17.01.2015 Views

chapter one the estimation of physical properties

chapter one the estimation of physical properties

chapter one the estimation of physical properties

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

PURE COMPONENT CONSTANTS<br />

2.22 CHAPTER TWO<br />

A discussion comparing <strong>the</strong> QSPR techniques with o<strong>the</strong>r methods for <strong>the</strong> <strong>properties</strong><br />

<strong>of</strong> this <strong>chapter</strong> is presented below and in Sec. 2-5.<br />

Discussion and Recommendations for Critical Properties. The methods <strong>of</strong> Joback<br />

(1984; 1987), Constantinou and Gani (1994), Wilson and Jasperson (1996)<br />

and Marrero and Pardillo (1999) were evaluated. Summaries <strong>of</strong> comparisons with<br />

data from Appendix A are given in Tables 2-1, 2-2, 2-4, and 2-6. A few results<br />

from QSPR methods are given in Table 2-7. Overall, <strong>the</strong> methods are all comparable<br />

in accuracy.<br />

A useful method for determining consistency among T c , P c , and V c is to use Eq.<br />

(2-3.2) relating <strong>the</strong> critical compressibility factor, Z c P c V c /RT c , to <strong>the</strong> acentric<br />

factor (Sec. 2-3). The <strong>the</strong>oretical basis <strong>of</strong> <strong>the</strong> acentric factor suggests that except<br />

for substances with T c 100 K, Z c must be less than 0.291. When Eq. (2-3.2) was<br />

tested on <strong>the</strong> 142 substances <strong>of</strong> Appendix A for which reliable values <strong>of</strong> Z c and <br />

are available and for which <strong>the</strong> dipole moment was less than 1.0 debye, <strong>the</strong> average<br />

absolute percent error in Z c was 2% with only 9 substances having errors greater<br />

than 5%. When applied to 301 compounds <strong>of</strong> all types in Appendix A, <strong>the</strong> average<br />

percent error was 5% with 32 errors being larger than 10%. Some <strong>of</strong> <strong>the</strong>se errors<br />

may be from data instead <strong>of</strong> correlation inadequacy. In general, data ra<strong>the</strong>r than<br />

<strong>estimation</strong> methods should be used for substances with <strong>one</strong> or two carbon atoms.<br />

Critical Temperature, T c . The methods all are broadly applicable, describing<br />

nearly all <strong>the</strong> substances <strong>of</strong> Appendix A; <strong>the</strong> average percent <strong>of</strong> error is around 1%<br />

with few, if any substances being <strong>of</strong>f by more than 10%. If an experimental T b is<br />

available, <strong>the</strong> method <strong>of</strong> Marrero and Pardillo has higher accuracy than does that<br />

<strong>of</strong> Wilson and Jasperson. On <strong>the</strong> o<strong>the</strong>r hand, for simplicity and breadth <strong>of</strong> substances,<br />

<strong>the</strong> Wilson/Jasperson method is best since it has <strong>the</strong> fewest groups to<br />

tabulate, is based mostly on atom contributions, and treats inorganic substances as<br />

well as organics. Finally, Joback’s method covers <strong>the</strong> broadest range <strong>of</strong> compounds<br />

even though it is somewhat less accurate and more complex.<br />

However, if <strong>the</strong>re is no measured T b available and estimated values must be<br />

used, <strong>the</strong> errors in <strong>the</strong>se methods increase considerably. Then, if <strong>the</strong> substance has<br />

fewer than 3 carbons, ei<strong>the</strong>r <strong>the</strong> Wilson/Jasperson or Marrero/Pardillo method is<br />

most reliable; if <strong>the</strong> substance is larger, <strong>the</strong> Constantinou/Gani approach generally<br />

gives better results with Second Order calculations being marginally better than<br />

First Order. The Joback method is somewhat less accurate than <strong>the</strong>se.<br />

The molecular descriptor method <strong>of</strong> Jurs is as accurate as <strong>the</strong> group/bond/atom<br />

methods, at least for <strong>the</strong> substances compared here, though <strong>the</strong> earlier method <strong>of</strong><br />

Grigoras is not. While <strong>the</strong> method is not as accessible, current applications show<br />

that once a user has established <strong>the</strong> capability <strong>of</strong> computing descriptors, <strong>the</strong>y can<br />

be used for many <strong>properties</strong>.<br />

Critical Pressure, P c . The methods all are broadly applicable, describing nearly<br />

all <strong>the</strong> substances <strong>of</strong> Appendix A. All methods give average errors <strong>of</strong> about 5%<br />

with about <strong>the</strong> same fraction <strong>of</strong> substances (20%) having errors greater than 10%.<br />

The Wilson/Jasperson method has <strong>the</strong> lowest errors when an experimental value<br />

<strong>of</strong> T c is used; when T c is estimated <strong>the</strong> errors in P c are larger than <strong>the</strong> o<strong>the</strong>r methods.<br />

All show better results for substances with 3 or more carbons, except for a few<br />

species. The Constantinou/Gani Second Order contributions do not significantly<br />

improve agreement though <strong>the</strong> Second Order contributions to <strong>the</strong> Wilson/Jasperson<br />

method are quite important. Thus, <strong>the</strong>re is little to choose among <strong>the</strong> methods. The<br />

decision can be based less on accuracy and reliability than on breadth <strong>of</strong> applicability<br />

and ease <strong>of</strong> use.<br />

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com)<br />

Copyright © 2004 The McGraw-Hill Companies. All rights reserved.<br />

Any use is subject to <strong>the</strong> Terms <strong>of</strong> Use as given at <strong>the</strong> website.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!