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Direct Energy, 2018a

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12 RELATING ENERGY CONVERSION PROCESSES 285<br />

would take energy to restore the system to the ordered state. Both of these<br />

systems can be described by the language of calculus of variations. As detailed<br />

in the fourth column, temperature can be chosen as the generalized<br />

path and entropy can be chosen as the generalized potential. Alternatively<br />

asdetailed in the fth column, entropy can be chosen asthe generalized<br />

path and temperature can be chosen as the generalized potential. Both<br />

of these columns assume that the pressure and volume remain constant.<br />

The quantity C v , which shows up in these columns, is the specic heat at<br />

constant volume in units<br />

J<br />

, and it wasintroduced in Sec. 8.3.<br />

g·K<br />

The equation of motion that results when temperature is chosen as the<br />

path and entropy ischosen asthe generalized potential isa statement of<br />

conservation of entropy, and each term of thisequation hasthe unitsof<br />

entropy. Thisrelationship ismore commonly known asthe second law of<br />

thermodynamics, and it shows up in the second to last row of Table 12.7.<br />

More commonly, the law is written for a closed system as [109, p. 236],<br />

ˆ δQ<br />

ΔS =<br />

T + S produced. (12.22)<br />

In words, it says the change in entropy within a control mass is equal to<br />

the sum of the entropy out of the control mass due to heat transfer plus<br />

the entropy produced by the system.<br />

(change in entropy) =(entropy out due to heat)+(entropy produced)<br />

A system can become more organized or more disordered, so ΔS may<br />

be positive or negative. If energy is supplied in ´ or out, entropy can be<br />

δQ<br />

transfered in or out of a system, so the quantity may be positive or<br />

T<br />

negative.<br />

<strong>Energy</strong> is listed in the third to last row of Table 12.7 in two dierent<br />

forms. The rst expression is an integral expression. For example, you<br />

can integrate the volume with respect to pressure to nd the energy of a<br />

system.<br />

ˆ<br />

E = VdP (12.23)<br />

Alternatively, the second expression<br />

ΔE = VΔP (12.24)<br />

can be used to nd change in energy in the case when volume is not a<br />

strong function of pressure over a small element.

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