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Modern Engineering Thermodynamics

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Problems 243<br />

amount of work W irr is dissipated within the system due to irreversibilities inside the system, then the<br />

entropy produced by these irreversibilities is<br />

<br />

W<br />

ðS P Þ = irr<br />

(7.68a)<br />

W 1 T 2<br />

T =constant<br />

and the corresponding entropy production rate is<br />

<br />

_S P<br />

W = _W<br />

T<br />

irr<br />

(7.58a)<br />

14. But if we know the irreversibilities are due to a velocity gradient dV/dx in a liquid with viscosity μ at a<br />

temperature T and that they occur in a system of volume V during a time interval 0–τ, then we can calculate<br />

the entropy production and entropy production rates directly from<br />

Z Z<br />

μ<br />

<br />

ðS dV 2dt<br />

P Þ W<br />

=<br />

dV (7.71)<br />

τ V T dx<br />

vis<br />

and<br />

Z<br />

μ<br />

<br />

dV 2dV<br />

_S P W<br />

=<br />

(7.72)<br />

V T dx<br />

vis<br />

Alternatively, if the irreversibilities are due to the flow of a constant electrical current I flowing in an<br />

isothermal system with uniform electrical resistance R e at temperature T, then we have<br />

_S P<br />

<br />

W<br />

elect<br />

ðspecialÞ<br />

= I2 R e<br />

T<br />

(7.74)<br />

Problems (* indicates problems in SI units)<br />

The first ten problems are designed to review some basic thermodynamic<br />

concepts of this and earlier chapters. They may<br />

have more than one correct answer.<br />

1. A closed system becomes an open system when<br />

a. There is no heat transfer to energy.<br />

b. There is no work transfer of energy.<br />

c. There is no mass flow.<br />

d. There is no entropy production.<br />

e. There is no kinetic or potential energy.<br />

f. None of the above.<br />

2. Which of the following are intensive properties: (a) pressure,<br />

(b) temperature, (c) volume, (d) mass, (e) quality, (f) power.<br />

3. The entropy change of a closed system is zero for which of the<br />

following processes: (a) adiabatic, (b) isothermal, (c) isentropic,<br />

(d) isenthalpic, (e) aergonic, (f) reversible.<br />

4.* An insulated, rigid container is divided into two<br />

compartments separated by a partition. One compartment<br />

contains air at 15°C and 0.101 MPa, the other compartment<br />

contains air at 40.°C and 0.101 MPa. When the dividing<br />

partition is removed, the total internal energy of the system<br />

(a) increases, (b) decreases, (c) does not change, (d) is converted<br />

into entropy, (e) is converted into temperature, (f) is converted<br />

into heat.<br />

5. A rigid container contains air (an ideal gas), at 70.0°F and<br />

14.7 psia. If the air is heated to 510.°F, its pressure (a) increases,<br />

(b) decreases, (c) does not change, (d) causes moving boundary<br />

work to occur, (e) causes polytropic work to occur, (f) is<br />

converted into thermal energy.<br />

6. A constant velocity throttling process (a) is reversible, (b) is<br />

isothermal, (c) is isentropic, (d) is isenthalpic, (e) is aergonic,<br />

(f) does not exist in the real world.<br />

7. Heat and work are both (a) intensive properties, (b) extensive<br />

properties, (c) process path dependent, (d) zero for an ideal gas,<br />

(e) zero for an adiabatic process, (f) zero for an aergonic process.<br />

8. An ideal gas must satisfy (a) pv n = constant, (b) u = u(T),<br />

(c) s = constant, (d) p 2 /p 1 = v 1 /v 2 ,(e)pv = nRT, (f)pv = mRT.<br />

9. In a steady flow irreversible process, the total entropy of a system<br />

a. Always increases.<br />

b. Always decreases.<br />

c. Always remains constant.<br />

d. Can increase, decrease, or remain constant.<br />

e. Cannot decrease.<br />

f. Cannot remain constant.<br />

10. To determine the maximum possible work that a heat engine<br />

could produce, one must assume<br />

a. No entropy is produced by the engine.<br />

b. No heat energy is discharged to the environment.

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