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Modern Engineering Thermodynamics

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Problems 165<br />

where v, T, and r are the specific volume, temperature, and<br />

radius of the star.<br />

a. Show that the collapse process is a polytropic process with<br />

n = 4/3.<br />

b. Beginning with the per unit mass differential form of the<br />

first law, find an expression for the star’s heat transfer as a<br />

function of its specific heats and temperature. Note that the<br />

star does p V work on itself as it collapses.<br />

c. Using the expression found in part b, along with c v =<br />

0.200 Btu/(lbm · R) and k = 1.4, calculate the amount of<br />

heat transfer per unit mass of star as its temperature changes<br />

from 5000. to 10,000. R.<br />

d. Explain the critical condition that exists when the specific<br />

heat ratio k takes on the value of 4/3.<br />

Computer Problems<br />

The following computer problems are designed to be completed<br />

using a spreadsheet or equation solver. They may be used as part of a<br />

weekly homework assignment.<br />

57. Develop a computer program that performs an energy balance on<br />

a closed system containing an incompressible substance (either a<br />

liquid or a solid). Include the following input (in proper units):<br />

the heat and work transports of energy, the system volume, the<br />

initial temperature of the system, and the density and specific<br />

heat of the incompressible material contained in the system.<br />

Output to the screen the system mass and final temperature.<br />

58. Develop a computer program that performs an energy balance on a<br />

closed system containing an ideal gas with constant specific heats.<br />

Include the following input (in proper units): the heat and work<br />

transports of energy, the system volume, the initial temperature<br />

and pressure of the system, and the constant volume specific heat<br />

and gas constant of the gas contained in the system. Output to the<br />

screen the system mass and the final pressure and temperature.<br />

59. Repeat Problem 58, except allow the user to choose the system<br />

ideal gas from a screen menu, and omit the prompts for gas<br />

properties. Use the data in Table C.13 of Thermodynamic Tables to<br />

accompany <strong>Modern</strong> <strong>Engineering</strong> <strong>Thermodynamics</strong> for the properties<br />

of the gases in your menu.<br />

60. Develop a computer program that generates data to allow you<br />

to plot on the computer the explosive energy contained in a<br />

1000. ft 3 pressure vessel containing compressed air vs.<br />

a. The vessel’s initial temperature when the initial pressure is<br />

held constant at 100. psia.<br />

b. The vessel’s initial pressure when the initial temperature is<br />

held constant at 80.0°F.<br />

c. Create a three-dimensional plot with the explosive energy on<br />

the vertical axis and the initial pressure and initial<br />

temperature on the horizontal axes.<br />

Assume the final temperature and pressure of the air after the<br />

vessel has ruptured are 70.0°F and14.7psiaineachcaseand<br />

that the air undergoes a polytropic decompression process<br />

with n = 1.25 when the vessel ruptures. Also assume that<br />

the air behaves as a constant specific heat ideal gas with<br />

k =1.40.<br />

61. A white dwarf is a spherical mass of gas in outer space. Its radial<br />

pressure gradient must always be in equilibrium with its own<br />

gravitational force field, or<br />

dp<br />

dr = − Gmρ/r2<br />

where G is the gravitational constant, ρ is the density of the gas<br />

at radius r (i.e., ρ = ρ(r)), and m is the mass of gas inside a<br />

sphere of radius r,<br />

m = 4π<br />

Z r<br />

0<br />

ρr 2 dr<br />

During its formation, the gas of a white dwarf obeys the<br />

polytropic equation<br />

pv −5/3 = α = constant<br />

These relations can be combined to yield a differential equation<br />

for the density field ρ = ρ(r) inside a white dwarf of the form<br />

d 2 ϕ<br />

dx 2 + 2 <br />

dϕ<br />

+ ϕ 2/3 = 0<br />

x dx<br />

where ϕ = ðρ/ρ 0 Þ 2/3 , ρ 0 = ρ(r = 0), and x = r/r*, where<br />

r = 5α/ 8πGρ 1/3<br />

0 .<br />

a. Solve the preceding differential equation for ϕ(x) using a<br />

computer numerical solution with the boundary conditions<br />

ϕ = 1 and dϕ/dx =0atx = 0 to show that ϕ(x) =0at<br />

x = 3.6537.<br />

b. Show that ϕ(x) = 0 corresponds to the radius R of the white<br />

dwarf and a white dwarf therefore has a mass m given by<br />

m = − 45:91ρ 0 ðr Þ 3 ðdϕ/dxÞj x=R .

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