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Modern Engineering Thermodynamics

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Problems 531<br />

horsepower hour. Assuming a heating value for coal of<br />

13.0 × 10 3 Btu/lbm and that the engine was reversible,<br />

determine the thermal efficiency of this engine.<br />

49. The air standard Ericsson cycle (see Figure 13.40) is made up of<br />

an isothermal compressor (T 2 =T 3 =T L ), an isothermal prime<br />

mover (T 1 =T 4 =T H ), and an isobaric regenerator (p 1 = p 2 and<br />

p 3 = p 4 ). Show that the compressor and prime mover must have<br />

identical pressure ratios, that is, p 2 /p 3 =p 1 /p 4 , and show that this<br />

also requires that v 3 /v 2 =v 4 /v 1 .<br />

50.* An Ericsson cycle operates with a compressor inlet pressure and<br />

volume of 1.00 MPa, 0.0200 m 3 and a turbine inlet pressure and<br />

volume of 5.00 MPa, 0.0400 m 3 . For a reversible cycle, determine<br />

a. The heat added.<br />

b. The heat rejected.<br />

c. The work done.<br />

d. The thermal efficiency of the cycle.<br />

51.* An inventor claims to have developed a Lenoir engine with an<br />

isentropic compression ratio of 8.00 to 1 that produces a<br />

combustion temperature of 1500.°C when the intake temperature<br />

is 20.0°C. Assuming k = 1.40 and that the engine operates on a<br />

cold ASC, show whether or not the inventor’s claim is possible.<br />

52.* A World War II Lenoir cycle “buzz bomb” has an air intake at<br />

10.0°C, a combustion temperature of 1000.°C, and a compression<br />

ratio of 2.30. Determine its cold ASC thermal efficiency.<br />

53.* Plot the cold ASC thermal efficiency of a Lenoir engine having an<br />

air intake at 15.0°C and a combustion temperature of 2000.°C vs.<br />

the isentropic compression ratio over the range 1.01 ≤ CR ≤ 5.50.<br />

54. A Brayton cold ASC has a turbine isentropic efficiency of 92.0%<br />

and a compressor isentropic pressure ratio of 13.37. The<br />

compressor and turbine inlet temperatures are 500. and 2200. R,<br />

respectively. Determine the value of the compressor isentropic<br />

efficiency that causes the overall thermodynamic thermal<br />

efficiency of this system to be exactly zero.<br />

55. A Brayton cold ASC has a turbine that is 80.0% isentropically<br />

efficient and a compressor with an isentropic pressure ratio of<br />

7.00. The compressor inlet temperature is 530. R and the<br />

turbine inlet temperature is 2460 R. Determine the compressor<br />

isentropic efficiency that causes the entire cycle thermal<br />

efficiency to become exactly zero. Assume k=1.40.<br />

56. Show that the product of the compressor and turbine isentropic<br />

efficiencies must be greater than (T L /T H ) 1/2 if a Brayton cycle gas<br />

turbine unit is to operate at its maximum power output.<br />

57. A test on an open loop Brayton cycle gas turbine produced the<br />

following results:<br />

Net power output = 180:5hp<br />

Air mass flow rate = 20:0 × 10 3 lbm/h<br />

Inlet air temperature = 80:0°F<br />

Inlet air pressure = 14:5 psia<br />

Compressor exit pressure = 195 psia<br />

Compressor isentropic efficiency = 85:0%<br />

Combustion chamber heat addition = 4:00 × 10 6 Btu/h<br />

Using a cold ASC analysis and assuming k = 1.40, determine<br />

a. The cycle thermal efficiency.<br />

b. The isentropic efficiency of the turbine.<br />

58. On July 29, 1949, the first gas turbine installed in the<br />

United States for generating electric power went into service at<br />

the Belle Isle station of the Oklahoma Gas and Electric<br />

Company. 15 It had a 15-stage compressor with an isentropic<br />

pressure ratio of 6 to 1, a 2-stage turbine with overall entrance<br />

and exit temperatures of 1400°F and 780°F, respectively, and the<br />

turbine-generator unit was rated at 3500 kW. Assuming a<br />

Brayton cold ASC, determine<br />

a. The isentropic efficiency of the turbine.<br />

b. The Brayton cold ASC thermal efficiency of the entire<br />

turbine-compressor unit.<br />

59.* The regenerator in a Brayton cycle is simply a heat exchanger<br />

designed to transfer heat from hot exhaust gas to cool inlet<br />

gas. In an “ideal” regenerator, the exit temperature of the<br />

inlet (heated) gas is equal to the entrance temperature of the<br />

exhaust (cooled) gas. Since this is not normally the case in<br />

practice, regenerator (or heat exchanger) efficiency can be<br />

defined as<br />

η regeneration =<br />

ð _Q regeneration Þ actual ðh out − h in Þ<br />

=<br />

heated<br />

ð _Q regeneration Þ ðh in Þ maximum<br />

cooled<br />

− ðh in Þ heated<br />

possible<br />

and, for constant specific heats, this reduces to<br />

ðT out − T in Þ<br />

η regeneration =<br />

heated<br />

ðT in Þ coo1ed − ðT in Þ heated<br />

Note that regeneration is practical only when the engine<br />

exhaust temperature is greater than the compressor exhaust<br />

temperature. Therefore, as the compression and expansion<br />

ratios of the compressor and prime mover increase, the<br />

effectiveness of regeneration decreases. Determine an expression<br />

for the limiting isentropic pressure ratio (PR) in terms of T 1 , T 3 ,<br />

and k for which regeneration is no longer useful in the Brayton<br />

ASC with regeneration as shown in Figure 13.69. Evaluate this<br />

expression to find the limiting pressure ratio when T 1 = 1500.°C,<br />

T 3 = 10.0°C, and k=1.40.<br />

60.* An aircraft gas turbine engine operating on a Brayton cycle has a<br />

cold ASC thermal efficiency of 25.0% when the intake air is at<br />

20.0°C and the combustion chamber outlet temperature is at<br />

1200.°C. Assuming k=1.40, determine<br />

a. The isentropic pressure ratio of the engine.<br />

b. The isentropic compression ratio of the engine.<br />

c. The isentropic outlet temperature of the engine’s<br />

compressor.<br />

d. The optimum isentropic pressure ratio for maximum<br />

isentropic power output from the engine.<br />

e. The optimum isentropic compression ratio for maximum<br />

isentropic power output from the engine.<br />

f. The engine’s thermal efficiency when operated at the<br />

maximum isentropic power output.<br />

61. In Professor John L. Krohn’s laboratory at Arkansas Tech<br />

University, air enters the compressor of an ideal Brayton cycle<br />

at p 1 = 14.5 psi, T 1 = 70.0°F with a volumetric flow rate of<br />

20.0 × 10 3 ft 3 /min. The compressor pressure ratio is 12.0<br />

15 On November 8, 1984, the Belle Isle gas turbine was designated as the 73rd National Historic Mechanical <strong>Engineering</strong> Landmark by the American<br />

Society of Mechanical Engineers.

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