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Modern Engineering Thermodynamics

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378 CHAPTER 11: More Thermodynamic Relations<br />

Note that following a path of constant T for the second integral in this equation is very logical since f depends<br />

on only v and T and we are integrating over v.<br />

For example, if we had an equation of state of the form pv = RT + αT 2 /v, then<br />

and<br />

then,<br />

Equation (11.19) now gives<br />

T<br />

<br />

∂p <br />

∂T<br />

v<br />

T<br />

p = RT<br />

v + αT2<br />

v 2<br />

<br />

∂p<br />

= R ∂T v + 2αT<br />

v<br />

v 2<br />

<br />

∂p <br />

∂T<br />

v<br />

= RT<br />

v + 2αT2<br />

v 2<br />

− p = RT<br />

<br />

v + 2αT2 − RT<br />

<br />

v 2 v + αT2<br />

v 2 = αT2<br />

v 2<br />

Z T1<br />

Z v1<br />

u 1 − u 0 = c 0 v dT +<br />

T 0<br />

=<br />

=<br />

Z T1<br />

v 0 =∞<br />

<br />

αT 2<br />

dv<br />

v 2<br />

<br />

c 0 v dT + αT2 − 1 <br />

v 1<br />

v<br />

T 0<br />

∞<br />

Z T1<br />

c 0 v dT + αT 1 2<br />

v<br />

T 0 1<br />

and if the zero pressure specific heat c 0 v is constant over the temperature range T 0 to T 1 , this equation reduces to<br />

u 1 − u 0 = c 0 v ðT 1 − T 0 Þ − αT2 1<br />

v 1<br />

A similar equation can be easily developed for a second state, and we can then combine them to produce an<br />

equation for the change in specific internal energy between these two states for this material as<br />

<br />

u 2 − u 1 = c 0 v ðT 2 − T 1 Þ − α T2 2<br />

v<br />

− T2 1<br />

2 v 1<br />

and the reference state values have completely cancelled out.<br />

11.7 CONSTRUCTING TABLES AND CHARTS<br />

We are now able to use Eqs. (11.19), (11.22), (11.24), and (11.26) to construct thermodynamic tables and charts.<br />

The construction of thermodynamic tables and charts like the ones in Thermodynamic Tables to accompany <strong>Modern</strong><br />

<strong>Engineering</strong> <strong>Thermodynamics</strong> require, first of all, that a great deal of accurate experimental p, v, T, andc v (or c p )databe<br />

obtained. These data are reduced to mathematical equations through curve-fitting techniques. The resultant mathematical<br />

equations are used to derive equations for u, h, ands using the thermodynamic property relations discussed<br />

previously. One of the simplest methods for generating saturation and superheat tables is carried out as follows.<br />

A. The following four data sets must be developed from appropriate experiments:<br />

Data set 1. Saturation temperature and saturation pressure (T sat , p sat ).<br />

Data set 2. Pressure, specific volume, and temperature in the superheated vapor region and along the<br />

saturated vapor curve (p, v, T).<br />

Data set 3. Saturated liquid specific volume (or density) and saturation temperature (v f , T sat ).<br />

Data set 4. Low- (or zero) pressure constant volume specific heat, c 0 v and temperature T in the superheated<br />

vapor region and along the saturated vapor curve. The superscript 0 is used to denote the fact that the c 0 v<br />

values are measured at essentially zero pressure.<br />

B. Once these four data sets have been obtained, a mathematical equation is curve fit to each of them to<br />

obtain four mathematical equations of the form<br />

Curve fit 1: p sat = p sat ðT sat Þ<br />

(11.31a)

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