Change In Internal Energy Of An Ideal Gas

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An ideal gas is compressed from 4.50 L to 3.00 L at a constant temperature of 295 K, with work done on the gas calculated as 2.5 kJ. The change in internal energy of the gas is determined to be zero since the gas remains in thermal contact with a heat reservoir, maintaining a constant temperature. Consequently, the thermal energy exchanged between the gas and the reservoir equals the work done, also 2.5 kJ. The discussion highlights the importance of understanding the relationship between work, heat transfer, and internal energy in thermodynamic processes. The key takeaway is that when an ideal gas is compressed isothermally, its internal energy does not change.
Searay330
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An ideal gas is compressed from a volume of Vi = 4.50 L to a volume of Vf = 3.00 L while in thermal contact with a heat reservoir at T = 295 K as in the figure below. During the compression process, the piston moves down a distance of d = 0.120 m under the action of an average external force of F = 21.0 kN.

(a) Find the work done on the gas, I Solved That its 2.5KJ.

ideal gas is PV = nRt
work done is W = F(yf - yi)
so work is W = 21000N*(.120m)
W = 2520J or 2.5 KJ(b) Find the change in internal energy of the gas.

(c) Find the thermal energy exchanged between the gas and the reservoir.

i tried to solve b and c but with no pressure or moles i have no formula that can get me the change in internal energy.

for b the change is internal energy is given by: U = Q + W
i have the W as 2.5kJ but i am still Missing Q the energy transferred to the Gas by Heat
 
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Don't you have an equation for the internal energy of an ideal gas?
 
DrClaude said:
Don't you have an equation for the internal energy of an ideal gas?
yes its (3/2)nR(tf - ti)
but i don't have moles and i can't get them from the ideal gas law because i don't have the pressure
and i can't get it from the W = PAChangeinY because i don't have A
 
I had missed that you didn't have the number of moles. Could you make some assumption, like that the system is initially at atmospheric pressure?
 
DrClaude said:
I had missed that you didn't have the number of moles. Could you make some assumption, like that the system is initially at atmospheric pressure?
im not sure that is the whole question but for the sake of learning to do this problem i can

so if i assume that the pressure is 101325PA then
101325PA * .0045 m3 = n8.31T where t is still unknown
 
Searay330 said:
where t is still unknown
Searay330 said:
while in thermal contact with a heat reservoir at T = 295 K
 
so because it is contact with the heat reservoir it can be assumed that it is at the temperature always?
 
Searay330 said:
so because it is contact with the heat reservoir it can be assumed that it is at the temperature always?
Yes. That's in essence the definition of a "reservoir."
 
so that means that 101325PA * .0045 m3 = n8.31(273K)
gives n = .185
then (3/2)(.185)*8.31*295 = 683.94
but because the temperature never changes does that still hold ?
allowing me to solve it all again with vf and then subtract both finding the answer
 
  • #10
Sorry, I'm slow tonight. I just realized that you are asked for the change in internal energy. So what happens when you calculate ΔU = (3/2)nR(Tf- Ti)? Hint: you don't need to know n.
 
  • #11
i am not sure because if it is contact with the heat reservoir that would that mean that temperature doesn't change and it would be 0
 
  • #12
Searay330 said:
i am not sure because if it is contact with the heat reservoir that would temperature doesn't change and it would be 0
Exactly, the internal energy of the gas doesn't change.
 
  • #13
Right so if the internal energy doesn't change that means that for part c Q = W or 2.5KJ

Thank you very much for your help
 
  • #14
Searay330 said:
Right so if the internal energy doesn't change that means that for part c Q = W or 2.5KJ

Thank you very much for your help
Your welcome. And sorry again, that should've been quicker.
 
  • #15
Searay330 said:
so because it is contact with the heat reservoir it can be assumed that it is at the temperature always?
Not exactly. It means that the temperature of the gas in the final thermodynamic equilibrium state of the system (295) is the same as in the initial thermodynamic equilibrium state of the system (295). During the transition from the initial thermodynamic equilibrium state to the final thermodynamic equilibrium state, the temperature of the gas does not have to be uniform at 295 throughout. In fact, even the average temperature of the gas can differ from 295 during the transition.

Chet
 
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