0.112225607199012, -3.39005953606712, -32.0503911730094, -197.5973051049, -407.693861553446, 13294.3775222331, 1.70846839774007, 37.3694198142245, 3581.44365815434, 423014.446424664, -751071025.760063, 52.3446127607898, -228.351290812417, -960652.417056937, -80705929.2526074, 1626980172256.69, 0.772465073604171, 46392.9973837746, -13731788.5134128, 1704703926305.12, -25110462818730.8, 31774883083552, 53.8685623675312, -55308.9094625169, -1028615.22421405, 2042494187562.34, 273918446.626977, -2.63963146312685E+15, -1078908541.08088, -29649262098.0124, -1.11754907323424E+15]; eta = h / 3500; Sigma = s / 5.9; Pi = 0; for i = 1 : 31 Pi = Pi + ni(i) * (eta - 0.7) ^ Ii(i) * (Sigma - 1.1) ^ Ji(i); end p2_hs = Pi ^ 4 * 100; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T2_prho=T2_prho(p,rho) //Solve by iteration. Observe that fo low temperatures this equation has 2 solutions. //Solve with half interval method if p < 16.5292 Low_Bound = T4_p(p); else Low_Bound = B23T_p(p); end High_Bound = 1073.15; rhos=-1000; while abs(rho - rhos) > 0.000001 Ts = (Low_Bound + High_Bound) / 2; rhos = 1 / v2_pT(p, Ts); if rhos < rho High_Bound = Ts; else Low_Bound = Ts; end end T2_prho = Ts; //*********************************************************************************************************** //*2.3 functions for region 3 endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function p3_rhoT = p3_rhoT(rho, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //7 Basic Equation for Region 3, Section. 6.1 Basic Equation //Table 30 and 31, Page 30 and 31 Ii = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 4, 5, 5, 5, 6, 6, 6, 7, 8, 9, 9, 10, 10, 11]; Ji = [0, 0, 1, 2, 7, 10, 12, 23, 2, 6, 15, 17, 0, 2, 6, 7, 22, 26, 0, 2, 4, 16, 26, 0, 2, 4, 26, 1, 3, 26, 0, 2, 26, 2, 26, 2, 26, 0, 1, 26]; ni = [1.0658070028513, -15.732845290239, 20.944396974307, -7.6867707878716, 2.6185947787954, -2.808078114862, 1.2053369696517, -8.4566812812502E-03, -1.2654315477714, -1.1524407806681, 0.88521043984318, -0.64207765181607, 0.38493460186671, -0.85214708824206, 4.8972281541877, -3.0502617256965, 0.039420536879154, 0.12558408424308, -0.2799932969871, 1.389979956946, -2.018991502357, -8.2147637173963E-03, -0.47596035734923, 0.0439840744735, -0.44476435428739, 0.90572070719733, 0.70522450087967, 0.10770512626332, -0.32913623258954, -0.50871062041158, -0.022175400873096, 0.094260751665092, 0.16436278447961, -0.013503372241348, -0.014834345352472, 5.7922953628084E-04, 3.2308904703711E-03, 8.0964802996215E-05, -1.6557679795037E-04, -4.4923899061815E-05]; R = 0.461526; //kJ/(KgK) tc = 647.096; //K pc = 22.064; //MPa rhoc = 322; //kg/m3 delta = rho / rhoc; tau = tc / T; fidelta = 0; for i = 2 : 40 fidelta = fidelta + ni(i) * Ii(i) * delta ^ (Ii(i) - 1) * tau ^ Ji(i); end fidelta = fidelta + ni(1) / delta; p3_rhoT = rho * R * T * delta * fidelta / 1000; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function u3_rhoT = u3_rhoT(rho, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //7 Basic Equation for Region 3, Section. 6.1 Basic Equation //Table 30 and 31, Page 30 and 31 Ii = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 4, 5, 5, 5, 6, 6, 6, 7, 8, 9, 9, 10, 10, 11]; Ji = [0, 0, 1, 2, 7, 10, 12, 23, 2, 6, 15, 17, 0, 2, 6, 7, 22, 26, 0, 2, 4, 16, 26, 0, 2, 4, 26, 1, 3, 26, 0, 2, 26, 2, 26, 2, 26, 0, 1, 26]; ni = [1.0658070028513, -15.732845290239, 20.944396974307, -7.6867707878716, 2.6185947787954, -2.808078114862, 1.2053369696517, -8.4566812812502E-03, -1.2654315477714, -1.1524407806681, 0.88521043984318, -0.64207765181607, 0.38493460186671, -0.85214708824206, 4.8972281541877, -3.0502617256965, 0.039420536879154, 0.12558408424308, -0.2799932969871, 1.389979956946, -2.018991502357, -8.2147637173963E-03, -0.47596035734923, 0.0439840744735, -0.44476435428739, 0.90572070719733, 0.70522450087967, 0.10770512626332, -0.32913623258954, -0.50871062041158, -0.022175400873096, 0.094260751665092, 0.16436278447961, -0.013503372241348, -0.014834345352472, 5.7922953628084E-04, 3.2308904703711E-03, 8.0964802996215E-05, -1.6557679795037E-04, -4.4923899061815E-05]; R = 0.461526; //kJ/(KgK) tc = 647.096; //K pc = 22.064; //MPa rhoc = 322; //kg/m3 delta = rho / rhoc; tau = tc / T; fitau = 0; for i = 2 : 40 fitau = fitau + ni(i) * delta ^ Ii(i) * Ji(i) * tau ^ (Ji(i) - 1); end u3_rhoT = R * T * (tau * fitau); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function h3_rhoT = h3_rhoT(rho, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //7 Basic Equation for Region 3, Section. 6.1 Basic Equation //Table 30 and 31, Page 30 and 31 Ii = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 4, 5, 5, 5, 6, 6, 6, 7, 8, 9, 9, 10, 10, 11]; Ji = [0, 0, 1, 2, 7, 10, 12, 23, 2, 6, 15, 17, 0, 2, 6, 7, 22, 26, 0, 2, 4, 16, 26, 0, 2, 4, 26, 1, 3, 26, 0, 2, 26, 2, 26, 2, 26, 0, 1, 26]; ni = [1.0658070028513, -15.732845290239, 20.944396974307, -7.6867707878716, 2.6185947787954, -2.808078114862, 1.2053369696517, -8.4566812812502E-03, -1.2654315477714, -1.1524407806681, 0.88521043984318, -0.64207765181607, 0.38493460186671, -0.85214708824206, 4.8972281541877, -3.0502617256965, 0.039420536879154, 0.12558408424308, -0.2799932969871, 1.389979956946, -2.018991502357, -8.2147637173963E-03, -0.47596035734923, 0.0439840744735, -0.44476435428739, 0.90572070719733, 0.70522450087967, 0.10770512626332, -0.32913623258954, -0.50871062041158, -0.022175400873096, 0.094260751665092, 0.16436278447961, -0.013503372241348, -0.014834345352472, 5.7922953628084E-04, 3.2308904703711E-03, 8.0964802996215E-05, -1.6557679795037E-04, -4.4923899061815E-05]; R = 0.461526; //kJ/(KgK) tc = 647.096; //K pc = 22.064; //MPa rhoc = 322; //kg/m3 delta = rho / rhoc; tau = tc / T; fidelta = 0; fitau = 0; for i = 2 : 40 fidelta = fidelta + ni(i) * Ii(i) * delta ^ (Ii(i) - 1) * tau ^ Ji(i); fitau = fitau + ni(i) * delta ^ Ii(i) * Ji(i) * tau ^ (Ji(i) - 1); end fidelta = fidelta + ni(1) / delta; h3_rhoT = R * T * (tau * fitau + delta * fidelta); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function s3_rhoT = s3_rhoT(rho, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //7 Basic Equation for Region 3, Section. 6.1 Basic Equation //Table 30 and 31, Page 30 and 31 Ii = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 4, 5, 5, 5, 6, 6, 6, 7, 8, 9, 9, 10, 10, 11]; Ji = [0, 0, 1, 2, 7, 10, 12, 23, 2, 6, 15, 17, 0, 2, 6, 7, 22, 26, 0, 2, 4, 16, 26, 0, 2, 4, 26, 1, 3, 26, 0, 2, 26, 2, 26, 2, 26, 0, 1, 26]; ni = [1.0658070028513, -15.732845290239, 20.944396974307, -7.6867707878716, 2.6185947787954, -2.808078114862, 1.2053369696517, -8.4566812812502E-03, -1.2654315477714, -1.1524407806681, 0.88521043984318, -0.64207765181607, 0.38493460186671, -0.85214708824206, 4.8972281541877, -3.0502617256965, 0.039420536879154, 0.12558408424308, -0.2799932969871, 1.389979956946, -2.018991502357, -8.2147637173963E-03, -0.47596035734923, 0.0439840744735, -0.44476435428739, 0.90572070719733, 0.70522450087967, 0.10770512626332, -0.32913623258954, -0.50871062041158, -0.022175400873096, 0.094260751665092, 0.16436278447961, -0.013503372241348, -0.014834345352472, 5.7922953628084E-04, 3.2308904703711E-03, 8.0964802996215E-05, -1.6557679795037E-04, -4.4923899061815E-05]; R = 0.461526; //kJ/(KgK) tc = 647.096; //K pc = 22.064; //MPa rhoc = 322; //kg/m3 delta = rho / rhoc; tau = tc / T; fi = 0; fitau = 0; for i = 2 : 40 fi = fi + ni(i) * delta ^ Ii(i) * tau ^ Ji(i); fitau = fitau + ni(i) * delta ^ Ii(i) * Ji(i) * tau ^ (Ji(i) - 1); end fi = fi + ni(1) * log(delta); s3_rhoT = R * (tau * fitau - fi); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Cp3_rhoT = Cp3_rhoT(rho, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //7 Basic Equation for Region 3, Section. 6.1 Basic Equation //Table 30 and 31, Page 30 and 31 Ii = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 4, 5, 5, 5, 6, 6, 6, 7, 8, 9, 9, 10, 10, 11]; Ji = [0, 0, 1, 2, 7, 10, 12, 23, 2, 6, 15, 17, 0, 2, 6, 7, 22, 26, 0, 2, 4, 16, 26, 0, 2, 4, 26, 1, 3, 26, 0, 2, 26, 2, 26, 2, 26, 0, 1, 26]; ni = [1.0658070028513, -15.732845290239, 20.944396974307, -7.6867707878716, 2.6185947787954, -2.808078114862, 1.2053369696517, -8.4566812812502E-03, -1.2654315477714, -1.1524407806681, 0.88521043984318, -0.64207765181607, 0.38493460186671, -0.85214708824206, 4.8972281541877, -3.0502617256965, 0.039420536879154, 0.12558408424308, -0.2799932969871, 1.389979956946, -2.018991502357, -8.2147637173963E-03, -0.47596035734923, 0.0439840744735, -0.44476435428739, 0.90572070719733, 0.70522450087967, 0.10770512626332, -0.32913623258954, -0.50871062041158, -0.022175400873096, 0.094260751665092, 0.16436278447961, -0.013503372241348, -0.014834345352472, 5.7922953628084E-04, 3.2308904703711E-03, 8.0964802996215E-05, -1.6557679795037E-04, -4.4923899061815E-05]; R = 0.461526; //kJ/(KgK) tc = 647.096; //K pc = 22.064; //MPa rhoc = 322; //kg/m3 delta = rho / rhoc; tau = tc / T; fitautau = 0; fidelta = 0; fideltatau = 0; fideltadelta = 0; for i = 2 : 40 fitautau = fitautau + ni(i) * delta ^ Ii(i) * Ji(i) * (Ji(i) - 1) * tau ^ (Ji(i) - 2); fidelta = fidelta + ni(i) * Ii(i) * delta ^ (Ii(i) - 1) * tau ^ Ji(i); fideltatau = fideltatau + ni(i) * Ii(i) * delta ^ (Ii(i) - 1) * Ji(i) * tau ^ (Ji(i) - 1); fideltadelta = fideltadelta + ni(i) * Ii(i) * (Ii(i) - 1) * delta ^ (Ii(i) - 2) * tau ^ Ji(i); end fidelta = fidelta + ni(1) / delta; fideltadelta = fideltadelta - ni(1) / (delta ^ 2); Cp3_rhoT = R * (-tau ^ 2 * fitautau + (delta * fidelta - delta * tau * fideltatau) ^ 2 / (2 * delta * fidelta + delta ^ 2 * fideltadelta)); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Cv3_rhoT = Cv3_rhoT(rho, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //7 Basic Equation for Region 3, Section. 6.1 Basic Equation //Table 30 and 31, Page 30 and 31 Ii = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 4, 5, 5, 5, 6, 6, 6, 7, 8, 9, 9, 10, 10, 11]; Ji = [0, 0, 1, 2, 7, 10, 12, 23, 2, 6, 15, 17, 0, 2, 6, 7, 22, 26, 0, 2, 4, 16, 26, 0, 2, 4, 26, 1, 3, 26, 0, 2, 26, 2, 26, 2, 26, 0, 1, 26]; ni = [1.0658070028513, -15.732845290239, 20.944396974307, -7.6867707878716, 2.6185947787954, -2.808078114862, 1.2053369696517, -8.4566812812502E-03, -1.2654315477714, -1.1524407806681, 0.88521043984318, -0.64207765181607, 0.38493460186671, -0.85214708824206, 4.8972281541877, -3.0502617256965, 0.039420536879154, 0.12558408424308, -0.2799932969871, 1.389979956946, -2.018991502357, -8.2147637173963E-03, -0.47596035734923, 0.0439840744735, -0.44476435428739, 0.90572070719733, 0.70522450087967, 0.10770512626332, -0.32913623258954, -0.50871062041158, -0.022175400873096, 0.094260751665092, 0.16436278447961, -0.013503372241348, -0.014834345352472, 5.7922953628084E-04, 3.2308904703711E-03, 8.0964802996215E-05, -1.6557679795037E-04, -4.4923899061815E-05]; R = 0.461526; //kJ/(KgK) tc = 647.096; //K pc = 22.064; //MPa rhoc = 322; //kg/m3 delta = rho / rhoc; tau = tc / T; fitautau = 0; for i = 1 : 40 fitautau = fitautau + ni(i) * delta ^ Ii(i) * Ji(i) * (Ji(i) - 1) * tau ^ (Ji(i) - 2); end Cv3_rhoT = R * (-(tau * tau * fitautau)); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function w3_rhoT = w3_rhoT(rho, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //7 Basic Equation for Region 3, Section. 6.1 Basic Equation //Table 30 and 31, Page 30 and 31 Ii = [0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 2, 2, 2, 3, 3, 3, 3, 3, 4, 4, 4, 4, 5, 5, 5, 6, 6, 6, 7, 8, 9, 9, 10, 10, 11]; Ji = [0, 0, 1, 2, 7, 10, 12, 23, 2, 6, 15, 17, 0, 2, 6, 7, 22, 26, 0, 2, 4, 16, 26, 0, 2, 4, 26, 1, 3, 26, 0, 2, 26, 2, 26, 2, 26, 0, 1, 26]; ni = [1.0658070028513, -15.732845290239, 20.944396974307, -7.6867707878716, 2.6185947787954, -2.808078114862, 1.2053369696517, -8.4566812812502E-03, -1.2654315477714, -1.1524407806681, 0.88521043984318, -0.64207765181607, 0.38493460186671, -0.85214708824206, 4.8972281541877, -3.0502617256965, 0.039420536879154, 0.12558408424308, -0.2799932969871, 1.389979956946, -2.018991502357, -8.2147637173963E-03, -0.47596035734923, 0.0439840744735, -0.44476435428739, 0.90572070719733, 0.70522450087967, 0.10770512626332, -0.32913623258954, -0.50871062041158, -0.022175400873096, 0.094260751665092, 0.16436278447961, -0.013503372241348, -0.014834345352472, 5.7922953628084E-04, 3.2308904703711E-03, 8.0964802996215E-05, -1.6557679795037E-04, -4.4923899061815E-05]; R = 0.461526; //kJ/(KgK) tc = 647.096; //K pc = 22.064; //MPa rhoc = 322; //kg/m3 delta = rho / rhoc; tau = tc / T; fitautau = 0; fidelta = 0; fideltatau = 0; fideltadelta = 0; for i = 2 : 40 fitautau = fitautau + ni(i) * delta ^ Ii(i) * Ji(i) * (Ji(i) - 1) * tau ^ (Ji(i) - 2); fidelta = fidelta + ni(i) * Ii(i) * delta ^ (Ii(i) - 1) * tau ^ Ji(i); fideltatau = fideltatau + ni(i) * Ii(i) * delta ^ (Ii(i) - 1) * Ji(i) * tau ^ (Ji(i) - 1); fideltadelta = fideltadelta + ni(i) * Ii(i) * (Ii(i) - 1) * delta ^ (Ii(i) - 2) * tau ^ Ji(i); end fidelta = fidelta + ni(1) / delta; fideltadelta = fideltadelta - ni(1) / (delta ^ 2); w3_rhoT = (1000 * R * T * (2 * delta * fidelta + delta ^ 2 * fideltadelta - (delta * fidelta - delta * tau * fideltatau) ^ 2 / (tau ^ 2 * fitautau))) ^ 0.5; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T3_ph = T3_ph(p, h) //Revised Supplementary Release on Backward Equations for the functions T(p,h), v(p,h) and T(p,s), v(p,s) for Region 3 of the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //2004 //Section 3.3 Backward Equations T(p,h) and v(p,h) for Subregions 3a and 3b //Boundary equation, Eq 1 Page 5 h3ab = 2014.64004206875 + 3.74696550136983 * p - 2.19921901054187E-02 * p ^ 2 + 8.7513168600995E-05 * p ^ 3; if h < h3ab //Subregion 3a //Eq 2, Table 3, Page 7 Ii = [-12, -12, -12, -12, -12, -12, -12, -12, -10, -10, -10, -8, -8, -8, -8, -5, -3, -2, -2, -2, -1, -1, 0, 0, 1, 3, 3, 4, 4, 10, 12]; Ji = [0, 1, 2, 6, 14, 16, 20, 22, 1, 5, 12, 0, 2, 4, 10, 2, 0, 1, 3, 4, 0, 2, 0, 1, 1, 0, 1, 0, 3, 4, 5]; ni = [-1.33645667811215E-07, 4.55912656802978E-06, -1.46294640700979E-05, 6.3934131297008E-03, 372.783927268847, -7186.54377460447, 573494.7521034, -2675693.29111439, -3.34066283302614E-05, -2.45479214069597E-02, 47.8087847764996, 7.64664131818904E-06, 1.28350627676972E-03, 1.71219081377331E-02, -8.51007304583213, -1.36513461629781E-02, -3.84460997596657E-06, 3.37423807911655E-03, -0.551624873066791, 0.72920227710747, -9.92522757376041E-03, -0.119308831407288, 0.793929190615421, 0.454270731799386, 0.20999859125991, -6.42109823904738E-03, -0.023515586860454, 2.52233108341612E-03, -7.64885133368119E-03, 1.36176427574291E-02, -1.33027883575669E-02]; ps = p / 100; hs = h / 2300; Ts = 0; for i = 1 : 31 Ts = Ts + ni(i) * (ps + 0.24) ^ Ii(i) * (hs - 0.615) ^ Ji(i); end T3_ph = Ts * 760; else //Subregion 3b //Eq 3, Table 4, Page 7,8 Ii = [-12, -12, -10, -10, -10, -10, -10, -8, -8, -8, -8, -8, -6, -6, -6, -4, -4, -3, -2, -2, -1, -1, -1, -1, -1, -1, 0, 0, 1, 3, 5, 6, 8]; Ji = [0, 1, 0, 1, 5, 10, 12, 0, 1, 2, 4, 10, 0, 1, 2, 0, 1, 5, 0, 4, 2, 4, 6, 10, 14, 16, 0, 2, 1, 1, 1, 1, 1]; ni = [3.2325457364492E-05, -1.27575556587181E-04, -4.75851877356068E-04, 1.56183014181602E-03, 0.105724860113781, -85.8514221132534, 724.140095480911, 2.96475810273257E-03, -5.92721983365988E-03, -1.26305422818666E-02, -0.115716196364853, 84.9000969739595, -1.08602260086615E-02, 1.54304475328851E-02, 7.50455441524466E-02, 2.52520973612982E-02, -6.02507901232996E-02, -3.07622221350501, -5.74011959864879E-02, 5.03471360939849, -0.925081888584834, 3.91733882917546, -77.314600713019, 9493.08762098587, -1410437.19679409, 8491662.30819026, 0.861095729446704, 0.32334644281172, 0.873281936020439, -0.436653048526683, 0.286596714529479, -0.131778331276228, 6.76682064330275E-03]; hs = h / 2800; ps = p / 100; Ts = 0; for i = 1 : 33 Ts = Ts + ni(i) * (ps + 0.298) ^ Ii(i) * (hs - 0.72) ^ Ji(i); end T3_ph = Ts * 860; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function v3_ph = v3_ph(p, h) //Revised Supplementary Release on Backward Equations for the functions T(p,h), v(p,h) and T(p,s), v(p,s) for Region 3 of the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //2004 //Section 3.3 Backward Equations T(p,h) and v(p,h) for Subregions 3a and 3b //Boundary equation, Eq 1 Page 5 h3ab = 2014.64004206875 + 3.74696550136983 * p - 2.19921901054187E-02 * p ^ 2 + 8.7513168600995E-05 * p ^ 3; if h < h3ab //Subregion 3a //Eq 4, Table 6, Page 9 Ii = [-12, -12, -12, -12, -10, -10, -10, -8, -8, -6, -6, -6, -4, -4, -3, -2, -2, -1, -1, -1, -1, 0, 0, 1, 1, 1, 2, 2, 3, 4, 5, 8]; Ji = [6, 8, 12, 18, 4, 7, 10, 5, 12, 3, 4, 22, 2, 3, 7, 3, 16, 0, 1, 2, 3, 0, 1, 0, 1, 2, 0, 2, 0, 2, 2, 2]; ni = [5.29944062966028E-03, -0.170099690234461, 11.1323814312927, -2178.98123145125, -5.06061827980875E-04, 0.556495239685324, -9.43672726094016, -0.297856807561527, 93.9353943717186, 1.92944939465981E-02, 0.421740664704763, -3689141.2628233, -7.37566847600639E-03, -0.354753242424366, -1.99768169338727, 1.15456297059049, 5683.6687581596, 8.08169540124668E-03, 0.172416341519307, 1.04270175292927, -0.297691372792847, 0.560394465163593, 0.275234661176914, -0.148347894866012, -6.51142513478515E-02, -2.92468715386302, 6.64876096952665E-02, 3.52335014263844, -1.46340792313332E-02, -2.24503486668184, 1.10533464706142, -4.08757344495612E-02]; ps = p / 100; hs = h / 2100; vs = 0; for i = 1 : 32 vs = vs + ni(i) * (ps + 0.128) ^ Ii(i) * (hs - 0.727) ^ Ji(i); end v3_ph = vs * 0.0028; else //Subregion 3b //Eq 5, Table 7, Page 9 Ii = [-12, -12, -8, -8, -8, -8, -8, -8, -6, -6, -6, -6, -6, -6, -4, -4, -4, -3, -3, -2, -2, -1, -1, -1, -1, 0, 1, 1, 2, 2]; Ji = [0, 1, 0, 1, 3, 6, 7, 8, 0, 1, 2, 5, 6, 10, 3, 6, 10, 0, 2, 1, 2, 0, 1, 4, 5, 0, 0, 1, 2, 6]; ni = [-2.25196934336318E-09, 1.40674363313486E-08, 2.3378408528056E-06, -3.31833715229001E-05, 1.07956778514318E-03, -0.271382067378863, 1.07202262490333, -0.853821329075382, -2.15214194340526E-05, 7.6965608822273E-04, -4.31136580433864E-03, 0.453342167309331, -0.507749535873652, -100.475154528389, -0.219201924648793, -3.21087965668917, 607.567815637771, 5.57686450685932E-04, 0.18749904002955, 9.05368030448107E-03, 0.285417173048685, 3.29924030996098E-02, 0.239897419685483, 4.82754995951394, -11.8035753702231, 0.169490044091791, -1.79967222507787E-02, 3.71810116332674E-02, -5.36288335065096E-02, 1.6069710109252]; ps = p / 100; hs = h / 2800; vs = 0; for i = 1 : 30 vs = vs + ni(i) * (ps + 0.0661) ^ Ii(i) * (hs - 0.72) ^ Ji(i); end v3_ph = vs * 0.0088; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T3_ps = T3_ps(p, s) //Revised Supplementary Release on Backward Equations for the functions T(p,h), v(p,h) and T(p,s), v(p,s) for Region 3 of the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //2004 //3.4 Backward Equations T(p,s) and v(p,s) for Subregions 3a and 3b //Boundary equation, Eq 6 Page 11 if s <= 4.41202148223476 //Subregion 3a //Eq 6, Table 10, Page 11 Ii = [-12, -12, -10, -10, -10, -10, -8, -8, -8, -8, -6, -6, -6, -5, -5, -5, -4, -4, -4, -2, -2, -1, -1, 0, 0, 0, 1, 2, 2, 3, 8, 8, 10]; Ji = [28, 32, 4, 10, 12, 14, 5, 7, 8, 28, 2, 6, 32, 0, 14, 32, 6, 10, 36, 1, 4, 1, 6, 0, 1, 4, 0, 0, 3, 2, 0, 1, 2]; ni = [1500420082.63875, -159397258480.424, 5.02181140217975E-04, -67.2057767855466, 1450.58545404456, -8238.8953488889, -0.154852214233853, 11.2305046746695, -29.7000213482822, 43856513263.5495, 1.37837838635464E-03, -2.97478527157462, 9717779473494.13, -5.71527767052398E-05, 28830.794977842, -74442828926270.3, 12.8017324848921, -368.275545889071, 6.64768904779177E+15, 0.044935925195888, -4.22897836099655, -0.240614376434179, -4.74341365254924, 0.72409399912611, 0.923874349695897, 3.99043655281015, 3.84066651868009E-02, -3.59344365571848E-03, -0.735196448821653, 0.188367048396131, 1.41064266818704E-04, -2.57418501496337E-03, 1.23220024851555E-03]; Sigma = s / 4.4; Pi = p / 100; teta = 0; for i = 1 : 33 teta = teta + ni(i) * (Pi + 0.24) ^ Ii(i) * (Sigma - 0.703) ^ Ji(i); end T3_ps = teta * 760; else //Subregion 3b //Eq 7, Table 11, Page 11 Ii = [-12, -12, -12, -12, -8, -8, -8, -6, -6, -6, -5, -5, -5, -5, -5, -4, -3, -3, -2, 0, 2, 3, 4, 5, 6, 8, 12, 14]; Ji = [1, 3, 4, 7, 0, 1, 3, 0, 2, 4, 0, 1, 2, 4, 6, 12, 1, 6, 2, 0, 1, 1, 0, 24, 0, 3, 1, 2]; ni = [0.52711170160166, -40.1317830052742, 153.020073134484, -2247.99398218827, -0.193993484669048, -1.40467557893768, 42.6799878114024, 0.752810643416743, 22.6657238616417, -622.873556909932, -0.660823667935396, 0.841267087271658, -25.3717501764397, 485.708963532948, 880.531517490555, 2650155.92794626, -0.359287150025783, -656.991567673753, 2.41768149185367, 0.856873461222588, 0.655143675313458, -0.213535213206406, 5.62974957606348E-03, -316955725450471, -6.99997000152457E-04, 1.19845803210767E-02, 1.93848122022095E-05, -2.15095749182309E-05]; Sigma = s / 5.3; Pi = p / 100; teta = 0; for i = 1 : 28 teta = teta + ni(i) * (Pi + 0.76) ^ Ii(i) * (Sigma - 0.818) ^ Ji(i); end T3_ps = teta * 860; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function v3_ps = v3_ps(p, s) //Revised Supplementary Release on Backward Equations for the functions T(p,h), v(p,h) and T(p,s), v(p,s) for Region 3 of the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //2004 //3.4 Backward Equations T(p,s) and v(p,s) for Subregions 3a and 3b //Boundary equation, Eq 6 Page 11 if s <= 4.41202148223476 //Subregion 3a //Eq 8, Table 13, Page 14 Ii = [-12, -12, -12, -10, -10, -10, -10, -8, -8, -8, -8, -6, -5, -4, -3, -3, -2, -2, -1, -1, 0, 0, 0, 1, 2, 4, 5, 6]; Ji = [10, 12, 14, 4, 8, 10, 20, 5, 6, 14, 16, 28, 1, 5, 2, 4, 3, 8, 1, 2, 0, 1, 3, 0, 0, 2, 2, 0]; ni = [79.5544074093975, -2382.6124298459, 17681.3100617787, -1.10524727080379E-03, -15.3213833655326, 297.544599376982, -35031520.6871242, 0.277513761062119, -0.523964271036888, -148011.182995403, 1600148.99374266, 1708023226634.27, 2.46866996006494E-04, 1.6532608479798, -0.118008384666987, 2.537986423559, 0.965127704669424, -28.2172420532826, 0.203224612353823, 1.10648186063513, 0.52612794845128, 0.277000018736321, 1.08153340501132, -7.44127885357893E-02, 1.64094443541384E-02, -6.80468275301065E-02, 0.025798857610164, -1.45749861944416E-04]; Pi = p / 100; Sigma = s / 4.4; omega = 0; for i = 1 : 28 omega = omega + ni(i) * (Pi + 0.187) ^ Ii(i) * (Sigma - 0.755) ^ Ji(i); end v3_ps = omega * 0.0028; else //Subregion 3b //Eq 9, Table 14, Page 14 Ii = [-12, -12, -12, -12, -12, -12, -10, -10, -10, -10, -8, -5, -5, -5, -4, -4, -4, -4, -3, -2, -2, -2, -2, -2, -2, 0, 0, 0, 1, 1, 2]; Ji = [0, 1, 2, 3, 5, 6, 0, 1, 2, 4, 0, 1, 2, 3, 0, 1, 2, 3, 1, 0, 1, 2, 3, 4, 12, 0, 1, 2, 0, 2, 2]; ni = [5.91599780322238E-05, -1.85465997137856E-03, 1.04190510480013E-02, 5.9864730203859E-03, -0.771391189901699, 1.72549765557036, -4.67076079846526E-04, 1.34533823384439E-02, -8.08094336805495E-02, 0.508139374365767, 1.28584643361683E-03, -1.63899353915435, 5.86938199318063, -2.92466667918613, -6.14076301499537E-03, 5.76199014049172, -12.1613320606788, 1.67637540957944, -7.44135838773463, 3.78168091437659E-02, 4.01432203027688, 16.0279837479185, 3.17848779347728, -3.58362310304853, -1159952.60446827, 0.199256573577909, -0.122270624794624, -19.1449143716586, -1.50448002905284E-02, 14.6407900162154, -3.2747778718823]; Pi = p / 100; Sigma = s / 5.3; omega = 0; for i = 1 : 31 omega = omega + ni(i) * (Pi + 0.298) ^ Ii(i) * (Sigma - 0.816) ^ Ji(i); end v3_ps = omega * 0.0088; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function p3_hs = p3_hs(h, s) //Supplementary Release on Backward Equations ( ) , p h s for Region 3, //Equations as a function of h and s for the Region Boundaries, and an Equation //( ) sat , T hs for Region 4 of the IAPWS Industrial formulation 1997 for the //Thermodynamic Properties of Water and Steam //2004 //Section 3 Backward functions p(h,s), T(h,s), and v(h,s) for Region 3 if s < 4.41202148223476 //Subregion 3a //Eq 1, Table 3, Page 8 Ii = [0, 0, 0, 1, 1, 1, 1, 1, 2, 2, 3, 3, 3, 4, 4, 4, 4, 5, 6, 7, 8, 10, 10, 14, 18, 20, 22, 22, 24, 28, 28, 32, 32]; Ji = [0, 1, 5, 0, 3, 4, 8, 14, 6, 16, 0, 2, 3, 0, 1, 4, 5, 28, 28, 24, 1, 32, 36, 22, 28, 36, 16, 28, 36, 16, 36, 10, 28]; ni = [7.70889828326934, -26.0835009128688, 267.416218930389, 17.2221089496844, -293.54233214597, 614.135601882478, -61056.2757725674, -65127225.1118219, 73591.9313521937, -11664650591.4191, 35.5267086434461, -596.144543825955, -475.842430145708, 69.6781965359503, 335.674250377312, 25052.6809130882, 146997.380630766, 5.38069315091534E+19, 1.43619827291346E+21, 3.64985866165994E+19, -2547.41561156775, 2.40120197096563E+27, -3.93847464679496E+29, 1.47073407024852E+24, -4.26391250432059E+31, 1.94509340621077E+38, 6.66212132114896E+23, 7.06777016552858E+33, 1.75563621975576E+41, 1.08408607429124E+28, 7.30872705175151E+43, 1.5914584739887E+24, 3.77121605943324E+40]; Sigma = s / 4.4; eta = h / 2300; Pi = 0; for i = 1 : 33 Pi = Pi + ni(i) * (eta - 1.01) ^ Ii(i) * (Sigma - 0.75) ^ Ji(i); end p3_hs = Pi * 99; else //Subregion 3b //Eq 2, Table 4, Page 8 Ii = [-12, -12, -12, -12, -12, -10, -10, -10, -10, -8, -8, -6, -6, -6, -6, -5, -4, -4, -4, -3, -3, -3, -3, -2, -2, -1, 0, 2, 2, 5, 6, 8, 10, 14, 14]; Ji = [2, 10, 12, 14, 20, 2, 10, 14, 18, 2, 8, 2, 6, 7, 8, 10, 4, 5, 8, 1, 3, 5, 6, 0, 1, 0, 3, 0, 1, 0, 1, 1, 1, 3, 7]; ni = [1.25244360717979E-13, -1.26599322553713E-02, 5.06878030140626, 31.7847171154202, -391041.161399932, -9.75733406392044E-11, -18.6312419488279, 510.973543414101, 373847.005822362, 2.99804024666572E-08, 20.0544393820342, -4.98030487662829E-06, -10.230180636003, 55.2819126990325, -206.211367510878, -7940.12232324823, 7.82248472028153, -58.6544326902468, 3550.73647696481, -1.15303107290162E-04, -1.75092403171802, 257.98168774816, -727.048374179467, 1.21644822609198E-04, 3.93137871762692E-02, 7.04181005909296E-03, -82.910820069811, -0.26517881813125, 13.7531682453991, -52.2394090753046, 2405.56298941048, -22736.1631268929, 89074.6343932567, -23923456.5822486, 5687958081.29714]; Sigma = s / 5.3; eta = h / 2800; Pi = 0; for i = 1 : 35 Pi = Pi + ni(i) * (eta - 0.681) ^ Ii(i) * (Sigma - 0.792) ^ Ji(i); end p3_hs = 16.6 / Pi; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function h3_pT = h3_pT(p, T) //Not avalible with if 97 //Solve function T3_ph-T=0 with half interval method. Ts = T+1; Low_Bound = h1_pT(p, 623.15); High_Bound = h2_pT(p, B23T_p(p)); while abs(T - Ts) > 0.00001 hs = (Low_Bound + High_Bound) / 2; Ts = T3_ph(p, hs); if Ts > T High_Bound = hs; else Low_Bound = hs; end end h3_pT = hs; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T3_prho = T3_prho(p, rho) //Solve by iteration. Observe that fo low temperatures this equation has 2 solutions. //Solve with half interval method Low_Bound = 623.15; High_Bound = 1073.15; ps=-1000; while abs(p - ps) > 0.00000001 Ts = (Low_Bound + High_Bound) / 2; ps = p3_rhoT(rho, Ts); if ps > p High_Bound = Ts; else Low_Bound = Ts; end end T3_prho = Ts; //*********************************************************************************************************** //*2.4 functions for region 4 endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function p4_T = p4_T(T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Section 8.1 The Saturation-Pressure Equation //Eq 30, Page 33 teta = T - 0.23855557567849 / (T - 650.17534844798); a = teta ^ 2 + 1167.0521452767 * teta - 724213.16703206; B = -17.073846940092 * teta ^ 2 + 12020.82470247 * teta - 3232555.0322333; C = 14.91510861353 * teta ^ 2 - 4823.2657361591 * teta + 405113.40542057; p4_T = (2 * C / (-B + (B ^ 2 - 4 * a * C) ^ 0.5)) ^ 4; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T4_p = T4_p(p) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Section 8.2 The Saturation-Temperature Equation //Eq 31, Page 34 Beta = p ^ 0.25; E = Beta ^ 2 - 17.073846940092 * Beta + 14.91510861353; f = 1167.0521452767 * Beta ^ 2 + 12020.82470247 * Beta - 4823.2657361591; G = -724213.16703206 * Beta ^ 2 - 3232555.0322333 * Beta + 405113.40542057; D = 2 * G / (-f - (f ^ 2 - 4 * E * G) ^ 0.5); T4_p = (650.17534844798 + D - ((650.17534844798 + D) ^ 2 - 4 * (-0.23855557567849 + 650.17534844798 * D)) ^ 0.5) / 2; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function h4_s = h4_s(s) //Supplementary Release on Backward Equations ( ) , p h s for Region 3,Equations as a function of h and s for the Region Boundaries, and an Equation( ) sat , T hs for Region 4 of the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //4 Equations for Region Boundaries Given Enthalpy and Entropy // Se picture page 14 if (s > -0.0001545495919 & s <= 3.77828134) //hL1_s //Eq 3,Table 9,Page 16 Ii = [0, 0, 1, 1, 2, 2, 3, 3, 4, 4, 4, 5, 5, 7, 8, 12, 12, 14, 14, 16, 20, 20, 22, 24, 28, 32, 32]; Ji = [14, 36, 3, 16, 0, 5, 4, 36, 4, 16, 24, 18, 24, 1, 4, 2, 4, 1, 22, 10, 12, 28, 8, 3, 0, 6, 8]; ni = [0.332171191705237, 6.11217706323496E-04, -8.82092478906822, -0.45562819254325, -2.63483840850452E-05, -22.3949661148062, -4.28398660164013, -0.616679338856916, -14.682303110404, 284.523138727299, -113.398503195444, 1156.71380760859, 395.551267359325, -1.54891257229285, 19.4486637751291, -3.57915139457043, -3.35369414148819, -0.66442679633246, 32332.1885383934, 3317.66744667084, -22350.1257931087, 5739538.75852936, 173.226193407919, -3.63968822121321E-02, 8.34596332878346E-07, 5.03611916682674, 65.5444787064505]; Sigma = s / 3.8; eta = 0; for i = 1 : 27 eta = eta + ni(i) * (Sigma - 1.09) ^ Ii(i) * (Sigma + 0.0000366) ^ Ji(i); end h4_s = eta * 1700; elseif (s > 3.77828134 & s <= 4.41202148223476 ) //hL3_s //Eq 4,Table 10,Page 16 Ii = [0, 0, 0, 0, 2, 3, 4, 4, 5, 5, 6, 7, 7, 7, 10, 10, 10, 32, 32]; Ji = [1, 4, 10, 16, 1, 36, 3, 16, 20, 36, 4, 2, 28, 32, 14, 32, 36, 0, 6]; ni = [0.822673364673336, 0.181977213534479, -0.011200026031362, -7.46778287048033E-04, -0.179046263257381, 4.24220110836657E-02, -0.341355823438768, -2.09881740853565, -8.22477343323596, -4.99684082076008, 0.191413958471069, 5.81062241093136E-02, -1655.05498701029, 1588.70443421201, -85.0623535172818, -31771.4386511207, -94589.0406632871, -1.3927384708869E-06, 0.63105253224098]; Sigma = s / 3.8; eta = 0; for i = 1 : 19 eta = eta + ni(i) * (Sigma - 1.09) ^ Ii(i) * (Sigma + 0.0000366) ^ Ji(i); end h4_s = eta * 1700; elseif (s > 4.41202148223476 & s <= 5.85 ) //Section 4.4 Equations ( ) 2ab " h s and ( ) 2c3b "h s for the Saturated Vapor Line //Page 19, Eq 5 //hV2c3b_s(s) Ii = [0, 0, 0, 1, 1, 5, 6, 7, 8, 8, 12, 16, 22, 22, 24, 36]; Ji = [0, 3, 4, 0, 12, 36, 12, 16, 2, 20, 32, 36, 2, 32, 7, 20]; ni = [1.04351280732769, -2.27807912708513, 1.80535256723202, 0.420440834792042, -105721.24483466, 4.36911607493884E+24, -328032702839.753, -6.7868676080427E+15, 7439.57464645363, -3.56896445355761E+19, 1.67590585186801E+31, -3.55028625419105E+37, 396611982166.538, -4.14716268484468E+40, 3.59080103867382E+18, -1.16994334851995E+40]; Sigma = s / 5.9; eta = 0; for i = 1 : 16 eta = eta + ni(i) * (Sigma - 1.02) ^ Ii(i) * (Sigma - 0.726) ^ Ji(i); end h4_s = eta ^ 4 * 2800; elseif (s > 5.85 & s < 9.155759395) //Section 4.4 Equations ( ) 2ab " h s and ( ) 2c3b "h s for the Saturated Vapor Line //Page 20, Eq 6 Ii = [1, 1, 2, 2, 4, 4, 7, 8, 8, 10, 12, 12, 18, 20, 24, 28, 28, 28, 28, 28, 32, 32, 32, 32, 32, 36, 36, 36, 36, 36]; Ji = [8, 24, 4, 32, 1, 2, 7, 5, 12, 1, 0, 7, 10, 12, 32, 8, 12, 20, 22, 24, 2, 7, 12, 14, 24, 10, 12, 20, 22, 28]; ni = [-524.581170928788, -9269472.18142218, -237.385107491666, 21077015581.2776, -23.9494562010986, 221.802480294197, -5104725.33393438, 1249813.96109147, 2000084369.96201, -815.158509791035, -157.612685637523, -11420042233.2791, 6.62364680776872E+15, -2.27622818296144E+18, -1.71048081348406E+31, 6.60788766938091E+15, 1.66320055886021E+22, -2.18003784381501E+29, -7.87276140295618E+29, 1.51062329700346E+31, 7957321.70300541, 1.31957647355347E+15, -3.2509706829914E+23, -4.18600611419248E+25, 2.97478906557467E+34, -9.53588761745473E+19, 1.66957699620939E+24, -1.75407764869978E+32, 3.47581490626396E+34, -7.10971318427851E+38]; Sigma1 = s / 5.21; Sigma2 = s / 9.2; eta = 0; for i = 1 : 30 eta = eta + ni(i) * (1 / Sigma1 - 0.513) ^ Ii(i) * (Sigma2 - 0.524) ^ Ji(i); end h4_s = exp(eta) * 2800; else h4_s = -99999; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function p4_s = p4_s(s) //Uses h4_s and p_hs for the diffrent regions to determine p4_s h_sat = h4_s(s); if (s > -0.0001545495919 & s <= 3.77828134) p4_s = p1_hs(hsat, s); elseif (s > 3.77828134 & s <= 5.210887663) p4_s = p3_hs(hsat, s); elseif (s > 5.210887663 & s < 9.155759395) p4_s = p2_hs(hsat, s); else p4_s = -99999; end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function h4L_p = h4L_p(p) if (p > 0.000611657 & p < 22.06395) Ts = T4_p(p); if p < 16.529 h4L_p = h1_pT(p, Ts); else //Iterate to find the the backward solution of p3sat_h Low_Bound = 1670.858218; High_Bound = 2087.23500164864; ps=-1000; while abs(p - ps) > 0.00001 hs = (Low_Bound + High_Bound) / 2; ps = p3sat_h(hs); if ps > p High_Bound = hs; else Low_Bound = hs; end end h4L_p = hs; end else h4L_p = -99999 end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function h4V_p = h4V_p(p) if (p > 0.000611657 & p < 22.06395) Ts = T4_p(p); if p < 16.529 h4V_p = h2_pT(p, Ts); else //Iterate to find the the backward solution of p3sat_h Low_Bound = 2087.23500164864; High_Bound = 2563.592004+5; ps=-1000; while abs(p - ps) > 0.000001 hs = (Low_Bound + High_Bound) / 2; ps = p3sat_h(hs); if ps < p High_Bound = hs; else Low_Bound = hs; end end h4V_p = hs; end else h4V_p = -99999 end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function x4_ph = x4_ph(p, h) //Calculate vapour fraction from hL and hV for given p h4v = h4V_p(p); h4L = h4L_p(p); if h > h4v x4_ph = 1; elseif h < h4L x4_ph = 0; else x4_ph = (h - h4L) / (h4v - h4L); end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function x4_ps = x4_ps(p, s) if p < 16.529 ssv = s2_pT(p, T4_p(p)); ssL = s1_pT(p, T4_p(p)); else ssv = s3_rhoT(1 / (v3_ph(p, h4V_p(p))), T4_p(p)); ssL = s3_rhoT(1 / (v3_ph(p, h4L_p(p))), T4_p(p)); end if s < ssL x4_ps = 0; elseif s > ssv x4_ps = 1; else x4_ps = (s - ssL) / (ssv - ssL); end endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T4_hs = T4_hs(h, s) //Supplementary Release on Backward Equations ( ) , p h s for Region 3, //Chapter 5.3 page 30. //The if 97 function is only valid for part of region4. Use iteration outsida. Ii = [0, 0, 0, 1, 1, 1, 1, 2, 2, 2, 3, 3, 3, 3, 4, 4, 5, 5, 5, 5, 6, 6, 6, 8, 10, 10, 12, 14, 14, 16, 16, 18, 18, 18, 20, 28]; Ji = [0, 3, 12, 0, 1, 2, 5, 0, 5, 8, 0, 2, 3, 4, 0, 1, 1, 2, 4, 16, 6, 8, 22, 1, 20, 36, 24, 1, 28, 12, 32, 14, 22, 36, 24, 36]; ni = [0.179882673606601, -0.267507455199603, 1.162767226126, 0.147545428713616, -0.512871635973248, 0.421333567697984, 0.56374952218987, 0.429274443819153, -3.3570455214214, 10.8890916499278, -0.248483390456012, 0.30415322190639, -0.494819763939905, 1.07551674933261, 7.33888415457688E-02, 1.40170545411085E-02, -0.106110975998808, 1.68324361811875E-02, 1.25028363714877, 1013.16840309509, -1.51791558000712, 52.4277865990866, 23049.5545563912, 2.49459806365456E-02, 2107964.67412137, 366836848.613065, -144814105.365163, -1.7927637300359E-03, 4899556021.00459, 471.262212070518, -82929439019.8652, -1715.45662263191, 3557776.82973575, 586062760258.436, -12988763.5078195, 31724744937.1057]; if (s > 5.210887825 & s < 9.15546555571324) Sigma = s / 9.2; eta = h / 2800; teta = 0; for i = 1 : 36 teta = teta + ni(i) * (eta - 0.119) ^ Ii(i) * (Sigma - 1.07) ^ Ji(i); end T4_hs = teta * 550; else //function psat_h if (s > -0.0001545495919 & s <= 3.77828134) Low_Bound = 0.000611; High_Bound = 165.291642526045; hL=-1000; while abs(hL - h) > 0.00001 & abs(High_Bound - Low_Bound) > 0.0001 PL = (Low_Bound + High_Bound) / 2; Ts = T4_p(PL); hL = h1_pT(PL, Ts); if hL > h High_Bound = PL; else Low_Bound = PL; end end elseif s > 3.77828134 & s <= 4.41202148223476 PL = p3sat_h(h); elseif s > 4.41202148223476 & s <= 5.210887663 PL = p3sat_h(h); end Low_Bound = 0.000611; High_Bound = PL; sss=-1000; while (abs(s - sss) > 0.000001 & abs(High_Bound - Low_Bound) > 0.0000001) p = (Low_Bound + High_Bound) / 2; //Calculate s4_ph Ts = T4_p(p); xs = x4_ph(p, h); if p < 16.529 s4v = s2_pT(p, Ts); s4L = s1_pT(p, Ts); else v4v = v3_ph(p, h4V_p(p)); s4v = s3_rhoT(1 / v4v, Ts); v4L = v3_ph(p, h4L_p(p)); s4L = s3_rhoT(1 / v4L, Ts); end sss = (xs * s4v + (1 - xs) * s4L); if sss < s High_Bound = p; else Low_Bound = p; end end T4_hs = T4_p(p); end //*********************************************************************************************************** //*2.5 functions for region 5 endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function h5_pT = h5_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Basic Equation for Region 5 //Eq 32,33, Page 36, Tables 37-41 Ji0 = [0, 1, -3, -2, -1, 2]; ni0 = [-13.179983674201, 6.8540841634434, -0.024805148933466, 0.36901534980333, -3.1161318213925, -0.32961626538917]; Iir = [1, 1, 1, 2, 3]; Jir = [0, 1, 3, 9, 3]; nir = [-1.2563183589592E-04, 2.1774678714571E-03, -0.004594282089991, -3.9724828359569E-06, 1.2919228289784E-07]; R = 0.461526; //kJ/(kg K) tau = 1000 / T; Pi = p; gamma0_tau = 0; for i = 1 : 6 gamma0_tau = gamma0_tau + ni0(i) * Ji0(i) * tau ^ (Ji0(i) - 1); end gammar_tau = 0; for i = 1 : 5 gammar_tau = gammar_tau + nir(i) * Pi ^ Iir(i) * Jir(i) * tau ^ (Jir(i) - 1); end h5_pT = R * T * tau * (gamma0_tau + gammar_tau); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function v5_pT = v5_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Basic Equation for Region 5 //Eq 32,33, Page 36, Tables 37-41 Ji0 = [0, 1, -3, -2, -1, 2]; ni0 = [-13.179983674201, 6.8540841634434, -0.024805148933466, 0.36901534980333, -3.1161318213925, -0.32961626538917]; Iir = [1, 1, 1, 2, 3]; Jir = [0, 1, 3, 9, 3]; nir = [-1.2563183589592E-04, 2.1774678714571E-03, -0.004594282089991, -3.9724828359569E-06, 1.2919228289784E-07]; R = 0.461526; //kJ/(kg K) tau = 1000 / T; Pi = p; gamma0_pi = 1 / Pi; gammar_pi = 0; for i = 1 : 5 gammar_pi = gammar_pi + nir(i) * Iir(i) * Pi ^ (Iir(i) - 1) * tau ^ Jir(i); end v5_pT = R * T / p * Pi * (gamma0_pi + gammar_pi) / 1000; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function u5_pT = u5_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Basic Equation for Region 5 //Eq 32,33, Page 36, Tables 37-41 Ji0 = [0, 1, -3, -2, -1, 2]; ni0 = [-13.179983674201, 6.8540841634434, -0.024805148933466, 0.36901534980333, -3.1161318213925, -0.32961626538917]; Iir = [1, 1, 1, 2, 3]; Jir = [0, 1, 3, 9, 3]; nir = [-1.2563183589592E-04, 2.1774678714571E-03, -0.004594282089991, -3.9724828359569E-06, 1.2919228289784E-07]; R = 0.461526; //kJ/(kg K) tau = 1000 / T; Pi = p; gamma0_pi = 1 / Pi; gamma0_tau = 0; for i = 1 : 6 gamma0_tau = gamma0_tau + ni0(i) * Ji0(i) * tau ^ (Ji0(i) - 1); end gammar_pi = 0; gammar_tau = 0; for i = 1 : 5 gammar_pi = gammar_pi + nir(i) * Iir(i) * Pi ^ (Iir(i) - 1) * tau ^ Jir(i); gammar_tau = gammar_tau + nir(i) * Pi ^ Iir(i) * Jir(i) * tau ^ (Jir(i) - 1); end u5_pT = R * T * (tau * (gamma0_tau + gammar_tau) - Pi * (gamma0_pi + gammar_pi)); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Cp5_pT = Cp5_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Basic Equation for Region 5 //Eq 32,33, Page 36, Tables 37-41 Ji0 = [0, 1, -3, -2, -1, 2]; ni0 = [-13.179983674201, 6.8540841634434, -0.024805148933466, 0.36901534980333, -3.1161318213925, -0.32961626538917]; Iir = [1, 1, 1, 2, 3]; Jir = [0, 1, 3, 9, 3]; nir = [-1.2563183589592E-04, 2.1774678714571E-03, -0.004594282089991, -3.9724828359569E-06, 1.2919228289784E-07]; R = 0.461526; //kJ/(kg K) tau = 1000 / T; Pi = p; gamma0_tautau = 0; for i = 1 : 6 gamma0_tautau = gamma0_tautau + ni0(i) * Ji0(i) * (Ji0(i) - 1) * tau ^ (Ji0(i) - 2); end gammar_tautau = 0; for i = 1 : 5 gammar_tautau = gammar_tautau + nir(i) * Pi ^ Iir(i) * Jir(i) * (Jir(i) - 1) * tau ^ (Jir(i) - 2); end Cp5_pT = -R * tau ^ 2 * (gamma0_tautau + gammar_tautau); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function s5_pT = s5_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Basic Equation for Region 5 //Eq 32,33, Page 36, Tables 37-41 Ji0 = [0, 1, -3, -2, -1, 2]; ni0 = [-13.179983674201, 6.8540841634434, -0.024805148933466, 0.36901534980333, -3.1161318213925, -0.32961626538917]; Iir = [1, 1, 1, 2, 3]; Jir = [0, 1, 3, 9, 3]; nir = [-1.2563183589592E-04, 2.1774678714571E-03, -0.004594282089991, -3.9724828359569E-06, 1.2919228289784E-07]; R = 0.461526; //kJ/(kg K) tau = 1000 / T; Pi = p; gamma0 = log(Pi); gamma0_tau = 0; for i = 1 : 6 gamma0_tau = gamma0_tau + ni0(i) * Ji0(i) * tau ^ (Ji0(i) - 1); gamma0 = gamma0 + ni0(i) * tau ^ Ji0(i); end gammar = 0; gammar_tau = 0; for i = 1 : 5 gammar = gammar + nir(i) * Pi ^ Iir(i) * tau ^ Jir(i); gammar_tau = gammar_tau + nir(i) * Pi ^ Iir(i) * Jir(i) * tau ^ (Jir(i) - 1); end s5_pT = R * (tau * (gamma0_tau + gammar_tau) - (gamma0 + gammar)); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Cv5_pT = Cv5_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Basic Equation for Region 5 //Eq 32,33, Page 36, Tables 37-41 Ji0 = [0, 1, -3, -2, -1, 2]; ni0 = [-13.179983674201, 6.8540841634434, -0.024805148933466, 0.36901534980333, -3.1161318213925, -0.32961626538917]; Iir = [1, 1, 1, 2, 3]; Jir = [0, 1, 3, 9, 3]; nir = [-1.2563183589592E-04, 2.1774678714571E-03, -0.004594282089991, -3.9724828359569E-06, 1.2919228289784E-07]; R = 0.461526; //kJ/(kg K) tau = 1000 / T; Pi = p; gamma0_tautau = 0; for i = 1 : 6 gamma0_tautau = gamma0_tautau + ni0(i) * (Ji0(i) - 1) * Ji0(i) * tau ^ (Ji0(i) - 2); end gammar_pi = 0; gammar_pitau = 0; gammar_pipi = 0; gammar_tautau = 0; for i = 1 : 5 gammar_pi = gammar_pi + nir(i) * Iir(i) * Pi ^ (Iir(i) - 1) * tau ^ Jir(i); gammar_pitau = gammar_pitau + nir(i) * Iir(i) * Pi ^ (Iir(i) - 1) * Jir(i) * tau ^ (Jir(i) - 1); gammar_pipi = gammar_pipi + nir(i) * Iir(i) * (Iir(i) - 1) * Pi ^ (Iir(i) - 2) * tau ^ Jir(i); gammar_tautau = gammar_tautau + nir(i) * Pi ^ Iir(i) * Jir(i) * (Jir(i) - 1) * tau ^ (Jir(i) - 2); end Cv5_pT = R * (tau ^ 2 * (-(gamma0_tautau + gammar_tautau)) - (1 + Pi * gammar_pi - tau * Pi * gammar_pitau) / (1 - Pi ^ 2 * gammar_pipi)); endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function w5_pT = w5_pT(p, T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam, September 1997 //Basic Equation for Region 5 //Eq 32,33, Page 36, Tables 37-41 Ji0 = [0, 1, -3, -2, -1, 2]; ni0 = [-13.179983674201, 6.8540841634434, -0.024805148933466, 0.36901534980333, -3.1161318213925, -0.32961626538917]; Iir = [1, 1, 1, 2, 3]; Jir = [0, 1, 3, 9, 3]; nir = [-1.2563183589592E-04, 2.1774678714571E-03, -0.004594282089991, -3.9724828359569E-06, 1.2919228289784E-07]; R = 0.461526; //kJ/(kg K) tau = 1000 / T; Pi = p; gamma0_tautau = 0; for i = 1 : 6 gamma0_tautau = gamma0_tautau + ni0(i) * (Ji0(i) - 1) * Ji0(i) * tau ^ (Ji0(i) - 2); end gammar_pi = 0; gammar_pitau = 0; gammar_pipi = 0; gammar_tautau = 0; for i = 1 : 5 gammar_pi = gammar_pi + nir(i) * Iir(i) * Pi ^ (Iir(i) - 1) * tau ^ Jir(i); gammar_pitau = gammar_pitau + nir(i) * Iir(i) * Pi ^ (Iir(i) - 1) * Jir(i) * tau ^ (Jir(i) - 1); gammar_pipi = gammar_pipi + nir(i) * Iir(i) * (Iir(i) - 1) * Pi ^ (Iir(i) - 2) * tau ^ Jir(i); gammar_tautau = gammar_tautau + nir(i) * Pi ^ Iir(i) * Jir(i) * (Jir(i) - 1) * tau ^ (Jir(i) - 2); end w5_pT = (1000 * R * T * (1 + 2 * Pi * gammar_pi + Pi ^ 2 * gammar_pi ^ 2) / ((1 - Pi ^ 2 * gammar_pipi) + (1 + Pi * gammar_pi - tau * Pi * gammar_pitau) ^ 2 / (tau ^ 2 * (gamma0_tautau + gammar_tautau)))) ^ 0.5; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T5_ph = T5_ph(p, h) //Solve with half interval method Low_Bound = 1073.15; High_Bound = 2273.15; hs=h-1; while abs(h - hs) > 0.00001 Ts = (Low_Bound + High_Bound) / 2; hs = h5_pT(p, Ts); if hs > h High_Bound = Ts; else Low_Bound = Ts; end end T5_ph = Ts; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T5_ps = T5_ps(p, s) //Solve with half interval method Low_Bound = 1073.15; High_Bound = 2273.15; ss=s-1; while abs(s - ss) > 0.00001 Ts = (Low_Bound + High_Bound) / 2; ss = s5_pT(p, Ts); if ss > s High_Bound = Ts; else Low_Bound = Ts; end end T5_ps = Ts; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function T5_prho=T5_prho(p,rho) //Solve by iteration. Observe that fo low temperatures this equation has 2 solutions. //Solve with half interval method Low_Bound = 1073.15; High_Bound = 2073.15; rhos=-1000; while abs(rho - rhos) > 0.000001 Ts = (Low_Bound + High_Bound) / 2; rhos = 1 / v2_pT(p, Ts); if rhos < rho High_Bound = Ts; else Low_Bound = Ts; end end T5_prho = Ts; //*********************************************************************************************************** //*3 Region Selection //*********************************************************************************************************** //*3.1 Regions as a function of pT endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function region_pT = region_pT(p, T) if T > 1073.15 & p < 10 & T < 2273.15 & p > 0.000611 region_pT = 5; elseif T <= 1073.15 & T > 273.15 & p <= 100 & p > 0.000611 if T > 623.15 if p > B23p_T(T) region_pT = 3; if T < 647.096 ps = p4_T(T); if abs(p - ps) < 0.00001 region_pT = 4; end end else region_pT = 2; end else ps = p4_T(T); if abs(p - ps) < 0.00001 region_pT = 4; elseif p > ps region_pT = 1; else region_pT = 2; end end else region_pT = 0; //**Error, Outside valid area end //*********************************************************************************************************** //*3.2 Regions as a function of ph endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function region_ph = region_ph( p, h) //Check if outside pressure limits if p < 0.000611657 | p > 100 region_ph = 0; return end //Check if outside low h. if h < 0.963 * p + 2.2 //Linear adaption to h1_pt()+2 to speed up calcualations. if h < h1_pT(p, 273.15) region_ph = 0; return end end if p < 16.5292 //Bellow region 3,Check region 1,4,2,5 //Check Region 1 Ts = T4_p(p); hL = 109.6635 * log(p) + 40.3481 * p + 734.58; //Approximate function for hL_p if abs(h - hL) < 100 //if approximate is not god enough use real function hL = h1_pT(p, Ts); end if h <= hL region_ph = 1; return end //Check Region 4 hV = 45.1768 * log(p) - 20.158 * p + 2804.4; //Approximate function for hV_p if abs(h - hV) < 50 //if approximate is not god enough use real function hV = h2_pT(p, Ts); end if h < hV region_ph = 4; return end //Check upper limit of region 2 Quick Test if h < 4000 region_ph = 2; return end //Check region 2 (Real value) h_45 = h2_pT(p, 1073.15); if h <= h_45 region_ph = 2; return end //Check region 5 if p > 10 region_ph = 0; return end h_5u = h5_pT(p, 2273.15); if h < h_5u region_ph = 5; return end region_ph = 0; return else //for p>16.5292 //Check if in region1 if h < h1_pT(p, 623.15) region_ph = 1; return end //Check if in region 3 or 4 (Bellow Reg 2) if h < h2_pT(p, B23T_p(p)) //Region 3 or 4 if p > p3sat_h(h) region_ph = 3; return else region_ph = 4; return end end //Check if region 2 if h < h2_pT(p, 1073.15) region_ph = 2; return end end region_ph = 0; //*********************************************************************************************************** //*3.3 Regions as a function of ps endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function region_ps = region_ps( p, s) if p < 0.000611657 | p > 100 | s < 0 | s > s5_pT(p, 2273.15) region_ps = 0; return end //Check region 5 if s > s2_pT(p, 1073.15) if p <= 10 region_ps = 5; return else region_ps = 0; return end end //Check region 2 if p > 16.529 ss = s2_pT(p, B23T_p(p)); //Between 5.047 & 5.261. Use to speed up! else ss = s2_pT(p, T4_p(p)); end if s > ss region_ps = 2; return end //Check region 3 ss = s1_pT(p, 623.15); if p > 16.529 & s > ss if p > p3sat_s(s) region_ps = 3; return else region_ps = 4; return end end //Check region 4 (Not inside region 3) if p < 16.529 & s > s1_pT(p, T4_p(p)) region_ps = 4; return end //Check region 1 if p > 0.000611657 & s > s1_pT(p, 273.15) region_ps = 1; return end region_ps = 1; //*********************************************************************************************************** //*3.4 Regions as a function of hs endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function region_hs = region_hs( h, s) if s < -0.0001545495919 region_hs = 0; return end //Check linear adaption to p=0.000611. if bellow region 4. hMin = (((-0.0415878 - 2500.89262) / (-0.00015455 - 9.155759)) * s); if s < 9.155759395 & h < hMin region_hs = 0; return end //******Kolla 1 eller 4. (+liten bit över B13) if s >= -0.0001545495919 & s <= 3.77828134 if h < h4_s(s) region_hs = 4; return elseif s < 3.397782955 //100MPa line is limiting TMax = T1_ps(100, s); hMax = h1_pT(100, TMax); if h < hMax region_hs = 1; return else region_hs = 0; return end else //The point is either in region 4,1,3. Check B23 hB = hB13_s(s); if h < hB region_hs = 1; return end TMax = T3_ps(100, s); vmax = v3_ps(100, s); hMax = h3_rhoT(1 / vmax, TMax); if h < hMax region_hs = 3; return else region_hs = 0; return end end end //******Kolla region 2 eller 4. (Övre delen av område b23-> max) if s >= 5.260578707 & s <= 11.9212156897728 if s > 9.155759395 //Above region 4 Tmin = T2_ps(0.000611, s); hMin = h2_pT(0.000611, Tmin); //function adapted to h(1073.15,s) hMax = -0.07554022 * s ^ 4 + 3.341571 * s ^ 3 - 55.42151 * s ^ 2 + 408.515 * s + 3031.338; if h > hMin & h < hMax region_hs = 2; return else region_hs = 0; return end end hV = h4_s(s); if h < hV //Region 4. Under region 3. region_hs = 4; return end if s < 6.04048367171238 TMax = T2_ps(100, s); hMax = h2_pT(100, TMax); else //function adapted to h(1073.15,s) hMax = -2.988734 * s ^ 4 + 121.4015 * s ^ 3 - 1805.15 * s ^ 2 + 11720.16 * s - 23998.33; end if h < hMax //Region 2. Över region 4. region_hs = 2; return else region_hs = 0; return end end //Kolla region 3 eller 4. Under kritiska punkten. if s >= 3.77828134 & s <= 4.41202148223476 hL = h4_s(s); if h < hL region_hs = 4; return end TMax = T3_ps(100, s); vmax = v3_ps(100, s); hMax = h3_rhoT(1 / vmax, TMax); if h < hMax region_hs = 3; return else region_hs = 0; return end end //Kolla region 3 eller 4 från kritiska punkten till övre delen av b23 if s >= 4.41202148223476 & s <= 5.260578707 hV = h4_s(s); if h < hV region_hs = 4; return end //Kolla om vi är under b23 giltighetsområde. if s <= 5.048096828 TMax = T3_ps(100, s); vmax = v3_ps(100, s); hMax = h3_rhoT(1 / vmax, TMax); if h < hMax region_hs = 3; return else region_hs = 0; return end else //Inom området för B23 i s led. if (h > 2812.942061) //Ovanför B23 i h_led if s > 5.09796573397125 TMax = T2_ps(100, s); hMax = h2_pT(100, TMax); if h < hMax region_hs = 2; return else region_hs = 0; return end else region_hs = 0; return end end if (h < 2563.592004) //Nedanför B23 i h_led men vi har redan kollat ovanför hV2c3b region_hs = 3; return end //Vi är inom b23 området i både s och h led. Tact = TB23_hs(h, s); pact = p2_hs(h, s); pBound = B23p_T(Tact); if pact > pBound region_hs = 3; return else region_hs = 2; return end end end region_hs = 0; //*********************************************************************************************************** //*3.5 Regions as a function of p and rho endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Region_prho = Region_prho(p,rho) v = 1 / rho; if p < 0.000611657 | p > 100 Region_prho = 0; return end if p < 16.5292 //Bellow region 3, Check region 1,4,2 if v < v1_pT(p, 273.15) //Observe that this is not actually min of v. Not valid Water of 4°C is ligther. Region_prho = 0; return end if v <= v1_pT(p, T4_p(p)) Region_prho = 1; return end if v < v2_pT(p, T4_p(p)) Region_prho = 4; return end if v <= v2_pT(p, 1073.15) Region_prho = 2; return end if p > 10 //Above region 5 Region_prho = 0; return end if v <= v5_pT(p, 2073.15) Region_prho = 5; return end else //Check region 1,3,4,3,2 (Above the lowest point of region 3.) if v < v1_pT(p, 273.15) //Observe that this is not actually min of v. Not valid Water of 4°C is ligther. Region_prho = 0; return end if v < v1_pT(p, 623.15) Region_prho = 1; return end //Check if in region 3 or 4 (Bellow Reg 2) if v < v2_pT(p, B23T_p(p)) //Region 3 or 4 if p > 22.064 //Above region 4 Region_prho = 3; return end if v < v3_ph(p, h4L_p(p)) | v > v3_ph(p, h4V_p(p)) //Uses iteration!! Region_prho = 3; return else Region_prho = 4; return end end //Check if region 2 if v < v2_pT(p, 1073.15) Region_prho = 2; return end end Region_prho = 0; //*********************************************************************************************************** //*4 Region Borders //*********************************************************************************************************** //*********************************************************************************************************** //*4.1 Boundary between region 2 and 3. endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function B23p_T = B23p_T(T) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //1997 //Section 4 Auxiliary Equation for the Boundary between Regions 2 and 3 //Eq 5, Page 5 B23p_T = 348.05185628969 - 1.1671859879975 * T + 1.0192970039326E-03 * T ^ 2; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function B23T_p = B23T_p(p) //Release on the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water and Steam //1997 //Section 4 Auxiliary Equation for the Boundary between Regions 2 and 3 //Eq 6, Page 6 B23T_p = 572.54459862746 + ((p - 13.91883977887) / 1.0192970039326E-03) ^ 0.5; //*********************************************************************************************************** //*4.2 Region 3. pSat_h & pSat_s endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function p3sat_h = p3sat_h(h) //Revised Supplementary Release on Backward Equations for the functions T(p,h), v(p,h) & T(p,s), v(p,s) for Region 3 of the IAPWS Industrial formulation 1997 for the Thermodynamic Properties of Water & Steam //2004 //Section 4 Boundary Equations psat(h) & psat(s) for the Saturation Lines of Region 3 //Se pictures Page 17, Eq 10, Table 17, Page 18 Ii = [0, 1, 1, 1, 1, 5, 7, 8, 14, 20, 22, 24, 28, 36]; Ji = [0, 1, 3, 4, 36, 3, 0, 24, 16, 16, 3, 18, 8, 24]; ni = [0.600073641753024, -9.36203654849857, 24.6590798594147, -107.014222858224, -91582131580576.8, -8623.32011700662, -23.5837344740032, 2.52304969384128E+17, -3.89718771997719E+18, -3.33775713645296E+22, 35649946963.6328, -1.48547544720641E+26, 3.30611514838798E+18, 8.13641294467829E+37]; hs = h / 2600; ps = 0; for i = 1:14 ps = ps + ni(i) * (hs - 1.02) ^ Ii(i) * (hs - 0.608) ^ Ji(i); end p3sat_h = ps * 22; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function p3sat_s = p3sat_s(s) Ii = [0, 1, 1, 4, 12, 12, 16, 24, 28, 32]; Ji = [0, 1, 32, 7, 4, 14, 36, 10, 0, 18]; ni = [0.639767553612785, -12.9727445396014, -2.24595125848403E+15, 1774667.41801846, 7170793495.71538, -3.78829107169011E+17, -9.55586736431328E+34, 1.87269814676188E+23, 119254746466.473, 1.10649277244882E+36]; Sigma = s / 5.2; Pi = 0; for i = 1:10 Pi = Pi + ni(i) * (Sigma - 1.03) ^ Ii(i) * (Sigma - 0.699) ^ Ji(i); end p3sat_s = Pi * 22; //*********************************************************************************************************** //4.3 Region boundary 1to3 & 3to2 as a functions of s endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function hB13_s = hB13_s(s) //Supplementary Release on Backward Equations ( ) , p h s for Region 3, //Chapter 4.5 page 23. Ii = [0, 1, 1, 3, 5, 6]; Ji = [0, -2, 2, -12, -4, -3]; ni = [0.913965547600543, -4.30944856041991E-05, 60.3235694765419, 1.17518273082168E-18, 0.220000904781292, -69.0815545851641]; Sigma = s / 3.8; eta = 0; for i = 1 : 6 eta = eta + ni(i) * (Sigma - 0.884) ^ Ii(i) * (Sigma - 0.864) ^ Ji(i); end hB13_s = eta * 1700; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function TB23_hs = TB23_hs(h, s) //Supplementary Release on Backward Equations ( ) , p h s for Region 3, //Chapter 4.6 page 25. Ii = [-12, -10, -8, -4, -3, -2, -2, -2, -2, 0, 1, 1, 1, 3, 3, 5, 6, 6, 8, 8, 8, 12, 12, 14, 14]; Ji = [10, 8, 3, 4, 3, -6, 2, 3, 4, 0, -3, -2, 10, -2, -1, -5, -6, -3, -8, -2, -1, -12, -1, -12, 1]; ni = [6.2909626082981E-04, -8.23453502583165E-04, 5.15446951519474E-08, -1.17565945784945, 3.48519684726192, -5.07837382408313E-12, -2.84637670005479, -2.36092263939673, 6.01492324973779, 1.48039650824546, 3.60075182221907E-04, -1.26700045009952E-02, -1221843.32521413, 0.149276502463272, 0.698733471798484, -2.52207040114321E-02, 1.47151930985213E-02, -1.08618917681849, -9.36875039816322E-04, 81.9877897570217, -182.041861521835, 2.61907376402688E-06, -29162.6417025961, 1.40660774926165E-05, 7832370.62349385]; Sigma = s / 5.3; eta = h / 3000; teta = 0; for i = 1 : 25 teta = teta + ni(i) * (eta - 0.727) ^ Ii(i) * (Sigma - 0.864) ^ Ji(i); end TB23_hs = teta * 900; //*********************************************************************************************************** //*5 Transport properties //*********************************************************************************************************** //*5.1 Viscosity (IAPWS formulation 1985, Revised 2003) //*********************************************************************************************************** endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function my_AllRegions_pT = my_AllRegions_pT( p, T) h0 = [0.5132047, 0.3205656, 0, 0, -0.7782567, 0.1885447]; h1 = [0.2151778, 0.7317883, 1.241044, 1.476783, 0, 0]; h2 = [-0.2818107, -1.070786, -1.263184, 0, 0, 0]; h3 = [0.1778064, 0.460504, 0.2340379, -0.4924179, 0, 0]; h4 = [-0.0417661, 0, 0, 0.1600435, 0, 0]; h5 = [0, -0.01578386, 0, 0, 0, 0]; h6 = [0, 0, 0, -0.003629481, 0, 0]; //Calcualte density. select region_pT(p, T) case 1 rho = 1 / v1_pT(p, T); case 2 rho = 1 / v2_pT(p, T); case 3 hs = h3_pT(p, T); rho = 1 / v3_ph(p, hs); case 4 rho = %nan; case 5 rho = 1 / v5_pT(p, T); else my_AllRegions_pT = %nan; return end rhos = rho / 317.763; Ts = T / 647.226; ps = p / 22.115; //Check valid area if T > 900 + 273.15 | (T > 600 + 273.15 & p > 300) | (T > 150 + 273.15 & p > 350) | p > 500 my_AllRegions_pT = %nan; return end my0 = Ts ^ 0.5 / (1 + 0.978197 / Ts + 0.579829 / (Ts ^ 2) - 0.202354 / (Ts ^ 3)); Sum = 0; for i = 0 : 5 Sum = Sum + h0(i+1) * (1 / Ts - 1) ^ i + h1(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 1 + h2(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 2 + h3(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 3 + h4(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 4 + h5(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 5 + h6(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 6; end my1 = exp(rhos * Sum); mys = my0 * my1; my_AllRegions_pT = mys * 0.000055071; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function my_AllRegions_ph = my_AllRegions_ph( p, h) h0 = [0.5132047, 0.3205656, 0, 0, -0.7782567, 0.1885447]; h1 = [0.2151778, 0.7317883, 1.241044, 1.476783, 0, 0]; h2 = [-0.2818107, -1.070786, -1.263184, 0, 0, 0]; h3 = [0.1778064, 0.460504, 0.2340379, -0.4924179, 0, 0]; h4 = [-0.0417661, 0, 0, 0.1600435, 0, 0]; h5 = [0, -0.01578386, 0, 0, 0, 0]; h6 = [0, 0, 0, -0.003629481, 0, 0]; //Calcualte density. select region_ph(p, h) case 1 Ts = T1_ph(p, h); T = Ts; rho = 1 / v1_pT(p, Ts); case 2 Ts = T2_ph(p, h); T = Ts; rho = 1 / v2_pT(p, Ts); case 3 rho = 1 / v3_ph(p, h); T = T3_ph(p, h); case 4 xs = x4_ph(p, h); if p < 16.529 v4v = v2_pT(p, T4_p(p)); v4L = v1_pT(p, T4_p(p)); else v4v = v3_ph(p, h4V_p(p)); v4L = v3_ph(p, h4L_p(p)); end rho = 1 / (xs * v4v + (1 - xs) * v4L); T = T4_p(p); case 5 Ts = T5_ph(p, h); T = Ts; rho = 1 / v5_pT(p, Ts); else my_AllRegions_ph = %nan; return end rhos = rho / 317.763; Ts = T / 647.226; ps = p / 22.115; //Check valid area if T > 900 + 273.15 | (T > 600 + 273.15 & p > 300) | (T > 150 + 273.15 & p > 350) | p > 500 my_AllRegions_ph = %nan; return end my0 = Ts ^ 0.5 / (1 + 0.978197 / Ts + 0.579829 / (Ts ^ 2) - 0.202354 / (Ts ^ 3)); Sum = 0; for i = 0 : 5 Sum = Sum + h0(i+1) * (1 / Ts - 1) ^ i + h1(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 1 + h2(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 2 + h3(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 3 + h4(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 4 + h5(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 5 + h6(i+1) * (1 / Ts - 1) ^ i * (rhos - 1) ^ 6; end my1 = exp(rhos * Sum); mys = my0 * my1; my_AllRegions_ph = mys * 0.000055071; //*********************************************************************************************************** //*5.2 Thermal Conductivity (IAPWS formulation 1985) endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function tc_ptrho = tc_ptrho( p, T, rho) //Revised release on the IAPWS formulation 1985 for the Thermal Conductivity of ordinary water //IAPWS September 1998 //Page 8 if T < 0 | p < 0.000611657 | T > 800 | p > 400 | ~((p <= 100 & T <= 100 + 273.15) | (p <= 150 & T <= 400 + 273.15) | (p <= 200 & T <= 250 + 273.15) | (p <= 400 & T <= 125 + 273.15)) tc_ptrho = %nan; //'Out of valid region' return end T = T / 647.26; rho = rho / 317.7; tc0 = T ^ 0.5 * (0.0102811 + 0.0299621 * T + 0.0156146 * T ^ 2 - 0.00422464 * T ^ 3); tc1 = -0.39707 + 0.400302 * rho + 1.06 * exp(-0.171587 * (rho + 2.39219) ^ 2); dT = abs(T - 1) + 0.00308976; Q = 2 + 0.0822994 / dT ^ (3 / 5); if T >= 1 s = 1 / dT; else s = 10.0932 / dT ^ (3 / 5); end tc2 = (0.0701309 / T ^ 10 + 0.011852) * rho ^ (9 / 5) * exp(0.642857 * (1 - rho ^ (14 / 5))) + 0.00169937 * s * rho ^ Q * exp((Q / (1 + Q)) * (1 - rho ^ (1 + Q))) - 1.02 * exp(-4.11717 * T ^ (3 / 2) - 6.17937 / rho ^ 5); tc = tc0 + tc1 + tc2; tc_ptrho = tc; //*********************************************************************************************************** //5.3 Surface Tension endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function Surface_Tension_T = Surface_Tension_T( T) //IAPWS Release on Surface Tension of Ordinary Water Substance, //September 1994 tc = 647.096; //K B = 0.2358; //N/m bb = -0.625; my = 1.256; if T < 0.01 | T > tc Surface_Tension_T = %nan; //"Out of valid region" return end tau = 1 - T / tc; Surface_Tension_T = B * tau ^ my * (1 + bb * tau); //*********************************************************************************************************** //*6 Units * //*********************************************************************************************************** endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_p = toSIunit_p( Ins ) //Translate bar to MPa toSIunit_p = Ins / 10; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_p = fromSIunit_p( Ins ) //Translate bar to MPa fromSIunit_p = Ins * 10; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_T = toSIunit_T( Ins ) //Translate degC to Kelvon toSIunit_T = Ins + 273.15; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_T = fromSIunit_T( Ins ) //Translate Kelvin to degC fromSIunit_T = Ins - 273.15; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_h = toSIunit_h( Ins ) toSIunit_h = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_h = fromSIunit_h( Ins ) fromSIunit_h = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_v = toSIunit_v( Ins ) toSIunit_v = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_v = fromSIunit_v( Ins ) fromSIunit_v = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_s = toSIunit_s( Ins ) toSIunit_s = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_s = fromSIunit_s( Ins ) fromSIunit_s = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_u = toSIunit_u( Ins ) toSIunit_u = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_u = fromSIunit_u( Ins ) fromSIunit_u = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_Cp = toSIunit_Cp( Ins ) toSIunit_Cp = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_Cp = fromSIunit_Cp( Ins ) fromSIunit_Cp = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_Cv = toSIunit_Cv( Ins ) toSIunit_Cv = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_Cv = fromSIunit_Cv( Ins ) fromSIunit_Cv = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_w = toSIunit_w( Ins ) toSIunit_w = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_w = fromSIunit_w( Ins ) fromSIunit_w = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_tc = toSIunit_tc( Ins ) toSIunit_tc = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_tc = fromSIunit_tc( Ins ) fromSIunit_tc = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_st = toSIunit_st( Ins ) toSIunit_st = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_st = fromSIunit_st( Ins ) fromSIunit_st = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_x = toSIunit_x( Ins ) toSIunit_x = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_x = fromSIunit_x( Ins ) fromSIunit_x = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_vx = toSIunit_vx( Ins ) toSIunit_vx = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_vx = fromSIunit_vx( Ins ) fromSIunit_vx = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function toSIunit_my = toSIunit_my( Ins ) toSIunit_my = Ins; endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function fromSIunit_my = fromSIunit_my( Ins ) fromSIunit_my = Ins; //*********************************************************************************************************** //*7 Verification * //*********************************************************************************************************** endfunction //---------------------------------------------------------------// // Translated from XSteam.m using m2sci.pl at 21:24 15/8/2006. //---------------------------------------------------------------// function err = check() err=0; //********************************************************************************************************* //* 7.1 Verifiy region 1 //IF-97 Table 5, Page 9 p=[30/10,800/10,30/10]; T=[300,300,500]; Fun={'v1_pT','h1_pT','u1_pT','s1_pT','Cp1_pT','w1_pT'}; IF97=[0.00100215168,0.000971180894,0.001202418;... 115.331273,184.142828,975.542239;... 112.324818,106.448356,971.934985;... 0.392294792,0.368563852,2.58041912;... 4.17301218,4.01008987,4.65580682;... 1507.73921,1634.69054,1240.71337]; R1=zeros(6,3); for i=1:3 for j=1:6 execstr(['R1('+mtlb_num2str(j)+','+mtlb_num2str(i)+')='+Fun(j)+'('+mtlb_num2str(p(i))+','+mtlb_num2str(T(i))+');']); end end Region1_error=abs((R1-IF97) ./ IF97) err=err+sum(sum(Region1_error>1E-8)) //IF-97 Table 7, Page 11 p=[30/10,800/10,800/10]; h=[500,500,1500]; IF97=[391.798509,378.108626,611.041229]; R1=zeros(1,3); for i=1:3 R1(i)=T1_ph(p(i),h(i)); end T1_ph_error=abs((R1-IF97) ./ IF97) err=err+sum(sum(T1_ph_error>1E-8)) //IF-97 Table 9, Page 12 p=[30/10,800/10,800/10]; s=[0.5,0.5,3]; IF97=[307.842258,309.979785,565.899909]; R1=zeros(1,3); for i=1:3 R1(i)=T1_ps(p(i),s(i)); end T1_ps_error=abs((R1-IF97) ./ IF97) err=err+sum(sum(T1_ps_error>1E-8)) //Supplementary Release on Backward Equations //for Pressure as a Function of Enthalpy and Entropy p(h,s) //Table 3, Page 6 h=[0.001,90,1500]; s=[0,0,3.4]; IF97=[0.0009800980612,91.929547272,58.68294423]; R1=zeros(1,3); for i=1:3 R1(i)=p1_hs(h(i),s(i)); end p1_hs_error=abs((R1-IF97) ./ IF97) err=err+sum(sum(p1_hs_error>1E-8)) //********************************************************************************************************* //* 7.2 Verifiy region 2 // IF-97 Table 15, Page 17 p=[0.035/10,0.035/10,300/10]; T=[300,700,700]; Fun={'v2_pT','h2_pT','u2_pT','s2_pT','Cp2_pT','w2_pT'}; IF97=[39.4913866,92.3015898,0.00542946619;... 2549.91145,3335.68375,2631.49474;... 2411.6916,3012.62819,2468.61076;... 8.52238967,10.1749996,5.17540298;... 1.91300162,2.08141274,10.3505092;... 427.920172,644.289068,480.386523]; R2=zeros(6,3); for i=1:3 for j=1:6 // R2(j,i)=execstr([ascii(Fun(j)),'(',mtlb_num2str(p(i)),',',mtlb_num2str(T(i)),');']); execstr(['R2('+string(j)+','+string(i)+')='+Fun(j)+'('+mtlb_num2str(p(i))+','+mtlb_num2str(T(i))+');']); end end Region2_error=abs((R2-IF97) ./ IF97) err=err+sum(sum(Region2_error>1E-8)) //IF-97 Table 24, Page 25 p=[0.01/10,30/10,30/10,50/10,50/10,250/10,400/10,600/10,600/10]; h=[3000,3000,4000,3500,4000,3500,2700,2700,3200]; IF97=[534.433241,575.37337,1010.77577,801.299102,1015.31583,875.279054,743.056411,791.137067,882.75686]; R2=zeros(1,9); for i=1:9 R2(i)=T2_ph(p(i),h(i)); end T2_ph_error=abs((R2-IF97) ./ IF97) err=err+sum(sum(T2_ph_error>1E-8)) //IF-97 Table 29, Page 29 p=[1/10,1/10,25/10,80/10,80/10,900/10,200/10,800/10,800/10]; s=[7.5,8,8,6,7.5,6,5.75,5.25,5.75]; IF97=[399.517097,514.127081,1039.84917,600.48404,1064.95556,1038.01126,697.992849,854.011484,949.017998]; R2=zeros(1,9); for i=1:9 R2(i)=T2_ps(p(i),s(i)); end T2_ps_error=abs((R2-IF97) ./ IF97) err=err+sum(sum(T2_ps_error>1E-8)) //Supplementary Release on Backward Equations for Pressure as a Function of Enthalpy and Entropy p(h,s) //Table 3, Page 6 h=[2800,2800,4100,2800,3600,3600,2800,2800,3400]; s=[6.5,9.5,9.5,6,6,7,5.1,5.8,5.8]; IF97=[1.371012767,0.001879743844,0.1024788997,4.793911442,83.95519209,7.527161441,94.3920206,8.414574124,83.76903879]; R2=zeros(1,9); for i=1:9 R2(i)=p2_hs(h(i),s(i)); end p2_hs_error=abs((R2-IF97) ./ IF97) err=err+sum(sum(p2_hs_error>1E-8)) //********************************************************************************************************* //* 7.3 Verifiy region 3 // IF-97 Table 33, Page 32 T=[650,650,750]; rho=[500,200,500]; Fun={'p3_rhoT','h3_rhoT','u3_rhoT','s3_rhoT','Cp3_rhoT','w3_rhoT'}; IF97=[25.5837018,22.2930643,78.3095639;... 1863.43019,2375.12401,2258.68845;... 1812.26279,2263.65868,2102.06932;... 4.05427273,4.85438792,4.46971906;... 13.8935717,44.6579342,6.34165359;... 502.005554,383.444594,760.696041]; R3=zeros(6,3); for i=1:3 for j=1:6 // R3(j,i)=execstr([ascii(Fun(j)),'(',mtlb_num2str(rho(i)),',',mtlb_num2str(T(i)),');']); R3(j,i)=evstr([Fun(j)+'('+mtlb_num2str(rho(i))+','+mtlb_num2str(T(i))+');']); end end Region3_error=abs((R3-IF97) ./ IF97) err=err+sum(sum(Region3_error>1E-8)) //T3_ph p=[200/10,500/10,1000/10,200/10,500/10,1000/10]; h=[1700,2000,2100,2500,2400,2700]; IF97=[629.3083892,690.5718338,733.6163014,641.8418053,735.1848618,842.0460876]; R3=zeros(1,6); for i=1:6 R3(i)=T3_ph(p(i),h(i)); end T3_ph_error=abs((R3-IF97) ./ IF97) err=err+sum(sum(T3_ph_error>1E-8)) //v3_ph p=[200/10,500/10,1000/10,200/10,500/10,1000/10]; h=[1700,2000,2100,2500,2400,2700]; IF97=[0.001749903962,0.001908139035,0.001676229776,0.006670547043,0.0028012445,0.002404234998]; R3=zeros(1,6); for i=1:6 R3(i)=v3_ph(p(i),h(i)); end v3_ph_error=abs((R3-IF97) ./ IF97) err=err+sum(sum(v3_ph_error>1E-7)) //T3_ps p=[200/10,500/10,1000/10,200/10,500/10,1000/10]; s=[3.7,3.5,4,5,4.5,5]; IF97=[620.8841563,618.1549029,705.6880237,640.1176443,716.3687517,847.4332825]; R3=zeros(1,6); for i=1:6 R3(i)=T3_ps(p(i),s(i)); end T3_ps_error=abs((R3-IF97) ./ IF97) err=err+sum(sum(T3_ps_error>1E-8)) //v3_ps p=[200/10,500/10,1000/10,200/10,500/10,1000/10]; s=[3.7,3.5,4,5,4.5,5]; IF97=[0.001639890984,0.001423030205,0.001555893131,0.006262101987,0.002332634294,0.002449610757]; R3=zeros(1,6); for i=1:6 R3(i)=v3_ps(p(i),s(i)); end v3_ps_error=abs((R3-IF97) ./ IF97) err=err+sum(sum(v3_ps_error>1E-8)) //p3_hs h=[1700,2000,2100,2500,2400,2700]; s=[3.8,4.2,4.3,5.1,4.7,5]; IF97=[25.55703246,45.40873468,60.7812334,17.20612413,63.63924887,88.39043281]; R3=zeros(1,6); for i=1:6 R3(i)=p3_hs(h(i),s(i)); end p3_hs_error=abs((R3-IF97) ./ IF97) err=err+sum(sum(p3_hs_error>1E-8)) //h3_pT (Iteration) p=[255.83702,222.93064,783.09564] ./ 10; T=[650,650,750]; IF97=[1863.271389,2375.696155,2258.626582]; R3=zeros(1,3); for i=1:3 R3(i)=h3_pT(p(i),T(i)); end h3_pT_error=abs((R3-IF97) ./ IF97) err=err+sum(sum(h3_pT_error>1E-6)) //Decimals in IF97 //********************************************************************************************************* //* 7.4 Verifiy region 4 //Saturation pressure, If97, Table 35, Page 34 T=[300,500,600]; IF97=[0.0353658941, 26.3889776, 123.443146]/10; R4=zeros(1,3); for i=1:3 R4(i)=p4_T(T(i)); end p4_t_error=abs((R4-IF97) ./ IF97) err=err+sum(sum( p4_t_error>1E-7)) T=[1,10,100]/10; IF97=[372.755919,453.035632,584.149488]; R4=zeros(1,3); for i=1:3 R4(i)=T4_p(T(i)); end T4_p_error=abs((R4-IF97) ./ IF97) err=err+sum(sum( T4_p_error>1E-7)) s=[1,2,3,3.8,4,4.2,7,8,9,5.5,5,4.5]; IF97=[308.5509647,700.6304472,1198.359754,1685.025565,1816.891476,1949.352563,2723.729985,2599.04721,2511.861477,2687.69385,2451.623609,2144.360448]; R4=zeros(1,12); for i=1:12 R4(i)=h4_s(s(i)); end h4_s_error=abs((R4-IF97) ./ IF97) err=err+sum(sum( h4_s_error>1E-7)) //********************************************************************************************************* //* 7.5 Verifiy region 5 // IF-97 Table 42, Page 39 T=[1500,1500,2000]; p=[5,80,80]/10; Fun={'v5_pT','h5_pT','u5_pT','s5_pT','Cp5_pT','w5_pT'}; IF97=[1.38455354,0.0865156616,0.115743146;... 5219.76332,5206.09634,6583.80291;... 4527.48654,4513.97105,5657.85774;... 9.65408431,8.36546724,9.15671044;... 2.61610228,2.64453866,2.8530675;... 917.071933,919.708859,1054.35806]; R5=zeros(6,3); for i=1:3 for j=1:6 // R5(j,i)=execstr([ascii(Fun(j)),'(',mtlb_num2str(p(i)),',',mtlb_num2str(T(i)),');']); execstr(['R5('+string(j)+','+string(i)+')='+Fun(j)+'('+mtlb_num2str(p(i))+','+mtlb_num2str(T(i))+');']); end end Region5_error=abs((R5-IF97) ./ IF97) err=err+sum(sum(Region5_error>1E-8)) //T5_ph (Iteration) p=[0.5,8,8]; h=[5219.76331549428,5206.09634477373,6583.80290533381]; IF97=[1500,1500,2000]; R5=zeros(1,3); for i=1:3 R5(i)=T5_ph(p(i),h(i)); end T5_ph_error=abs((R5-IF97) ./ IF97) err=err+sum(sum(T5_ph_error>1E-7)) //Decimals in IF97 //T5_ps (Iteration) p=[0.5,8,8]; s=[9.65408430982588,8.36546724495503,9.15671044273249]; IF97=[1500,1500,2000]; R5=zeros(1,3); for i=1:3 R5(i)=T5_ps(p(i),s(i)); end T5_ps_error=abs((R5-IF97) ./ IF97) err=err+sum(sum(T5_ps_error>1E-4)) //Decimals in IF97 //********************************************************************************************************* //* 7.6 Verifiy calling funtions fun={'Tsat_p','T_ph','T_ps','T_hs','psat_T','p_hs','hV_p','hL_p','hV_T','hL_T','h_pT','h_ps','h_px','h_prho','h_Tx','vV_p','vL_p','vV_T','vL_T','v_pT','v_ph','v_ps','rhoV_p','rhoL_p','rhoV_T','rhoL_T','rho_pT','rho_ph','rho_ps','sV_p','sL_p','sV_T','sL_T','s_pT','s_ph','uV_p','uL_p','uV_T','uL_T','u_pT','u_ph','u_ps','CpV_p','CpL_p','CpV_T','CpL_T','Cp_pT','Cp_ph','Cp_ps','CvV_p','CvL_p','CvV_T','CvL_T','Cv_pT','Cv_ph','Cv_ps','wV_p','wL_p','wV_T','wL_T','w_pT','w_ph','w_ps','my_pT','my_ph','my_ps','tcL_p','tcV_p','tcL_T','tcV_T','tc_pT','tc_ph','tc_hs','st_T','st_p','x_ph','x_ps','vx_ph','vx_ps'}; In1={'1','1','1','100','100','84','1','1','100','100','1','1','1','1','100','1','1','100','100','1','1','1','1','1','100','100','1','1','1','0.006117','0.0061171','0.0001','100','1','1','1','1','100','100','1','1','1','1','1','100','100','1','1','1','1','1','100','100','1','1','1','1','1','100','100','1','1','1','1','1','1','1','1','25','25','1','1','100','100','1','1','1','1','1'}; In2={'0','100','1','0.2','0','0.296','0','0','0','0','20','1','0.5','2','0.5','0','0','0','0','100','1000','5','0','0','0','0','100','1000','1','0','0','0','0','20','84.01181117','0','0','0','0','100','1000','1','0','0','0','0','100','200','1','0','0','0','0','100','200','1','0','0','0','0','100','200','1','100','1000','1','0','0','0','0','25','100','0.34','0','0','1000','4','418','4'}; Control={'99.60591861','23.84481908','73.70859421','13.84933511','1.014179779','2.295498269','2674.949641','417.4364858','2675.572029','419.099155','84.01181117','308.6107171','1546.193063','1082.773391','1547.33559210927','1.694022523','0.001043148','1.671860601','0.001043455','1.695959407','0.437925658','1.03463539','0.590310924','958.6368897','0.598135993','958.3542773','0.589636754','2.283492601','975.6236788','9.155465556','1.8359E-05','9.155756716','1.307014328','0.296482921','0.296813845','2505.547389','417.332171','2506.015308','418.9933299','2506.171426','956.2074342','308.5082185','2.075938025','4.216149431','2.077491868','4.216645119','2.074108555','4.205574175','4.190607038','1.552696979','3.769699683','1.553698696','3.76770022','1.551397249','4.035176364','3.902919468','472.0541571','1545.451948','472.2559492','1545.092249','472.3375235','1542.682475','1557.8585','1.22704E-05','1.20252E-05','0.000384222','0.677593822','0.024753668','0.607458162','0.018326723','0.607509806','0.605710062','0.606283124','0.0589118685876641','0.058987784','0.258055424','0.445397961','0.288493093','0.999233827'}; for i=1:max(size(fun)), T=['XSteam('''+fun(i)+''','+In1(i)+','+In2(i)+')']; Res=evstr(T); Error=(Res-(evstr(Control(i))))/evstr(Control(i)); Check=[T+'='+mtlb_num2str(Res)+' - (Control)'+Control(i)+'='+mtlb_num2str(Error)]; disp(Check) if Error>1E-5 err=err+1; disp(['To large error :'+fun(i)+' Error = '+mtlb_num2str(Error)]); pause end end endfunction