How Does Entropy Change in an Isothermal Compression of an Ideal Gas?

  • Thread starter Thread starter Nylex
  • Start date Start date
  • Tags Tags
    Entropy
AI Thread Summary
In an isothermal compression of 1 mol of an ideal gas at 400 K, the initial pressure is 100 kPa and the final pressure is 1000 kPa, with heat exchange occurring with a reservoir at 300 K. The entropy change for the gas can be calculated using the formula ΔS = nR ln(V2/V1), where the work done on the gas is equal to the heat removed from it due to the isothermal condition. The first law of thermodynamics indicates that the change in internal energy (ΔU) is zero, confirming that Qin equals the negative of the work done on the gas. The process is frictionless and maintains equilibrium throughout the compression. The next step involves calculating the entropy change for the reservoir, which also requires understanding the heat exchange dynamics during the process.
Nylex
Messages
552
Reaction score
2
Can anyone help me with this, please?

1. 1 mol of an ideal gas is compressed slowly and isothermally at 400 K in a piston-cylinder arrangement. Initial pressure = 100 kPa, final pressure 1000 kPa. The system is surrounded by a resevoir at 300 K such that heat exchange can take place between the piston-cylinder arrangement and the resevoir. System is isolated, so no heat exchange with outside world.

Calculate the entropy change of the gas, resevoir and universe if:

i. the piston is frictionless.

I'm stuck trying to do the entropy change for the gas. If I manage to do it, I should be able to do the rest.

I know delta S = INT dQ/T (haven't used tex before)

Also, from the 1st law: delta U = Qin + Won

For an isothermal change, delta U = 0 (as U depends on T only)

=> Qin = -Won

=> Qin = INT P dV

I'm not sure where to go from there, cos I can't put dQ = P dV in the integral above, can I (then substitute P = nRT/V, obviously)?
 
Physics news on Phys.org
Sure. It says in the excersize that the gas is compressed slowly and isothermally, so there always is an equilibrium. nRT/V can be put into the integral, making Q = nRT * INT (dV/V) from V1 to V2. (Which makes Q = nRT *ln(V2/V1).
Using relative volumes is enough here. Good luck!
 
Ok, thanks :).
 
I'm stuck again. How do I calculate the entropy change for the resevoir now?

1st law: delta U = Qin + Won

Won = 0, right? So delta U = Qin and I'm stuck :/.
 
Alright, you already showed us that delta U = 0, since it's an ideal gas. So Qin = -Won. In this case the Work on the gas is positive, the piston has to do work on the gas to compress it, so heat has to be removed from the gas, which follows fromthe formula.
Won = - INT P dV ---> so Qin = INT P dV = nRT * INT dV/V
So not Won = 0 but delta U = 0. This is because it's an isothermal process, which already suggests no change of internal energy (in the case of an ideal gas that is).
Now solve the integral and put relative values for V2 and V1 into it. There you go!
 
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
Back
Top