OUNT OF HEAT THAT FLOWS DURING THE EXPANSION

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The discussion revolves around calculating various parameters of a monotonic ideal gas undergoing an isothermal expansion. The initial pressure P1 is calculated to be 2680 Pa using the ideal gas law. The work done by the gas during the expansion is 9.7 kJ, and the first law of thermodynamics is applied to find the heat flow, Q, which equals -W due to the constant temperature condition. There is some confusion regarding the convention of work done by the gas versus work done on the gas, which is clarified throughout the discussion. The participants emphasize the importance of maintaining correct sign conventions when applying thermodynamic equations.
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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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