- #1
Jeremy1789
- 2
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I'm struggling to understand a concept which I assume is basic, but I can't seem to fit the pieces together. When speaking about an ideal gas, I understand that
ΔH = ΔU + Δ(PV) = ΔU + RΔT
So far so good. I also understand the relationship:
ΔU = Q + W... (W here is work being done on the system)
In an adiabatic reversible process, Q = 0, which also makes sense. So,
W = ΔU = nCvΔT
Now, where my confusion lies is in the next part. My book works out a problem, and says:
ΔH = W = nCpΔT
How can both ΔU and ΔH equal W? This doesn't make sense to me, unless Δ(PV) from the first equation was 0. I don't see how this could be 0 unless we were talking about an isothermal case. It also doesn't make sense because W can't equal both nCvΔT and nCpΔT simultaneously, since Cp = Cv + R.
Am I missing something?
ΔH = ΔU + Δ(PV) = ΔU + RΔT
So far so good. I also understand the relationship:
ΔU = Q + W... (W here is work being done on the system)
In an adiabatic reversible process, Q = 0, which also makes sense. So,
W = ΔU = nCvΔT
Now, where my confusion lies is in the next part. My book works out a problem, and says:
ΔH = W = nCpΔT
How can both ΔU and ΔH equal W? This doesn't make sense to me, unless Δ(PV) from the first equation was 0. I don't see how this could be 0 unless we were talking about an isothermal case. It also doesn't make sense because W can't equal both nCvΔT and nCpΔT simultaneously, since Cp = Cv + R.
Am I missing something?