Entropy-Isobaric Expansion of a gas to thermal equilibrium

AI Thread Summary
An ideal gas undergoes isobaric expansion, doubling its volume while reaching thermal equilibrium with a heat bath. The internal energy is given by U=3/2RT, and the change in entropy can be calculated using the equation ΔS = ∫dQ/T. To find the change in entropy for the gas, the temperature change must first be determined, followed by evaluating the integral for the gas's heat flow. The entropy change of the surroundings is equal and opposite to that of the gas, and the total change in entropy for the universe is the sum of both changes.
TheTourist
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One mole of an ideal gas undergoes an isobaric expansion to reach thermal equilibrium with a surrounding heat bath. In doing so, it expands by a factor of two in volume. The internal energy of the gas is described by, U=3/2RT.
Calculate the resulting change in entropy of the gas, the heat bath, and the Universe.

Homework Equations



\deltaS=\frac{delta Q}{T}

I understand all the theory behind this, I just can't seem to derive an equation which would allow me to obtain an answer with the information given, I always seem the need a temperature. I have tried using the above equations for U and delta S, and using the 1st of law of thermodynamics, but can't seem to get anywhere.

Thanks
 
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TheTourist said:
One mole of an ideal gas undergoes an isobaric expansion to reach thermal equilibrium with a surrounding heat bath. In doing so, it expands by a factor of two in volume. The internal energy of the gas is described by, U=3/2RT.
Calculate the resulting change in entropy of the gas, the heat bath, and the Universe.


Homework Equations



\deltaS=\frac{delta Q}{T}

I understand all the theory behind this, I just can't seem to derive an equation which would allow me to obtain an answer with the information given, I always seem the need a temperature. I have tried using the above equations for U and delta S, and using the 1st of law of thermodynamics, but can't seem to get anywhere.

Thanks
The change in entropy is:

\Delta S = \int_{rev} dQ/T

The reversible path is one in which external pressure remains constant and heat flows reversibly from the surroundings to the gas (eg. via a Carnot heat engine/pump). dQ = CpdT. So the change in entropy of the gas is:

\Delta S = \int_{rev} C_pdT/T

For the surroundings, which remain at constant temperature, the heat flow is equal and opposite to the heat flow into the gas:

\Delta S = -\Delta Q/T_{surr} = -\frac{1}{T_{surr}\int_{rev}C_pdT_{gas}

You just have to work out the change in temperature of the gas.

AM
 
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I have this exact question to do for tomorrow. I don't understand what this question is asking. Is there any more steps to the solution that what you have already provided?
Thanks
 
Deadlyhedley said:
I have this exact question to do for tomorrow. I don't understand what this question is asking. Is there any more steps to the solution that what you have already provided?
Thanks
First you work out the temperature change.

Then you evaluate the integral \int_{T_i}^{T_f} dQ/T for the gas. That gives you the change in entropy of the gas.

Then you evaluate Q_{surr}/T_{surr} = -Q_{gas}/T_{surr} to determine the change in entropy of the surroundings.

Then you add them together to get the change in entropy of the universe.

AM
 
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