Projected area: Difference between revisions
Removed cylinder projected area formula. It relied on {\beta}, the angle between surface normal and plane normal . Cylinders do not have just one normal. |
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The '''Lee-Kesler method''' | |||
<ref>Lee B.I., Kesler M.G., "A Generalized Thermodynamic Correlation Based on Three-Parameter Corresponding States", AIChE J., 21(3), 510-527, 1975 | |||
</ref> | |||
allows the estimation of the [[saturated vapor pressure]] at a given temperature for all components for which the [[critical pressure]] P<sub>c</sub>, the [[critical temperature]] T<sub>c</sub>, and the [[acentric factor]] ω are known. | |||
== Equations == | |||
<math> \ln P_r = f^{(0)} + \omega \cdot f^{(1)} </math> | |||
<math> f^{(0)}=5.92714 - \frac{6.09648}{T_r} - 1.28862 \cdot \ln T_r + 0.169347 \cdot T_r^6 </math> | |||
<math> f^{(1)}=15.2518 - \frac{15.6875}{T_r}-13.4721 \cdot \ln T_r + 0.43577 \cdot T_r^6 </math> | |||
with | |||
<math>P_r=\frac{P}{P_c}</math> ([[reduced pressure]]) und <math>T_r=\frac{T}{T_c}</math> ([[reduced temperature]]). | |||
== Typical errors == | |||
The prediction error can be up to 10% for polar components and small pressures and the calculated pressure is typically too low. For pressures above 1 bar, that means, above the normal boiling point, the typical errors are below 2%. | |||
<ref>Reid R.C., Prausnitz J.M., Poling B.E., "The Properties of Gases & Liquids", 4. Auflage, McGraw-Hill, 1988 | |||
</ref> | |||
== Example calculation == | |||
For [[benzene]] with | |||
* T<sub>c</sub> = 562.12 K<ref name="Brunner">Brunner E., Thies M.C., Schneider G.M., J.Supercrit.Fluids, 39(2), 160-173, 2006</ref> | |||
* P<sub>c</sub> = 4898 kPa<ref name="Brunner" /> | |||
* T<sub>b</sub> = 353.15 K<ref>Silva L.M.C., Mattedi S., Gonzalez-Olmos R., Iglesias M., J.Chem.Thermodyn., 38(12), 1725-1736, 2006</ref> | |||
* ω = 0.2120<ref>[[Dortmund Data Bank]]</ref> | |||
the following calculation for T=T<sub>b</sub> results: | |||
* T<sub>r</sub> = 353.15 / 562.12 = 0.628247 | |||
* f<sup>(0)</sup> = -3.167428 | |||
* f<sup>(1)</sup> = -3.429560 | |||
* P<sub>r</sub> = exp( f<sup>(0)</sup> + ω f<sup>(1)</sup> ) = 0.020354 | |||
* P = P<sub>r</sub> * P<sub>c</sub> = 99.69 kPa | |||
The correct result would be P = 101.325 kPa, the normal (atmospheric) pressure. The deviation is -1.63 kPa or -1.61 %. | |||
It is important to use the same absolute units for T and T<sub>c</sub> as well as for P and P<sub>c</sub>. The unit system used (K or R for T) is irrelevant because of the usage of the reduced values T<sub>r</sub> and P<sub>r</sub>. | |||
== References == | |||
<references/> | |||
{{DEFAULTSORT:Lee-Kesler Method}} | |||
[[Category:Thermodynamic models]] |
Revision as of 18:58, 4 October 2013
The Lee-Kesler method [1] allows the estimation of the saturated vapor pressure at a given temperature for all components for which the critical pressure Pc, the critical temperature Tc, and the acentric factor ω are known.
Equations
with
(reduced pressure) und (reduced temperature).
Typical errors
The prediction error can be up to 10% for polar components and small pressures and the calculated pressure is typically too low. For pressures above 1 bar, that means, above the normal boiling point, the typical errors are below 2%. [2]
Example calculation
For benzene with
the following calculation for T=Tb results:
- Tr = 353.15 / 562.12 = 0.628247
- f(0) = -3.167428
- f(1) = -3.429560
- Pr = exp( f(0) + ω f(1) ) = 0.020354
- P = Pr * Pc = 99.69 kPa
The correct result would be P = 101.325 kPa, the normal (atmospheric) pressure. The deviation is -1.63 kPa or -1.61 %.
It is important to use the same absolute units for T and Tc as well as for P and Pc. The unit system used (K or R for T) is irrelevant because of the usage of the reduced values Tr and Pr.
References
- ↑ Lee B.I., Kesler M.G., "A Generalized Thermodynamic Correlation Based on Three-Parameter Corresponding States", AIChE J., 21(3), 510-527, 1975
- ↑ Reid R.C., Prausnitz J.M., Poling B.E., "The Properties of Gases & Liquids", 4. Auflage, McGraw-Hill, 1988
- ↑ 3.0 3.1 Brunner E., Thies M.C., Schneider G.M., J.Supercrit.Fluids, 39(2), 160-173, 2006
- ↑ Silva L.M.C., Mattedi S., Gonzalez-Olmos R., Iglesias M., J.Chem.Thermodyn., 38(12), 1725-1736, 2006
- ↑ Dortmund Data Bank