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Modern Engineering Thermodynamics

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7.7 Clausius’s Definition of Entropy 219<br />

T<br />

An infinite<br />

number of<br />

infinitesimal<br />

heat engine<br />

cycles<br />

dT<br />

An arbitrary<br />

thermodynamic<br />

cycle for a<br />

closed system<br />

FIGURE 7.11<br />

An infinite number of infinitesimal heat engine cycles approximating an arbitrary closed system thermodynamic cycle.<br />

A<br />

operating over an infinitely small temperature difference, T H ≈ T L = T and ðQ H Þ rev − jQ L j rev ≈ dQ rev .Then,in<br />

the limit, the previous equation becomes<br />

" lim ∑ # I <br />

Q dQ<br />

=<br />

= 0 (7.21)<br />

n!∞<br />

n cycles<br />

T<br />

T<br />

The temperature T in this equation is the absolute temperature at the point where the heat transfer dQ occurs.<br />

Clausius then noted the remarkable result that, since, by definition,<br />

I<br />

ðAny thermodynamic property differentialÞ = 0<br />

cycle<br />

the argument of the integral in Eq. (7.21) must define a thermodynamic property. That is,<br />

<br />

dQ<br />

= Differential of some thermodynamic property<br />

T<br />

rev<br />

But, which property? The term dQ by itself is a path function and thus cannot be a thermodynamic property<br />

rev<br />

differential. However, when dQ is divided by T, a property differential results. Clausius realized that he had<br />

rev<br />

discovered a new thermodynamic property and he chose to name it entropy 7 and represent the total entropy of a<br />

system by the symbol S, where<br />

<br />

dS =<br />

dQ <br />

(7.22)<br />

T<br />

or<br />

or<br />

S 2 − S 1 =<br />

s 2 − s 1 = S 2 − S 1<br />

m<br />

Z 2<br />

1<br />

cycle<br />

<br />

= 1 m<br />

rev<br />

dQ<br />

T<br />

<br />

Z 2<br />

1<br />

rev<br />

<br />

rev<br />

dQ<br />

T<br />

<br />

rev<br />

(7.23)<br />

(7.24)<br />

Be careful to note that Eqs. (7.22)–(7.24), which define entropy, are for a closed system of fixed mass m only. The<br />

effect of mass flow on system entropy is taken up in a separate section of this chapter.<br />

The use of a relative temperature scale in a grouping of units can sometimes be confusing. For example, when a<br />

temperature unit appears in the denominator of a units grouping, it can be written either as °F or R (or °C orK<br />

in SI) because only the degree size there is important. Therefore, Eq. (7.24) indicates that the units of specific<br />

entropy can be written correctly in either of the following forms:<br />

s ½in Btu/ ðlbm.°FÞŠ≡ s ½in Btu/ ðlbm.RÞŠ<br />

7 Here is a translation of how Clausius, in 1865, described why he chose the word entropy for the name of his new property. “We<br />

might call S the transformational content of the body, just as we termed the quantity U the heat and work content of the body. But since<br />

I believe it is better to borrow terms for important quantities from the ancient languages so that they may be adopted unchanged in all<br />

modern languages, I propose to call the quantity S the entropy of the body, from the Greek word ητροπή, meaning a transformation.”

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