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Modern Engineering Thermodynamics

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76 CHAPTER 3: Thermodynamic Properties<br />

EXAMPLE 3.5 (Continued )<br />

state (the critical state), and we are asked to determine a thermodynamic property (the mass) at the initial state. In Table 3.4<br />

or Table C.12a of Thermodynamic Tables to accompany <strong>Modern</strong> <strong>Engineering</strong> <strong>Thermodynamics</strong>, we find for water that p c = 3203.8<br />

psia, T c = 1165.1R, and v c = 0.05053 ft 3 /lbm. Also, since both the volume and mass are constant here, v 2 = v 1 = v c .This<br />

process can then be diagrammed as follows:<br />

Constant volume<br />

Initial state !<br />

process<br />

p 1 = 14:696 psia<br />

T 1 = 212°F ðsaturatedÞ<br />

v 1 = v 2 ðfrom the process pathÞ<br />

Final state<br />

p 2 = p c<br />

T 2 = T c<br />

v 2 = v c<br />

Therefore,<br />

m = V v 1<br />

= V v 2<br />

= V v c<br />

=<br />

0:500 ft 3<br />

0:05053 ft 3 = 9:90 lbm<br />

/lbm<br />

We can now find the quality in the initial state by using Eq. (3.26) and the data given in Example 3.2 as<br />

x 1 = v − v f 1<br />

v fg1<br />

= v c − v f 1<br />

v g1 − v f 1<br />

=<br />

ð 0:05053 − 0:01672 Þft3 /lbm<br />

ð26:8 − 0:01672Þft 3 /lbm = 1:26 × 10−3 = 0:126% vapor<br />

Final state (critical point)<br />

x = 1.00<br />

p<br />

x = 0.00<br />

Process<br />

path<br />

14.696<br />

psia<br />

v 1 = v 2 = v c<br />

Initial state<br />

v<br />

p-v diagram<br />

FIGURE 3.19<br />

Example 3.5. Note that, since the quality is not defined at the critical state (quality is one of the properties that has a discontinuity<br />

there), no value for x 2 = x c can be given.<br />

3.9 THERMODYNAMIC EQUATIONS OF STATE<br />

In this section, we discuss some of the basic p-v-T equations of state for various substances. These equations can<br />

be easily typed into a computer spreadsheet, which greatly simplifies the calculations and allows for studying<br />

the effect of varying individual terms and plotting of the results. All engineering students today have access to a<br />

computer, and numerous computer programs can be found on the Internet that calculate the thermodynamic<br />

properties of water, refrigerants, and various other substances.<br />

WHO WAS EMMY NOETHER?<br />

PART 3<br />

From 1908 to 1915, Emmy Noether taught at the University of Erlangen’s Mathematical Institute without pay, occasionally<br />

substituting for her father when he was too ill to lecture. In the spring of 1915, she was invited to return to the University<br />

of Göttingen by David Hilbert and Felix Klein. Their effort to recruit her, however, was blocked by the faculty: Women,<br />

they insisted, should not become faculty. One faculty member protested: “What will our soldiers think when they return to<br />

the university and find that they are required to learn at the feet of a woman?” Hilbert responded with indignation, stating,<br />

“I do not see that the sex of the candidate is an argument against her admission as faculty. 3 After all, we are a university,<br />

not a bath house.”

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