Table 6.6-1 The Critical and Other Constants for Selected Fluids Molecular Weight (g mol-) V. (m/kmol)...

 

 

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Table 6.6-1 The Critical and Other Constants for Selected Fluids Molecular Weight (g mol-) V. (m/kmol) Substance Symbol T.(K) P (MPa) Z. Toil (K) Acetylene Ammonia C,H2 NH3 26.038 308.3 405.6 6.140 0.113 0.271 0.184 0.250 189.2 17.031 11.28 0.0724 0.0749 0.242 239.7 Ar 39.948 150.8 Argon Benzene n-Butane Isobutane 1-Butene Carbon dioxide Carbon monoxide Carbon tetrachloride 4.874 0.291 -0.004 87.3 CH6 C4H10 C4H10 78,114 562.1 4.894 0.259 0.271 0.212 353.3 58.124 58.124 425.2 3.800 0.255 0.274 0.193 272.7 408.1 419.6 3.648 0.263 0.283 0.176 261.3 0.240 0.0940 56.108 4.023 0.277 0.187 266.9 194.7 CO2 CO 44.010 304.2 7.376 0.274 0.225 28.010 132,9 3.496 0.0931 0.295 0.049 81.7 349.7 153.823 556.4 4.560 0.276 0.272 0.194 n-Decane n-Dodecane Ethane C10H22 C12H26 C,H6 C4H100 C,H4 Не 142.286 617.6 2.108 0.603 0.247 0.490 447.3 170.340 658.3 1.824 0.713 0.24 0.562 489.5 30.070 305.4 4.884 0.148 0.285 0.098 184.5 307.7 Ethyl ether Ethylene Helium 74.123 466.7 3.638 5.036 0.280 0.262 0.281 28.054 282.4 0.129 0.276 0.085 169.4 4.003 5.19 0.227 0.0573 0.301 -0.387 4.21 540.2 n-Heptane n-Hexane C;H16 C,H14 H2 100.205 2.736 0.304 0.263 0.351 371.6 86.178 507.4 2.969 0.370 0.260 0.296 341.9 2.016 33.2 1.297 Hydrogen Hydrogen fluoride Hydrogen sulfide Methane Naphthalene Neon Nitric oxide Nitrogen n-Octane Oxygen n-Pentane Isopentane Propane Propylene Refrigerant R12 Refrigerant HFC-134a Sulfur dioxide Toluene Water Xenon 0.065 0.305 -0.22 20.4 | HF 20.006 461.0 6.488 (0.069 0.12 0.372 292.7 373.2 H2S CH4 CioHg Ne 34.080 8.942 0.0985 0.284 0.100 212.8 16.043 190.6 4.600 0.099 0.288 0.008 111.7 128,174 748.4 4.05 0.410 0.267 0.302 491.1 20.183 44.4 2.756 0.0417 0.058 0.0895 0.311 27.0 NO 30.006 180.0 6.485 0.250 0.607 121.4 N2 C3H18 O2 CSH12 CSH12 C,Hg C3H6 CC,F2 CH2FCF, SO2 C,Hs H2O Xe 28.013 126.2 3.394 0.290 0.040 77.4 114.232 568.8 2.482 0.492 0.259 0.288 0.394 398.8 31.999 154.6 5.046 0.0732 0.021 90.2 309.2 72.151 469.6 3.374 0.304 0.262 0.271 0.251 72.151 3.384 4,246 301.0 231.1 460.4 0.306 0.227 44.097 42.081 369.8 365.0 0.203 0.281 0,152 4.620 0.181 0.275 0.148 225.4 4.124 4.060 120.914 385.0 0.217 243.4 0.280 0.258 0.268 0.264 0.176 102.03 64.063 0.332 0.251 374,23 0.198 247.1 0.122 0.316 263 383.8 373.2 430.8 7.883 92.141 591.7 4.113 0.257 647.3 18.015 131.300 22.048 5.836 0.056 0.229 0.344 289.7 0.118 0.286 0.002 165.0 Source: Adapted from R. C. Reid, J. M. Prausnitz, and B. E. Poling, The Properties of Gases and Liquids, 4th ed., McGraw-Hill, New York, 1986, Appendix A and other sources. 44 Applied Hydrocarbon Thermodynamics LINES OF CONSTANT REDUCED TEMPERATURE TR-1.60- 1.0 -1.6- 1.3 1.5 1.50 0.9 1.40 1.0 F1.30- 0.8 1.20 0.7 1.16- 1.14 1.12 0.6 1.10- 0.5 0.4 0.3 0.2 3.0 2.5 2.0 1.5 1.0 REDUCED PRESSURE P=. R Pc %3D 0.1 0.5 where P represents reduced vapor pressure. The a is called Riedel's parameter. The following year, basically the same parameter was independently introduced by Martin and Hou(45) in their development of an equation of state. In the same year Figure 4.5. Generalized compressibility factor chart. The two-parameter corresponding states principle led to an important generalization of thermodynamic properties. But as more experimental data became available, a great many fluids of non-spherical molecules were found to de- viate from the principle. This has necessitated a "third pa- 1.08 V1.06 1.05 0.95 0.90 1.00 0.80 RT Z=PV However, if the principle of corresponding states were exact, the vapor pressure curves for all the components, plotted in the reduced form, should result in one composite curve; that in practice does not occur due to differences in molecular structures of various substances. Therefore, to account for the deviation from the corresponding states principle, a third parameter called the acentric factor @ (see Reid et al.3 for listing of values for various pure components) is introduced in the generalized relationship expressed by Equation 11.3: Pr = exp(A+ @B) (11.4) %3D where A and B are expressed by the following equations: 6.09648 -1.28866 In(T, )+0.16934(T,)° T, A = 5.92714 – (11.5). 15.6875 B = 15.2518 – -13.4721 In(T;)+0.4357(T,)° (11.6) In Equation 11.4, since the product of A + @B_is dimensionless, vapor pressure P takes pertinent units that are used for critical pressure, P. The consistency of Equation 11.4 is evident because when T= T, consequently, T, = 1, the condition at which both A and B are 0 eventually resulting in the equality of P, and P, that is, at %3D V. Table 6.6-1 The Critical and Other Constants for Selected Fluids Molecular Weight (g mol-) V. (m/kmol) Substance Symbol T.(K) P (MPa) Z. Toil (K) Acetylene Ammonia C,H2 NH3 26.038 308.3 405.6 6.140 0.113 0.271 0.184 0.250 189.2 17.031 11.28 0.0724 0.0749 0.242 239.7 Ar 39.948 150.8 Argon Benzene n-Butane Isobutane 1-Butene Carbon dioxide Carbon monoxide Carbon tetrachloride 4.874 0.291 -0.004 87.3 CH6 C4H10 C4H10 78,114 562.1 4.894 0.259 0.271 0.212 353.3 58.124 58.124 425.2 3.800 0.255 0.274 0.193 272.7 408.1 419.6 3.648 0.263 0.283 0.176 261.3 0.240 0.0940 56.108 4.023 0.277 0.187 266.9 194.7 CO2 CO 44.010 304.2 7.376 0.274 0.225 28.010 132,9 3.496 0.0931 0.295 0.049 81.7 349.7 153.823 556.4 4.560 0.276 0.272 0.194 n-Decane n-Dodecane Ethane C10H22 C12H26 C,H6 C4H100 C,H4 Не 142.286 617.6 2.108 0.603 0.247 0.490 447.3 170.340 658.3 1.824 0.713 0.24 0.562 489.5 30.070 305.4 4.884 0.148 0.285 0.098 184.5 307.7 Ethyl ether Ethylene Helium 74.123 466.7 3.638 5.036 0.280 0.262 0.281 28.054 282.4 0.129 0.276 0.085 169.4 4.003 5.19 0.227 0.0573 0.301 -0.387 4.21 540.2 n-Heptane n-Hexane C;H16 C,H14 H2 100.205 2.736 0.304 0.263 0.351 371.6 86.178 507.4 2.969 0.370 0.260 0.296 341.9 2.016 33.2 1.297 Hydrogen Hydrogen fluoride Hydrogen sulfide Methane Naphthalene Neon Nitric oxide Nitrogen n-Octane Oxygen n-Pentane Isopentane Propane Propylene Refrigerant R12 Refrigerant HFC-134a Sulfur dioxide Toluene Water Xenon 0.065 0.305 -0.22 20.4 | HF 20.006 461.0 6.488 (0.069 0.12 0.372 292.7 373.2 H2S CH4 CioHg Ne 34.080 8.942 0.0985 0.284 0.100 212.8 16.043 190.6 4.600 0.099 0.288 0.008 111.7 128,174 748.4 4.05 0.410 0.267 0.302 491.1 20.183 44.4 2.756 0.0417 0.058 0.0895 0.311 27.0 NO 30.006 180.0 6.485 0.250 0.607 121.4 N2 C3H18 O2 CSH12 CSH12 C,Hg C3H6 CC,F2 CH2FCF, SO2 C,Hs H2O Xe 28.013 126.2 3.394 0.290 0.040 77.4 114.232 568.8 2.482 0.492 0.259 0.288 0.394 398.8 31.999 154.6 5.046 0.0732 0.021 90.2 309.2 72.151 469.6 3.374 0.304 0.262 0.271 0.251 72.151 3.384 4,246 301.0 231.1 460.4 0.306 0.227 44.097 42.081 369.8 365.0 0.203 0.281 0,152 4.620 0.181 0.275 0.148 225.4 4.124 4.060 120.914 385.0 0.217 243.4 0.280 0.258 0.268 0.264 0.176 102.03 64.063 0.332 0.251 374,23 0.198 247.1 0.122 0.316 263 383.8 373.2 430.8 7.883 92.141 591.7 4.113 0.257 647.3 18.015 131.300 22.048 5.836 0.056 0.229 0.344 289.7 0.118 0.286 0.002 165.0 Source: Adapted from R. C. Reid, J. M. Prausnitz, and B. E. Poling, The Properties of Gases and Liquids, 4th ed., McGraw-Hill, New York, 1986, Appendix A and other sources. 44 Applied Hydrocarbon Thermodynamics LINES OF CONSTANT REDUCED TEMPERATURE TR-1.60- 1.0 -1.6- 1.3 1.5 1.50 0.9 1.40 1.0 F1.30- 0.8 1.20 0.7 1.16- 1.14 1.12 0.6 1.10- 0.5 0.4 0.3 0.2 3.0 2.5 2.0 1.5 1.0 REDUCED PRESSURE P=. R Pc %3D 0.1 0.5 where P represents reduced vapor pressure. The a is called Riedel's parameter. The following year, basically the same parameter was independently introduced by Martin and Hou(45) in their development of an equation of state. In the same year Figure 4.5. Generalized compressibility factor chart. The two-parameter corresponding states principle led to an important generalization of thermodynamic properties. But as more experimental data became available, a great many fluids of non-spherical molecules were found to de- viate from the principle. This has necessitated a "third pa- 1.08 V1.06 1.05 0.95 0.90 1.00 0.80 RT Z=PV However, if the principle of corresponding states were exact, the vapor pressure curves for all the components, plotted in the reduced form, should result in one composite curve; that in practice does not occur due to differences in molecular structures of various substances. Therefore, to account for the deviation from the corresponding states principle, a third parameter called the acentric factor @ (see Reid et al.3 for listing of values for various pure components) is introduced in the generalized relationship expressed by Equation 11.3: Pr = exp(A+ @B) (11.4) %3D where A and B are expressed by the following equations: 6.09648 -1.28866 In(T, )+0.16934(T,)° T, A = 5.92714 – (11.5). 15.6875 B = 15.2518 – -13.4721 In(T;)+0.4357(T,)° (11.6) In Equation 11.4, since the product of A + @B_is dimensionless, vapor pressure P takes pertinent units that are used for critical pressure, P. The consistency of Equation 11.4 is evident because when T= T, consequently, T, = 1, the condition at which both A and B are 0 eventually resulting in the equality of P, and P, that is, at %3D V.

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Reduced Temperature and pressure In thermodynamics the reduced properties of a fluid are a set of state variables scaled by the fluids state propertie... View the full answer