OUNT OF HEAT THAT FLOWS DURING THE EXPANSION

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SUMMARY

The discussion focuses on the isothermal expansion of a monatomic ideal gas, specifically 3 moles at a temperature of 50 degrees Celsius. The gas performs 9.7 kJ of work during the expansion. The calculations reveal that the initial pressure P1 is 2680 Pa, and the relationship between the volumes and pressures during the expansion is governed by the equation W = nRTln(V2/V1). The heat flow Q during the expansion is determined using the first law of thermodynamics, where Q = -W, confirming that heat flows into the gas as it expands.

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coffeem
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Homework Statement
3 Moles of a monotomatic ideal gas undergo an isothermal (T=50 Degrees Clecius) reversible expansion from a volume of 3m^3 and a pressure P1 to a volume V2 and a pressure P2. The gas does 9.7kJ of work in the expansion. Find:

a) the pressure P1
b) The volume V2
c) The pressure P2
d) The amound of heat that flows during the expansion

The attempt at a solution

My attempt is as follows:

n = 3
T = 323K
V1 = 3m^3

a) P1V1 = nRT

rearanging:

P1 = 2680Pa

b) I am slightly more stuck on:

for an isothermal expansion: dW = -PdV
by subbing into the ideal gas eq" of state:

W = nRTln(V1/V2)

Now since change in T = 0, therefore the chance in E = 0.

and first law of thermodynamics: E = Q +W
therefore Q = -W

so Can i just rearrange with this to find V2 from the expression for work? thanks
 
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Yes, but take care, the work done by the gas is given, and you wrote the formula for the external work, done on the gas.

ehild
 
coffeem said:
for an isothermal expansion: dW = -PdV
In this case, dW would be the work done ON the gas. The convention is to use W to represent work done BY the gas, in which case dW = PdV. Note: this is true for any process, not just isothermal.
by subbing into the ideal gas eq" of state:

W = nRTln(V1/V2)
This is true only if the process is isothermal (constant T). Again, you are using W as the work done on the gas which is not the conventional way to express W. W = nRTln(V2/V1) gives youi the work done BY the gas.
Now since change in T = 0, therefore the change in E = 0.

and first law of thermodynamics: E = Q +W
therefore Q = -W
Again, you should use the convention for W as the work done BY the gas. Q = E (or U) + W or E = Q - W where W is the work done BY the gas and Q is the heat flow INTO the gas.

so Can i just rearrange with this to find V2 from the expression for work? thanks
Yes. But keep the signs straight. (Use Q = W = \int PdV = nRT\ln{(V_2/V_1)}).

AM
 

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