WaterSteamPro functions

    WaterSteamPro

    Common functions which is recommended to use.

  1. Surface tension [lbf/ft] as function of temperature t [degF]:

    wsuSURFTENT (t)

    Based upon the IAPWS Release on The Surface Tension of Ordinary Water Substance 1995.

  2. Specific volume [ft3/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuVPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA2 is used for the determining of area. After that the necessary function (wsuVxPT) is used.

  3. Specific internal energy [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuUPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA2 is used for the determining of area. After that the necessary function (wsuUxPT) is used.

  4. Specific entropy [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuSPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA2 is used for the determining of area. After that the necessary function (wsuSxPT) is used.

  5. Specific enthalpy [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuHPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA2 is used for the determining of area. After that the necessary function (wsuHxPT) is used.

  6. Specific heat capacity at constant pressure (Cp) [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCPPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA2 is used for the determining of area. After that the necessary function (wsuCPxPT) is used.

  7. Specific heat capacity at constant volume (Cv) [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCVPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA2 is used for the determining of area. After that the necessary function (wsuCVxPT) is used.

  8. Sound velocity [ft/sec] as function of pressure p [psi], temperature t [degF]:

    wsuWPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA2 is used for the determining of area. After that the necessary function (wsuWxPT) is used.

  9. Thermal conduction [BTU/(hour·ft·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuTHERMCONDPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. For calculation used the function wsuTHERMCONDRT with density from the common function wsuVPT.

  10. Dynamic viscosity [(lbf·sec)/ft2] as function of pressure p [psi], temperature t [degF]:

    wsuDYNVISPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. For calculation used the function wsuDYNVISRT with density from the common function wsuVPT.

  11. Prandtl number as function of pressure p [psi], temperature t [degF]:

    wsuPRANDTLEPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. For calculation used the formula: Pr = DYNVIS · CP / THERMCOND, where DYNVIS calculated via the function wsuDYNVISPT, CP - via wsuCPPT and THERMCOND - via wsuTHERMCONDPT.

  12. Kinematic viscosity [ft2/sec] as function of pressure p [psi], temperature t [degF]:

    wsuKINVISPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. For calculation used the formula: KINVIS = DYNVIS · V, where DYNVIS calculated via the function wsuDYNVISPT and V - via wsuVPT.

  13. Isoentropic exponent as function of pressure p [psi], temperature t [degF]:

    wsuKPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. For calculation used the formula: K = W · W / (P · V), where W (sound velocity) calculated via the function wsuWPT, P - pressure and V (specific volume) - via wsuVPT.

  14. Joule-Thompson coefficient [degF/psi] as function of pressure p [psi], temperature t [degF]:

    wsuJOULETHOMPSONPT (p, t)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA2 is used for the determining of area. After that the necessary function (wsuJOULETHOMPSONxPT) is used.

  15. Specific volume [ft3/lbm] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuVPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuVxPT or wsuVSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  16. Specific internal energy [BTU/lbm] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuUPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuUxPT or wsuUSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  17. Specific entropy [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuSPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuSxPT or wsuSSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  18. Specific enthalpy [BTU/lbm] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuHPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuHxPT or wsuHSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  19. Specific heat capacity at constant pressure (Cp) [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuCPPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuCPxPT or wsuCPSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  20. Specific heat capacity at constant volume (Cv) [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuCVPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuCVxPT or wsuCVSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  21. Sound velocity [ft/sec] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuWPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuWxPT or wsuWSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  22. Thermal conduction [BTU/(hour·ft·degF)] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuTHERMCONDPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuTHERMCONDPT or wsuTHERMCONDSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  23. Dynamic viscosity [(lbf·sec)/ft2] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuDYNVISPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuDYNVISPT or wsuDYNVISSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  24. Prandtl number as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuPRANDTLEPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuPRANDTLEPPT or wsuPRANDTLEPSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  25. Kinematic viscosity [ft2/sec] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuKINVISPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuKINVISPT or wsuKINVISSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  26. Isoentropic exponent as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuKPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuKPT or wsuKSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  27. Joule-Thompson coefficient [degF/psi] as function of pressure p [psi], temperature t [degF], degree of dryness x []:

    wsuJOULETHOMPSONPTX (p, t, x)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREA is used for the determining of area. After that the necessary function (wsuJOULETHOMPSONPT or wsuJOULETHOMPSONSTX) is used. If the area is not the double-phase area than the degree of dryness is ignored.

  28. Temperature [degF] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuTPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used.

  29. Temperature [degF] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuTPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPS) is used.

  30. Specific internal energy [BTU/lbm] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuUPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuUxPT or wsuUSTX).

  31. Specific volume [ft3/lbm] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuVPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuVxPT or wsuVSTX).

  32. Specific entropy [BTU/(lbm·degF)] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuSPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuSxPT or wsuSSTX).

  33. Specific heat capacity at constant pressure (Cp) [BTU/(lbm·degF)] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuCPPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuCPxPT or wsuCPSTX).

  34. Specific heat capacity at constant volume (Cv) [BTU/(lbm·degF)] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuCVPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuCVxPT or wsuCVSTX).

  35. Sound velocity [ft/sec] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuWPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuWxPT or wsuWSTX).

  36. Dynamic viscosity [(lbf·sec)/ft2] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuDYNVISPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuDYNVISPT or wsuDYNVISSTX).

  37. Kinematic viscosity [ft2/sec] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuKINVISPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuKINVISPT or wsuKINVISSTX).

  38. Prandtl number as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuPRANDTLEPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuPRANDTLEPT or wsuPRANDTLESTX).

  39. Thermal conduction [BTU/(hour·ft·degF)] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuTHERMCONDPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuTHERMCONDPT or wsuTHERMCONDSTX).

  40. Isoentropic exponent as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuKPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuKPT or wsuKSTX).

  41. Joule-Thompson coefficient [degF/psi] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuJOULETHOMPSONPH (p, h)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPH) is used. And the final step is calling the necessary function (wsuJOULETHOMPSONPT or wsuJOULETHOMPSONSTX).

  42. Specific internal energy [BTU/lbm] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuUPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuUxPT or wsuUSTX).

  43. Specific volume [ft3/lbm] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuVPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuVxPT or wsuVSTX).

  44. Specific enthalpy [BTU/lbm] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuHPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuHxPT or wsuHSTX).

  45. Specific heat capacity at constant pressure (Cp) [BTU/(lbm·degF)] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuCPPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuCPxPT or wsuCPSTX).

  46. Specific heat capacity at constant volume (Cv) [BTU/(lbm·degF)] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuCVPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuCVxPT or wsuCVSTX).

  47. Sound velocity [ft/sec] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuWPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuWxPT or wsuWSTX).

  48. Dynamic viscosity [(lbf·sec)/ft2] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuDYNVISPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuDYNVISPT or wsuDYNVISSTX).

  49. Kinematic viscosity [ft2/sec] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuKINVISPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuKINVISPT or wsuKINVISSTX).

  50. Prandtl number as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuPRANDTLEPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuPRANDTLEPT or wsuPRANDLTESTX).

  51. Isoentropic exponent as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuKPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuKPT or wsuKSTX).

  52. Thermal conduction [BTU/(hour·ft·degF)] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuTHERMCONDPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPS is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuTHERMCONDPT or wsuTHERMCONDSTX).

  53. Joule-Thompson coefficient [degF/psi] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuJOULETHOMPSONPS (p, s)

    This is the common function. The arguments lies in all IF-97 parameters range. The function wsuWATERSTATEAREAPH is used for the determining of area. After that the necessary function (wsuTxPS) is used. And the final step is calling the necessary function (wsuJOULETHOMPSONPT or wsuJOULETHOMPSONSTX).

  54. Temperature [degF] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuTEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  55. Specific volume [ft3/lbm] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuVEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  56. Specific internal energy [BTU/lbm] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuUEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  57. Specific enthalpy [BTU/lbm] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuHEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  58. Specific entropy [BTU/(lbm·degF)] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuSEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  59. Specific heat capacity at constant pressure (Cp) [BTU/(lbm·degF)] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuCPEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  60. Specific heat capacity at constant volume (Cv) [BTU/(lbm·degF)] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuCVEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  61. Sound velocity [ft/sec] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuWEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  62. Thermal conduction [BTU/(hour·ft·degF)] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuTHERMCONDEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  63. Kinematic viscosity [ft2/sec] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuKINVISEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  64. Dynamic viscocity [(lbf·sec)/ft2] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuDYNVISEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  65. Prandtl number as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuPRANDTLEEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  66. Isoentropic coefficient as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuKEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  67. Joule-Thompson coefficient [degF/psi] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuJOULETHOMPSONEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  68. Temperature [degF] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuTEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  69. Specific volume [ft3/lbm] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuVEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  70. Specific internal energy [BTU/lbm] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuUEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  71. Specific enthalpy [BTU/lbm] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuHEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  72. Specific entropy [BTU/(lbm·degF)] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuSEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  73. Specific heat capacity at constant pressure (Cp) [BTU/(lbm·degF)] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuCPEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  74. Specific heat capacity at constant volume (Cv) [BTU/(lbm·degF)] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuCVEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  75. Sound velocity [ft/sec] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuWEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  76. Thermal conduction [BTU/(hour·ft·degF)] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuTHERMCONDEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  77. Kinematic viscosity [ft2/sec] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuKINVISEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  78. Dynamic viscocity [(lbf·sec)/ft2] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuDYNVISEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  79. Prandtl number as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuPRANDTLEEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  80. Isoentropic coefficient as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuKEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  81. Joule-Thompson coefficient [degF/psi] as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuJOULETHOMPSONEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff). Note: In ActiveX object "WSP.WSPCalculator" this function named as "wsuJOULETHOMPSONEXPANSIONPTXPEF" due to limitation in function name length in COM.

  82. Degree of dryness as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], degree of dryness in initial point x0 [], pressure in final point p1 [psi], internal efficiency eff []:

    wsuXEXPANSIONPTXPEFF (p0, t0, x0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, x0 to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  83. Degree of dryness as function of pressure in initial point p0 [psi], temperature in initial point t0 [degF], pressure in final point p1 [psi], internal efficiency eff []:

    wsuXEXPANSIONPTPEFF (p0, t0, p1, eff)

    This is the common function. Function return the value in the end of the expansion process from the initial point with arguments p0, t0, to pressure p1 with efficiency eff. Process calculate with next formula: h1 = h0 - eff * (h0 - h1isoent), where h0 - specific enthalpy in initial point, h1 - specific enthalpy in final point of the expansion, eff - efficiency, h1isoentr - specific enthalpy in final point with isoentropic expansion (s = Const). For the calculating the process of compression you must to use instead the efficiency eff the inverse number (i.e. 1/eff).

  84. WaterSteamPro (Source)

    Functions from IAPWS IF-97 and other formulations.

  85. Pressure at line between areas 2 and 3 [psi] as function of temperature t [degF]:

    wsuP23T (t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam. Used in function wsuWATERSTATEAREA when area is determined.

  86. Temperature at line between areas 2 and 3 [degF] as function of pressure p [psi]:

    wsuT23P (p)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam. Used in function wsuWATERSTATEAREA when area is determined.

  87. Water state area as function of pressure p [psi], temperature t [degF]:

    wsuWATERSTATEAREA (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam areas allocation for determining area. Used in common functions.

    Note: Function result has type "long".

  88. Water state area (version 2) as function of pressure p [psi], temperature t [degF]:

    wsuWATERSTATEAREA2 (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam areas allocation for determining area (version 2 - without area 4 - saturation line). Used in common functions.

    Note: Function result has type "long".

  89. Thermal conduction [BTU/(hour·ft·degF)] as function of density r [lbm/ft3], temperature t [degF]:

    wsuTHERMCONDRT (r, t)

    Based upon the IAPWS Formulation 1985 for thermal Conductivity with ITS-90 (International Temperature Scale) correction.

  90. Dynamic viscosity [(lbf·sec)/ft2] as function of density r [lbm/ft3], temperature t [degF]:

    wsuDYNVISRT (r, t)

    Based upon the IAPWS Formulation 1985 for the Viscosity of Ordinary Water Substance with ITS-90 (International Temperature Scale) correction.

  91. Specific volume in area 1 [ft3/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuV1PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  92. Specific internal energy in area 1 [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuU1PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  93. Specific entropy in area 1 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuS1PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  94. Specific enthalpy in area 1 [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuH1PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  95. Specific heat capacity at constant pressure (Cp) in area 1 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCP1PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  96. Specific heat capacity at constant volume (Cv) in area 1 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCV1PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  97. Sound velocity in area 1 [ft/sec] as function of pressure p [psi], temperature t [degF]:

    wsuW1PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  98. Joule-Thompson coefficient in area 1 [degF/psi] as function of pressure p [psi], temperature t [degF]:

    wsuJOULETHOMPSON1PT (p, t)

    Function use the formula: JT = (T*dV/dT - V)/Cp, where T - temperature, dV/dT - differential quotient (dV/dT)p, V - volume, Cp - isobaric heat capacity (Cp).

  99. Specific volume in area 2 [ft3/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuV2PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  100. Specific internal energy in area 2 [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuU2PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  101. Specific entropy in area 2 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuS2PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  102. Specific enthalpy in area 2 [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuH2PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  103. Specific heat capacity at constant pressure (Cp) in area 2 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCP2PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  104. Specific heat capacity at constant volume (Cv) in area 2 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCV2PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  105. Sound velocity in area 2 [ft/sec] as function of pressure p [psi], temperature t [degF]:

    wsuW2PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  106. Joule-Thompson coefficient in area 2 [degF/psi] as function of pressure p [psi], temperature t [degF]:

    wsuJOULETHOMPSON2PT (p, t)

    Function use the formula: JT = (T*dV/dT - V)/Cp, where T - temperature, dV/dT - differential quotient (dV/dT)p, V - volume, Cp - isobaric heat capacity (Cp).

  107. Pressure in area 3 [psi] as function of density r [lbm/ft3], temperature t [degF]:

    wsuP3RT (r, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  108. Density in area 3 [lbm/ft3] as function of density r [lbm/ft3], temperature t [degF], initial density r0 [lbm/ft3]:

    wsuR3PTR0 (r, t, r0)

    Use Newton method with initial value to determine the density from p and t. Used for unification of calculation properties in all IF-97 areas.

  109. Density in area 3 [lbm/ft3] as function of pressure p [psi], temperature t [degF]:

    wsuR3PT (p, t)

    Calculate the density in area 3 with function wsuR3PTR0 with the corresponding initial values for water and steam. Used for unification of calculation properties in all IF-97 areas.

  110. Specific internal energy in area 3 [BTU/lbm] as function of density r [lbm/ft3], temperature t [degF]:

    wsuU3RT (r, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  111. Specific entropy in area 3 [BTU/(lbm·degF)] as function of density r [lbm/ft3], temperature t [degF]:

    wsuS3RT (r, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  112. Specific enthalpy in area 3 [BTU/lbm] as function of density r [lbm/ft3], temperature t [degF]:

    wsuH3RT (r, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  113. Specific heat capacity at constant pressure (Cp) in area 3 [BTU/(lbm·degF)] as function of density r [lbm/ft3], temperature t [degF]:

    wsuCP3RT (r, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  114. Specific heat capacity at constant volume (Cv) in area 3 [BTU/(lbm·degF)] as function of density r [lbm/ft3], temperature t [degF]:

    wsuCV3RT (r, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  115. Sound velocity in area 3 [ft/sec] as function of density r [lbm/ft3], temperature t [degF]:

    wsuW3RT (r, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  116. Specific volume in area 3 [ft3/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuV3PT (p, t)

    Based upon function wsuR3PT.

  117. Specific internal energy in area 3 [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuU3PT (p, t)

    Based upon functions wsuR3PT and wsuU3RT.

  118. Specific entropy in area 3 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuS3PT (p, t)

    Based upon functions wsuR3PT and wsuS3RT.

  119. Specific enthalpy in area 3 [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuH3PT (p, t)

    Based upon functions wsuR3PT and wsuH3RT.

  120. Specific heat capacity at constant pressure (Cp) in area 3 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCP3PT (p, t)

    Based upon functions wsuR3PT and wsuCP3RT.

  121. Specific heat capacity at constant volume (Cv) in area 3 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCV3PT (p, t)

    Based upon functions wsuR3PT and wsuCV3RT.

  122. Sound velocity in area 3 [ft/sec] as function of pressure p [psi], temperature t [degF]:

    wsuW3PT (p, t)

    Based upon functions wsuR3PT and wsuW3RT.

  123. Joule-Thompson coefficient in area 3 [degF/psi] as function of density r [lbm/ft3], temperature t [degF]:

    wsuJOULETHOMPSON3RT (r, t)

    Calculate the Joule-Thompson coefficient for area 3 of IF-97 Formulation.

  124. Joule-Thompson coefficient in area 3 [degF/psi] as function of pressure p [psi], temperature t [degF]:

    wsuJOULETHOMPSON3PT (p, t)

    Calculate the Joule-Thompson coefficient for area 3 of IF-97 Formulation. This function use for the first function wsuR3PT(p, t) for calculating density and after return the value from the function wsuJOULETHOMPSON3RT(r, t).

  125. Specific volume in area 5 [ft3/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuV5PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  126. Specific internal energy in area 5 [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuU5PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  127. Specific entropy in area 5 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuS5PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  128. Specific enthalpy in area 5 [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuH5PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  129. Specific heat capacity at constant pressure (Cp) in area 5 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCP5PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  130. Specific heat capacity at constant volume (Cv) in area 5 [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCV5PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  131. Sound velocity in area 5 [ft/sec] as function of pressure p [psi], temperature t [degF]:

    wsuW5PT (p, t)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  132. Temperature in area 1 [degF] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuT1PH (p, h)

    Based upon the Additional Formulations for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  133. Joule-Thompson coefficient in area 5 [degF/psi] as function of pressure p [psi], temperature t [degF]:

    wsuJOULETHOMPSON5PT (p, t)

    Function use the formula: JT = (T*dV/dT - V)/Cp, where T - temperature, dV/dT - differential quotient (dV/dT)p, V - volume, Cp - isobaric heat capacity (Cp).

  134. Temperature in area 1 [degF] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuT1PS (p, s)

    Based upon the Additional Formulations for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  135. Temperature in area 2a [degF] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuT2APH (p, h)

    Based upon the Additional Formulations for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  136. Temperature in area 2a [degF] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuT2APS (p, s)

    Based upon the Additional Formulations for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  137. Temperature in area 2b [degF] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuT2BPH (p, h)

    Based upon the Additional Formulations for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  138. Temperature in area 2b [degF] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuT2BPS (p, s)

    Based upon the Additional Formulations for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  139. Temperature in area 2c [degF] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuT2CPH (p, h)

    Based upon the Additional Formulations for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  140. Temperature in area 2c [degF] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuT2CPS (p, s)

    Based upon the Additional Formulations for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  141. Temperature in area 2 [degF] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuT2PH (p, h)

    Based upon functions wsuT2APH, wsuT2BPH and wsuT2CPH.

  142. Temperature in area 2 [degF] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuT2PS (p, s)

    Based upon functions wsuT2APS, wsuT2BPS and wsuT2CPS.

  143. Temperature in area 3 [degF] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuT3PH (p, h)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam. The function use the Newton method for determine the root of function with two arguments.

  144. Temperature in area 3 [degF] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuT3PS (p, s)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam. The function use the Newton method for determine the root of function with two arguments.

  145. Temperature in area 5 [degF] as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuT5PH (p, h)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam. The function use the Newton method for determine the root of function with two arguments.

  146. Temperature in area 5 [degF] as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuT5PS (p, s)

    Based upon the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam. The function use the Newton method for determine the root of function with two arguments.

  147. Pressure at line between areas 2b and 2c [psi] as function of specific enthalpy h [BTU/lbm]:

    wsuP2B2CH (h)

    Based upon the Additional Formulation for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  148. Specific enthalpy at line between areas 2b and 2c [BTU/lbm] as function of pressure p [psi]:

    wsuH2B2CP (p)

    Based upon the Additional Formulation for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam.

  149. Water State Area as function of pressure p [psi], specific enthalpy h [BTU/lbm]:

    wsuWATERSTATEAREAPH (p, h)

    Based upon the Additional Formulation for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam areas allocation for determining area. Used in common functions.

    Note: Function result has type "long".

  150. Water State Area as function of pressure p [psi], specific entropy s [BTU/(lbm·degF)]:

    wsuWATERSTATEAREAPS (p, s)

    Based upon the Additional Formulation for the IAPWS Industrial Formulation 1997 for thermodynamic Properties of Water and Steam areas allocation for determining area. Used in common functions.

    Note: Function result has type "long".

  151. WaterSteamPro (Saturation Line)

    Functions of properties at saturation line.

  152. Pressure at saturation line [psi] as function of temperature t [degF]:

    wsuPST (t)

    Based upon the Supplementary Release on Saturation Properties of Ordinary Water Substance from IAPWS.

  153. Temperature at saturation line [degF] as function of pressure p [psi]:

    wsuTSP (p)

    Based upon the Supplementary Release on Saturation Properties of Ordinary Water Substance from IAPWS.

  154. Specific volume of steam at saturation line [ft3/lbm] as function of temperature t [degF]:

    wsuVSST (t)

  155. Specific volume of water at saturation line [ft3/lbm] as function of temperature t [degF]:

    wsuVSWT (t)

  156. Specific internal energy of steam at saturation line [BTU/lbm] as function of temperature t [degF]:

    wsuUSST (t)

  157. Specific internal energy of water at saturation line [BTU/lbm] as function of temperature t [degF]:

    wsuUSWT (t)

  158. Specific entropy of steam at saturation line [BTU/(lbm·degF)] as function of temperature t [degF]:

    wsuSSST (t)

  159. Specific entropy of water at saturation line [BTU/(lbm·degF)] as function of temperature t [degF]:

    wsuSSWT (t)

  160. Specific enthalpy of steam at saturation line [BTU/lbm] as function of temperature t [degF]:

    wsuHSST (t)

  161. Specific enthalpy of water at saturation line [BTU/lbm] as function of temperature t [degF]:

    wsuHSWT (t)

  162. Specific heat capacity at constant pressure (Cp) of steam at saturation line [BTU/(lbm·degF)] as function of temperature t [degF]:

    wsuCPSST (t)

  163. Specific heat capacity at constant pressure (Cp) of water at saturation line [BTU/(lbm·degF)] as function of temperature t [degF]:

    wsuCPSWT (t)

  164. Specific heat capacity at constant volume (Cv) of steam at saturation line [BTU/(lbm·degF)] as function of temperature t [degF]:

    wsuCVSST (t)

  165. Specific heat capacity at constant volume (Cv) of water at saturation line [BTU/(lbm·degF)] as function of temperature t [degF]:

    wsuCVSWT (t)

  166. Sound velocity in steam at saturation line [ft/sec] as function of temperature t [degF]:

    wsuWSST (t)

  167. Sound velocity in water at saturation line [ft/sec] as function of temperature t [degF]:

    wsuWSWT (t)

  168. Thermal conduction of steam at saturation line [BTU/(hour·ft·degF)] as function of temperature t [degF]:

    wsuTHERMCONDSST (t)

  169. Thermal conduction of water at saturation line [BTU/(hour·ft·degF)] as function of temperature t [degF]:

    wsuTHERMCONDSWT (t)

  170. Dynamic viscosity of steam at saturation line [(lbf·sec)/ft2] as function of temperature t [degF]:

    wsuDYNVISSST (t)

  171. Dynamic viscosity of water at saturation line [(lbf·sec)/ft2] as function of temperature t [degF]:

    wsuDYNVISSWT (t)

  172. Prandtl number of steam at saturation line as function of temperature t [degF]:

    wsuPRANDTLESST (t)

  173. Prandtl number of water at saturation line as function of temperature t [degF]:

    wsuPRANDTLESWT (t)

  174. Kinematic viscosity of steam at saturation line [ft2/sec] as function of temperature t [degF]:

    wsuKINVISSST (t)

  175. Kinematic viscosity of water at saturation line [ft2/sec] as function of temperature t [degF]:

    wsuKINVISSWT (t)

  176. Isoentropic exponent of steam at saturation line as function of temperature t [degF]:

    wsuKSST (t)

  177. Isoentropic exponent of water at saturation line as function of temperature t [degF]:

    wsuKSWT (t)

  178. Joule-Thompson coefficient of steam at saturation line [degF/psi] as function of temperature t [degF]:

    wsuJOULETHOMPSONSST (t)

  179. Joule-Thompson coefficient of water at saturation line [degF/psi] as function of temperature t [degF]:

    wsuJOULETHOMPSONSWT (t)

  180. Specific evaporation heat [BTU/lbm] as function of temperature t [degF]:

    wsuRST (t)

    Calculate as r = (hs - hw), where hs - specific enthalpy of steam at saturation line, hw - specific enthalpy of water at saturation line.

  181. WaterSteamPro (Double phase area)

    Functions of properties in double-phase area.

  182. Specific volume in double phase area [ft3/lbm] as function of temperature t [degF], degree of dryness x []:

    wsuVSTX (t, x)

    This function use the functions wsuVSST and wsuVSWT which return specific volumes of steam and water at saturation line. The function use next formula: Vx = (1 - X)·Vw + X·Vs, where Vs = wsuVSST, Vw = wsuVSWT and X - degree of dryness.

  183. Specific internal energy in double phase area [BTU/lbm] as function of temperature t [degF], degree of dryness x []:

    wsuUSTX (t, x)

    This function use the functions wsuUSST and wsuUSWT which return specific internal energies of steam and water at saturation line. The function use next formula: Ux = (1 - X)·Uw + X·Us, where Us = wsuUSST, Uw = wsuUSWT and X - degree of dryness.

  184. Specific entropy in double phase area [BTU/(lbm·degF)] as function of temperature t [degF], degree of dryness x []:

    wsuSSTX (t, x)

    This function use the functions wsuSSST and wsuSSWT which return specific entropies of steam and water at saturation line. The function use next formula: Sx = (1 - X)·Sw + X·Ss, where Ss = wsuSSST, Sw = wsuSSWT and X - degree of dryness.

  185. Specific enthalpy in double phase area [BTU/lbm] as function of temperature t [degF], degree of dryness x []:

    wsuHSTX (t, x)

    This function use the functions wsuHSST and wsuHSWT which return specific enthalpies of steam and water at saturation line. The function use next formula: Hx = (1 - X)·Hw + X·Hs, where Hs = wsuHSST, Hw = wsuHSWT and X - degree of dryness.

  186. Specific heat capacity at constant pressure (Cp) in double phase area [BTU/(lbm·degF)] as function of temperature t [degF], degree of dryness x []:

    wsuCPSTX (t, x)

    This function use the functions wsuCPSST and wsuCPSWT which return specific heat capacities at constant pressure (Cp) of steam and water at saturation line. The function use next formula: CPx = (1 - X)·CPw + X·CPs, where CPs = wsuCPSST, CPw = wsuCPSWT and X - degree of dryness.

  187. Specific heat capacity at constant volume (Cv) in double phase area [BTU/(lbm·degF)] as function of temperature t [degF], degree of dryness x []:

    wsuCVSTX (t, x)

    This function use the functions wsuCVSST and wsuCVSWT which return specific heat capacities at constant volume (Cv) of steam and water at saturation line. The function use next formula: CVx = (1 - X)·CVw + X·CVs, where CVs = wsuCVSST, CVw = wsuCVSWT and X - degree of dryness.

  188. Sound velocity in double phase area [ft/sec] as function of temperature t [degF], degree of dryness x []:

    wsuWSTX (t, x)

    This function use the functions wsuWSST and wsuWSWT which return sound velocities of steam and water at saturation line. The function use next formula: Wx = (1 - X)·Ww + X·Ws, where Ws = wsuWSST, Ww = wsuWSWT and X - degree of dryness.

  189. Thermal conduction in double phase area [BTU/(hour·ft·degF)] as function of temperature t [degF], degree of dryness x []:

    wsuTHERMCONDSTX (t, x)

    This function use the functions wsuTHERMCONDSST and wsuTHERMCONDSWT which return thermal conductions of steam and water at saturation line. The function use next formula: THERMCONDx = (1 - X)·THERMCONDw + X·THERMCONDs, where THERMCONDs = wsuTHERMCONDSST, THERMCONDw = wsuTHERMCONDSWT and X - degree of dryness.

  190. Dynamic viscosity in double phase area [(lbf·sec)/ft2] as function of temperature t [degF], degree of dryness x []:

    wsuDYNVISSTX (t, x)

    This function use the functions wsuDYNVISSST and wsuDYNVISSWT which return dynamic viscosities of steam and water at saturation line. The function use next formula: DYNVISx = (1 - X)·DYNVISw + X·DYNVISs, where DYNVISs = wsuDYNVISSST, DYNVISw = wsuDYNVISSWT and X - degree of dryness.

  191. Prandtl number in double phase area as function of temperature t [degF], degree of dryness x []:

    wsuPRANDTLESTX (t, x)

    This function use the functions wsuPRANDTLESST and wsuPRANDTLESWT which return Prandtl numbers of steam and water at saturation line. The function use next formula: PRANDTLEx = (1 - X)·PRANDTLEw + X·PRANDTLEs, where PRANDTLEs = wsuPRANDTLESST, PRANDTLEw = wsuPRANDTLESWT and X - degree of dryness.

  192. Kinematic viscosity in double phase area [ft2/sec] as function of temperature t [degF], degree of dryness x []:

    wsuKINVISSTX (t, x)

    This function use the functions wsuKINVISSST and wsuKINVISSWT which return kinematic viscosities of steam and water at saturation line. The function use next formula: KINVISx = (1 - X)·KINVISw + X·KINVISs, where KINVISs = wsuKINVISSST, KINVISw = wsuKINVISSWT and X - degree of dryness.

  193. Isoentropic exponent in double phase area as function of temperature t [degF], degree of dryness x []:

    wsuKSTX (t, x)

    This function use the functions wsuKSST and wsuKSWT which return isoentropic exponent of steam and water at saturation line. The function use next formula: Kx = (1 - X)·Kw + X·Ks, where Ks = wsuKSST, Kw = wsuKSWT and X - degree of dryness.

  194. Joule-Thompson coefficient in double phase area [degF/psi] as function of temperature t [degF], degree of dryness x []:

    wsuJOULETHOMPSONSTX (t, x)

    This function use the functions wsuJOULETHOMPSONSST and wsuJOULETHOMPSONSWT which return isoentropic exponent of steam and water at saturation line. The function use next formula: JOULETHOMPSONx = (1 - X)·JOULETHOMPSONw + X·JOULETHOMPSONs, where JOULETHOMPSONs = wsuJOULETHOMPSONSST, JOULETHOMPSONw = wsuJOULETHOMPSONSWT and X - degree of dryness.

  195. Degree of dryness as function of temperature t [degF], specific volume v [ft3/lbm]:

    wsuXSTV (t, v)

    This function use formula: X = (V - Vw)/(Vs - Vw), where Vw = wsuVSWT, Vs = wsuVSST.

  196. Degree of dryness as function of temperature t [degF], specific internal energy u [BTU/lbm]:

    wsuXSTU (t, u)

    This function use formula: X = (U - Uw)/(Us - Uw), where Uw = wsuUSWT, Us = wsuUSST.

  197. Degree of dryness as function of temperature t [degF], specific entropy s [BTU/(lbm·degF)]:

    wsuXSTS (t, s)

    This function use formula: X = (S - Sw)/(Ss - Sw), where Sw = wsuSSWT, Ss = wsuSSST.

  198. Degree of dryness as function of temperature t [degF], specific enthalpy h [BTU/lbm]:

    wsuXSTH (t, h)

    This function use formula: X = (H - Hw)/(Hs - Hw), where Hw = wsuHSWT, Hs = wsuHSST.

  199. Degree of dryness as function of temperature t [degF], specific heat capacity at constant pressure (Cp) cp [BTU/(lbm·degF)]:

    wsuXSTCP (t, cp)

    This function use formula: X = (CP - CPw)/(CPs - CPw), where CPw = wsuCPSWT, CPs = wsuCPSST.

  200. Degree of dryness as function of temperature t [degF], specific heat capacity at constant volume (Cv) cv [BTU/(lbm·degF)]:

    wsuXSTCV (t, cv)

    This function use formula: X = (CV - CVw)/(CVs - CVw), where CVw = wsuCVSWT, CVs = wsuCVSST.

  201. Degree of dryness as function of temperature t [degF], sound velocity w [ft/sec]:

    wsuXSTW (t, w)

    This function use formula: X = (W - Ww)/(Ws - Ww), where Ww = wsuWSWT, Ws = wsuWSST.

  202. Degree of dryness as function of temperature t [degF], thermal conduction tc [BTU/(hour·ft·degF)]:

    wsuXSTTHERMCOND (t, tc)

    This function use formula: X = (TC - TCw)/(TCs - TCw), where TCw = wsuTHERMCONDSWT, TCs = wsuTHERMCONDSST.

  203. Degree of dryness as function of temperature t [degF], dynamic viscosity dv [(lbf·sec)/ft2]:

    wsuXSTDYNVIS (t, dv)

    This function use formula: X = (DV - DVw)/(DVs - DVw), where DVw = wsuDYNVISSWT, DVs = wsuDYNVISSST.

  204. Degree of dryness as function of temperature t [degF], kinematic viscosity kv [ft2/sec]:

    wsuXSTKINVIS (t, kv)

    This function use formula: X = (KV - KVw)/(KVs - KVw), where KVw = wsuKINVISSWT, KVs = wsuKINVISSST.

  205. Degree of dryness as function of temperature t [degF], Prandtl number pr []:

    wsuXSTPRANDTLE (t, pr)

    This function use formula: X = (PR - PRw)/(PRs - PRw), where PRw = wsuPRANDTLESWT, PRs = wsuPRANDTLESST.

  206. Degree of dryness as function of temperature t [degF], Isoentropic exponent k []:

    wsuXSTK (t, k)

    This function use formula: X = (K - Kw)/(Ks - Kw), where Kw = wsuKSWT, Ks = wsuKSST.

  207. Degree of dryness as function of temperature t [degF], Joule-Thomspon coefficient jt [degF/psi]:

    wsuXSTJOULETHOMPSON (t, jt)

    This function use formula: X = (JOULETHOMPSON - JOULETHOMPSONw)/(JOULETHOMPSONs - JOULETHOMPSONw), where JOULETHOMPSONw = wsuJOULETHOMPSONSWT, JOULETHOMPSONs = wsuJOULETHOMPSONSST.

  208. WaterSteamPro (MetaStable)

    Functions for calculating properties of meta-stable supercooled steam

  209. Specific volume of meta-stable supercooled steam [ft3/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuVMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  210. Specific internal energy of meta-stable supercooled steam [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuUMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  211. Specific entropy of meta-stable supercooled steam [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuSMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  212. Specific enthalpy of meta-stable supercooled steam [BTU/lbm] as function of pressure p [psi], temperature t [degF]:

    wsuHMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  213. Specific heat capacity at constant pressure (Cp) of meta-stable supercooled steam [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCPMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  214. Specific heat capacity at constant volume (Cv) of meta-stable supercooled steam [BTU/(lbm·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuCVMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  215. Sound velocity of meta-stable supercooled steam [ft/sec] as function of pressure p [psi], temperature t [degF]:

    wsuWMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  216. Thermal conduction of meta-stable supercooled steam [BTU/(hour·ft·degF)] as function of pressure p [psi], temperature t [degF]:

    wsuTHERMCONDMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  217. Dynamic viscosity of meta-stable supercooled steam [(lbf·sec)/ft2] as function of pressure p [psi], temperature t [degF]:

    wsuDYNVISMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  218. Prandtl number of meta-stable supercooled steam as function of pressure p [psi], temperature t [degF]:

    wsuPRANDTLEMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  219. Kinematic viscosity of meta-stable supercooled steam [ft2/sec] as function of pressure p [psi], temperature t [degF]:

    wsuKINVISMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  220. Isoentropic exponent of meta-stable supercooled steam as function of pressure p [psi], temperature t [degF]:

    wsuKMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  221. Joule-Thompson coefficient of meta-stable supercooled steam [degF/psi] as function of pressure p [psi], temperature t [degF]:

    wsuJOULETHOMPSONMSPT (p, t)

    This function calculate the properties of super-cooled steam (in meta-stable area). The parameters range lie below pressure 10 MPa and degree of dryness above 95%. For calculating used the special formulation for calculating meta-stable area based upon IAPWS IF-97.

  222. WaterSteamPro (System)

    System and adjustment functions.

  223. Set and return internal tolerance of the WaterSteamPro as function of tolerance tolerance []:

    wsuSETTOLERANCE (tolerance)

    Used in functions with arguments (p, h) and (p, s). This tolerance is relative.

  224. Internal tolerance of the WaterSteamPro:

    wsuGETTOLERANCE ()

    Used in functions with arguments (p, h) and (p, s). This tolerance is relative.

  225. Set and return a mode of management of tolerance as function of mode mode []:

    wsuSETTOLERANCEMODE (mode)

    Used in functions with arguments p, h and p, s (wsuTxPH and wsuTxPS). If argument equal to zero the management of tolerance disabled and the speed of functions is increased while the tolerance is decreased.

    Note: Function result has type "long".

  226. Mode of management of tolerance:

    wsuGETTOLERANCEMODE ()

    Used in functions with arguments p, h and p, s (wsuTxPH and wsuTxPS). Zero if the management of tolerance is disabled.

    Note: Function result has type "long".

  227. Set and return a mode of checking the range of functions arguments as function of mode mode []:

    wsuSETCHECKRANGEMODE (mode)

    Used in functions before calculating. If argument mode equal to zero the checking is disabled and the speed of functions is increased but may occur errors and the result may be wrong.

    Note: Function result has type "long".

  228. Mode of checking the range of functions arguments:

    wsuGETCHECKRANGEMODE ()

    Return zero if the checking is disabled.

    Note: Function result has type "long".

  229. Set and return a last error code as function of error code ErrCode []:

    wsuSETLASTERROR (ErrCode)

    This function can be used for estimation of quantity of errors since all error codes are enumerated starting with zero (no error) and subsequently in increasing order. In the case of a range overrun the function returns (and sets) zero value - that means no error.

    Note: Function result has type "long".

  230. Last error code:

    wsuGETLASTERROR ()

    Return last error occurred in any functions except system functions. Any function call (except system) set the error code to zero (no error).

    Note: Function result has type "long".

  231. Last error description:

    wsuGETLASTERRORDESCRIPTION ()

    Return last error description occurred in any function call except system functions. The result of function define in library OKAWSPU.DLL as LPCSTR (ANSI-symbols), but in ActiveX-object WSP.WSPCalculator - as BSTR (Unicode). So in Visual Basic you must use the ActiveX-version of function.

    Note: Function result has type "string".

  232. Process related registration of the WaterSteamPro as function of registration name name [], registration key key []:

    wsuLOCALREGISTRATION (name, key)

    May be used in commercial programs.

    Note: Function result has type "void".

  233. Set and return maximum difference between saturation temperature and input temperature for function wsuWATERSTATEAREA [degF] as function of delta delta [degF]:

    wsuSETDELTATS (delta)

    If difference less than argument of this function (delta) the function wsuWATERSTATEAREA return double phase area.

  234. Maximum difference between saturation temperature and input temperature for function wsuWATERSTATEAREA [degF]:

    wsuGETDELTATS ()

    If difference less than argument of this function (delta) the function wsuWATERSTATEAREA return double phase area.

  235. Set and return maximum iteration's count for Newton method as function of maximum iteration maxiteration []:

    wsuSETMAXITERATION (maxiteration)

    This number used when the Newton method used. If number of iterations more than this value the error WSP_CANT_FIND_ROOT (3) occur.

    Note: Function result has type "long".

  236. Maximum iteration's count for Newton method:

    wsuGETMAXITERATION ()

    This number used when the Newton method used. If number of iterations more than this value the error WSP_CANT_FIND_ROOT (3) occur.

    Note: Function result has type "long".

  237. Set and return maximum difference between pressure values at estimation of the area 3 parameters [psi] as function of delta pressure delta [psi]:

    wsuSETDELTAPRESSURE (delta)

    In area 3 used the Newton method. This method stopped when the difference between values less then delta or maximum iteration count reached.

  238. Maximum difference between pressure values at estimation of the area 3 parameters [psi]:

    wsuGETDELTAPRESSURE ()

    In area 3 used the Newton method. This method stopped when the difference between values less then return value of this function or maximum iteration count reached.

  239. Set and return initial value for water in area 3 [lbm/ft3] as function of density r [lbm/ft3]:

    wsuSETINITWATERDENSITY (r)

    In area 3 used the Newton method. This method need the initial value. The function wsuR3PT use this value to determine density of water.

  240. Initial value for water in area 3 [lbm/ft3]:

    wsuGETINITWATERDENSITY ()

    In area 3 used the Newton method. This method need the initial value. The function wsuR3PT use this value to determine density of water.

  241. Set and return the initial value for steam in area 3 [lbm/ft3] as function of density r [lbm/ft3]:

    wsuSETINITSTEAMDENSITY (r)

    In area 3 used the Newton method. This method need the initial value. The function wsuR3PT use this value to determine density of steam.

  242. Initial value for steam in area 3 [lbm/ft3]:

    wsuGETINITSTEAMDENSITY ()

    In area 3 used the Newton method. This method need the initial value. The function wsuR3PT use this value to determine density of steam.

  243. Internal version of the WaterSteamPro:

    wsuGETWSPVERSION ()

    The format of version is x.yzzz where x - major version, y - minor version, zzz - revision.