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Modern Engineering Thermodynamics

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Problems 93<br />

c. For a saturated mixture of liquid and vapor, explain whether<br />

or not the pressure and temperature can be varied<br />

independently.<br />

23. A vessel with a volume of 10.0 ft 3 contains 3.00 lbm of a<br />

mixture of liquid water and water vapor in equilibrium at a<br />

pressure of 100. psia (Figure 3.28). Determine<br />

a. The mass of liquid present.<br />

b. The mass of vapor present.<br />

c. Hydrogen gas is heated at a constant pressure of 0.00 psia<br />

from 0 to 5000.°F.<br />

d. Air is compressed from 0.00°F, 0.00 psia to 1000.°F, 5000.<br />

psia.<br />

34. Determine the changes in specific internal energy and specific<br />

enthalpy as air is compressed from 0.00°F, 14.7 psia to 1000.°F,<br />

5000. psia (Figure 3.29). Assume variable specific heat ideal gas<br />

behavior.<br />

p = 100. psia<br />

Total volume = 10.0 ft 3<br />

FIGURE 3.28<br />

Problem 23.<br />

Vapor<br />

Liquid<br />

Total mass of<br />

liquid + vapor = 3.00 lbm<br />

24.* Determine the change in the specific internal energy of 3.00 kg<br />

of graphite as it is heated at atmospheric pressure from 20.0 to<br />

200.°C. Assume a constant specific heat.<br />

25. Determine the change in the enthalpy of 5.00 lbm of ice as it is<br />

heated from 22.0 to 32.0°F under constant atmospheric<br />

pressure. Assume a constant specific heat.<br />

26.* Determine the change in the specific internal energy of solid<br />

aluminum as it is heated at atmospheric pressure from 300. to<br />

500. K. Use an average specific heat over this temperature range.<br />

27. Determine the change in the specific enthalpy of solid lead as it<br />

is heated from 14.7 psia, 80.0°F to 1000. psia, 200.°F. The<br />

density of lead is 710. lbm/ft 3 . Assume a constant specific heat.<br />

28. Determine the change in the specific internal energy of 7.00 lbm<br />

of methane gas as it is heated from 32.0 to 200.°F at<br />

atmospheric pressure. Assume ideal gas behavior.<br />

29.* Determine the change in the specific enthalpy of carbon dioxide<br />

gas as it is heated at a constant pressure of 1 atm from 300. to<br />

500. K. Assume ideal gas behavior.<br />

30.* Argon gas is heated in a constant pressure process from 20.0 to<br />

500.°C. Assuming ideal gas behavior, determine<br />

a. The ratio of the final to initial volumes.<br />

b. The change in specific internal energy.<br />

c. The change in specific enthalpy of the argon.<br />

31. Helium gas is heated in a constant volume process from −200.<br />

to 500.°F. Assuming ideal gas behavior, determine<br />

a. The ratio of the final to initial pressures.<br />

b. The change in specific internal energy.<br />

c. The change in specific enthalpy of the helium.<br />

32. Gaseous oxygen is heated in a constant temperature process<br />

until its volume is doubled. Assuming ideal gas behavior,<br />

determine<br />

a. The ratio of the final to initial pressures.<br />

b. The change in specific internal energy.<br />

c. The change in specific enthalpy of the oxygen.<br />

33. Using Figure 3.21, estimate the average values for the constant<br />

pressure and constant volume specific heats for the following<br />

gases and processes:<br />

a. Carbon dioxide is heated at a constant pressure of 10,000 psia<br />

from 1000. to 2000.°F.<br />

b. Carbon dioxide gas is compressed isothermally at 1000.°F<br />

from 0 to 10,000. psia.<br />

FIGURE 3.29<br />

Problem 34.<br />

T 1 = 0.00°F<br />

p 1 = 14.7 psia<br />

u 2 − u 1 = ?<br />

h 2 − h 1 = ?<br />

T 2 = 1000. °F<br />

p 2 = 5000. psia<br />

State 1 State 2<br />

35. Professor John L. Krohn at Arkansas Tech University invented a<br />

process whereby air is heated at constant volume from 60.0°F<br />

and v = 3.30 ft 3 /lbm to a pressure of 180. psi. The air then<br />

expands adiabatically to atmospheric pressure and v = 14.6 ft 3 /<br />

lbm. Assuming ideal gas behavior with variable specific heat,<br />

determine<br />

a. The temperature of the heated air (T 2 )in°F.<br />

b. The heat transfer for the first process in Btu/lbm.<br />

c. The work for the second process in Btu/lbm,<br />

36. Professor Krohn uses the constant pressure specific heat<br />

equation for water vapor given in by c p = A(B + CT + DT 2 +<br />

ET 3 + FT 4 ), where A = 0.1102 Btu/lbm · R, B = 4.070,<br />

C = −0.000616 R −1 , D = 1.281 × 10 −6 R −2 , E = −0.508 × 10 −9<br />

R −3 , F = 0.0769 × 10 −12 R −4 , and T is in Rankine (R). He wants<br />

you to estimate the change in enthalpy for water vapor from<br />

p 1 = 14.7 psi, T 1 = 250.°F top 2 = 14.7 psi, T 2 = 500.°F, and<br />

compare this result to the change in enthalpy found in the<br />

superheated steam tables.<br />

37.* In 1879, the French physicist Emile Amagat generated<br />

experimental data in a mine shaft at Verpilleux, France, for his<br />

research on the compressibility of gases. There, he used a vertical<br />

column of mercury 327 m high to measure the compressibility<br />

of nitrogen at a pressure of 430. atm. Assuming the temperature<br />

at the bottom of the mine shaft was 30.0°C, determine the<br />

specific volume of the nitrogen, assuming it is an ideal gas with<br />

constant specific heats.<br />

38.* Calculate the specific volume of hydrogen (H 2 ) gas at a<br />

temperature of 20.0°C and a pressure of 11.0 MPa using<br />

a. The ideal gas equation of state.<br />

b. The Clausius equation of state (use the van der Waals value<br />

for b).<br />

39. Determine the temperature of water vapor at 200. psia when it<br />

has a specific volume of 2.724 ft 3 /lbm using<br />

a. The ideal gas equation of state.<br />

b. The van der Waals equation of state.<br />

c. The steam tables (Table C.3a).<br />

Then compute the percentage error of a and b with the actual<br />

value given in c.

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