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Modern Engineering Thermodynamics

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8.4 Diffusional Mixing 271<br />

Exercises<br />

26. Recompute the entropy production rate _S P in Example 8.14 when the steady state surface temperature of the board<br />

increases to 38.0°C. Keep the values of all the other variables the same as they are in Example 8.14.<br />

Answer: _S P<br />

W = 1:61 × 10–4 W/K:<br />

27. Determine the entropy production rate _S P in Example 8.14 if the current is increased to 50.0 mA. Keep the values of all<br />

the other variables the same as they are in Example 8.14. Answer: _S P<br />

W = 8:25 × 10–4 W/K:<br />

28. If the circuit voltage is increased from 5.00 V to 30.0 V in Example 8.14, determine the new entropy production rate.<br />

Keep the values of all the other variables the same as they are in Example 8.14. Answer: _S P<br />

W = 9:90 × 10–4 W/K:<br />

8.4 DIFFUSIONAL MIXING<br />

Here, we wish to use the indirect method to analyze the entropy production that results from a simple diffusion<br />

type of mixing process. Consider the rigid, insulated container shown in Figure 8.18. It contains the same substance<br />

on both sides of the partition but generally at different pressures, temperatures, and amounts. When the<br />

partition is removed, the material in the chambers mixes by diffusion, resulting in a final temperature T 2 and<br />

final pressure p 2 . We are interested in the amount of entropy produced by this mixing process.<br />

The energy balance equation for this system gives<br />

1Q 2<br />

0<br />

ðadiabaticÞ<br />

− 1 W 2<br />

= U 2 − U 1 + KE 2 − KE 1 + PE 2 − PE 1<br />

⎵<br />

0 ðadiabaticÞ<br />

0 ðstationary systemÞ<br />

or<br />

U 2 = m 2 u 2 = U 1 = m a u a + m b u b<br />

where<br />

u 2 = m au a + m b u b<br />

m a + m b<br />

= u b + yu ð a − u b Þ (8.9)<br />

and<br />

The entropy balance equation gives<br />

y =<br />

1 − y =<br />

m a<br />

m a + m b<br />

m b<br />

m a + m b<br />

1ðS P Þ 2<br />

= S 2 − S 1 − 1 Q 2<br />

T b<br />

0<br />

or<br />

ðadiabaticÞ<br />

Entropy production in two-component mixing:<br />

1ðS P Þ 2<br />

= m 2 s 2 − m a s a − m b s b p<br />

= ðm a + m b Þ½s 2 − s b + ys ð b − s a ÞŠ<br />

(8.10)<br />

Partition<br />

Insulation<br />

T a , p a<br />

a , m a<br />

A<br />

T b , p b<br />

b , m b<br />

A<br />

Mixing<br />

process<br />

T 2 , p 2<br />

2, m 2<br />

A<br />

State 1 State 2<br />

FIGURE 8.18<br />

Mixing of single-species substances.

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