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Modern Engineering Thermodynamics

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9.4 Open System Entropy Balance Equations 281<br />

where ð _S P Þ m<br />

= 0, since we are neglecting diffusion of dissimilar species inside the system. The individual entropy<br />

transport rate terms are given in Eqs. (7.61), (7.63), and (9.1) as<br />

Z <br />

ð_S T Þ Q<br />

=<br />

Σ<br />

½ð_S T Þ m<br />

Š net<br />

= ∑<br />

in<br />

<br />

_q<br />

T b<br />

dA (7.61)<br />

act<br />

ð_S T Þ W<br />

= 0 (7.63)<br />

_ms −∑<br />

out<br />

_ms (9.1)<br />

Using the concept of entropy production rate per unit volume, σ, we can express the total entropy production<br />

rate of Eq. (9.3) (neglecting ð _S P Þ m )as<br />

Z<br />

_S P = ð _S P Þ Q + ð _S P Þ W =<br />

V<br />

Z<br />

ðσ Q + σ W ÞdV =<br />

where the total entropy production per unit volume is σ = σ Q + σ W . The relation for σ Q is given by Eq. (7.64) as<br />

V<br />

σdV<br />

<br />

σ Q = − _q <br />

dT<br />

T 2 dx<br />

actual<br />

(7.64)<br />

and the equations for σ W for viscous flow and electrical resistance are given by Eqs. (7.70) and (7.73) as<br />

ðσ W Þ vis = μ T<br />

<br />

dV 2<br />

and ðσ W Þ<br />

dx<br />

elect = J2 e ρ e<br />

T<br />

Putting Eqs. (7.61) and (9.1) into Eq. (7.3) produces a general open system entropy rate balance (SRB) equation as<br />

General open system entropy rate balance (SRB)<br />

Z <br />

_q<br />

dA +∑ _ms − ∑ _ms + _S P = _S system (9.4)<br />

Σ T b act inlet outlet<br />

and, when the system boundaries are isothermal (i.e., T b is constant), this equation reduces to<br />

Isothermal boundary open system entropy rate balance<br />

<br />

_Q<br />

_ms −∑ _ms + _S p = _S system (9.5)<br />

T b act<br />

out<br />

+∑<br />

in<br />

Z<br />

where _Q /T b = ð _q /T b ÞdA: In this equation, _Q is the actual heat transfer rate, and T b is the temperature of the system<br />

Σ<br />

boundary where _Q occurs. The equation for the direct method for determining the entropy production rate is given by<br />

Eq. (9.6) as 1 Z<br />

_S P = Vσ dV > 0 (9.6)<br />

where σ is the total entropy production rate density (EPRD) for the system, given by<br />

σ = σ Q + ðσ W<br />

Þ vis + ðσ W Þ elect + <br />

However, since the use of Eq. (9.6) for the direct determination of _S P is often quite difficult, the example<br />

problems presented in this chapter use the indirect method for determining the entropy production rate ( _S P )in<br />

the entropy rate balance, Eq. (9.5). When this is done, the entropy rate balance can be used to generate<br />

1 In this chapter, we assume that the processes of interest are truly irreversible, so we write _S P > 0, rather than the less restrictive _S P ≥ 0.

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