Isothermal Compression of a Diatomic Gas: Calculating Work, Heat Flow, and Final Pressure , Assignments of Physics

A solution to problem 4 in physics 213, week 2, where one and one-half moles of a diatomic gas undergo isothermal compression from a volume of 0.015 m3 to 0.0015 m3. How to sketch the process on a pv diagram, calculate the work done on the gas, determine the heat flow into the gas, and find the final pressure of the gas using the ideal gas equation of state.

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Solution
Physics 213 Problem 4 Week 2
Isothermal Compression
a) One and one-half moles of a diatomic gas at temperature 35oC are compressed isothermally
from a volume of 0.015 m3 to a volume of 0.0015 m3. Sketch the process on a pV diagram
and show what corresponds to the work done on the gas. Calculate the work done on the gas.
(Ignore vibrational energy of the molecules.)
The figure above shows the path along which the gas is compressed from the initial state to the
final state. The path is an isotherm. The equation of state of an ideal gas is p = nRT/V. The
differential of the work done by the gas is dW = pdV. Substituting for p, we obtain dW =
(nRT/V) dV. Since the temperature, T, is constant (isothermal process), we can integrate the
work from the initial to the final volume. Note that the work done by the gas is the negative of
the work done on the gas: Wby = Won.
Won =−Wby =− pdV
Vi
Vf
=−nRT dV
V=nRTln Vi
Vf
Vi
Vf
Won = = (1.5 mol) (8.314 J / mol·K) (273 K + 35 K) ln(0.015 m3/ 0.0015 m3) = 8844 J
Positive work is done on the gas.
Note that we did the integral for Wby by substituting nRT/V for p and took the factor nRT out of
the integral sign. This procedure is correct only for isothermal (T = constant) processes. Had
the process been, for example, isobaric (constant pressure), we would have simply brought p out
of the integral and found that Wby = p (Vf Vi). The point is that the way we do the integral
varies with the nature of the process. Wby = nRT ln(Vf / Vi) for isothermal processes only.
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Solution

Physics 213 Problem 4 Week 2 Isothermal Compression

a) One and one-half moles of a diatomic gas at temperature 35oC are compressed isothermally from a volume of 0.015 m^3 to a volume of 0.0015 m^3. Sketch the process on a pV diagram and show what corresponds to the work done on the gas. Calculate the work done on the gas. (Ignore vibrational energy of the molecules.)

The figure above shows the path along which the gas is compressed from the initial state to the final state. The path is an isotherm. The equation of state of an ideal gas is p = nRT/V. The differential of the work done by the gas is dW = pdV. Substituting for p, we obtain dW = (nRT/V) dV. Since the temperature, T, is constant (isothermal process), we can integrate the work from the initial to the final volume. Note that the work done by the gas is the negative of the work done on the gas: Wby = − Won.

W (^) on = − W (^) by = − pdV Vi

V (^) f ∫ = − nRT^

dV V

= nRT ln Vi V (^) f

Vi

V (^) f

W on = = (1.5 mol) (8.314 J / mol·K) (273 K + 35 K) ln(0.015 m^3 / 0.0015 m^3 ) = 8844 J

Positive work is done on the gas.

Note that we did the integral for Wby by substituting nRT/V for p and took the factor nRT out of the integral sign. This procedure is correct only for isothermal (T = constant) processes. Had the process been, for example, isobaric (constant pressure), we would have simply brought p out of the integral and found that Wby = p (Vf − Vi). The point is that the way we do the integral varies with the nature of the process. Wby = nRT ln(Vf / Vi) for isothermal processes only.

b) How much heat flowed into the gas?

Use the First Law and the fact that U = U(T) for ideal gases.

∆U = Qin + Won = Qin − Wby

∆U = 0 since T = constant.

0 = Qin − Wby

Qin = Wby = − 8844 J

Note that ∆U = 0 since the temperature did not change and that for an ideal gas, the internal energy depends only on T. Heat flows out of the gas.

c) What is the final pressure of the gas?

p = nRT/V = (1.5 mol) × (8.314 J / mol·K) × (273 K + 35 K) / (0.0015 m^3 ) = 2.56 × 106 Pa

The initial pressure can also be found from the equation of state.

p = nRT/V = (1.5 mol) × (8.314 J / mol·K) × (273 K + 35 K) / (0.015 m^3 ) = 2.56 × 105 Pa

The pressure has increased by a factor of ten while the volume has decreased by a factor of ten. The product pressure times volume is constant, since T is constant.