I agree, that in order to have an Enthalpy of Rxn a temperature change needs to be measurable. However, if the process is adiabatic with an isothermal phase transition (that is, ΔH = 0) application of the system given to the 1st Law gives ΔU = ΔH - PΔV = (0) - PΔV = - PΔV = work done by the system on surroundings or surroundings on the system. For ΔV > 0 => Expansion Process => Exothermic Work or, ΔV < 0 => Compression Process => Endothermic Work. So while it is true ΔH in this case would be zero, the work done by the surroundings on the system would not be zero, and (in my humble opinion) 'work' would be the objective value in the problem.
So, from the posted problem, I see an adiabatic compression of 2 moles of N
2(g) at 1bar pressure (~1 atm) to 2 moles of N
2(g) at 200 bar (~200 atm). Such a compression would most likely drive the N
2(g-phase) => N
2(l-phase) and would transition via adiabatic process (where enthalpy, ΔH = 0) and demonstrate a '0' temperature change. This condition warrants use of the expression defining 'Heat of Condensation/Vaporization for N
2. That is ΔU
g/l = ΔH
g/l transition = mass of N
2 x ΔH
t, and ΔH
t = published phase transition constant for N
2. From Wiki (
https://en.wikipedia.org/wiki/Nitrogen), ΔH
v(N
2) = 5.56 Kj/mole. So, for 2 moles molecular nitrogen = 2 Molar Volumes (2V
mN
2) undergoing phase transition (g →l) due to compression process => ΔU = ΔH - (- Work by Compression*) = ΔU = ΔH + (Work by Compression*) => ...
* Work by Compression => Work done by the surroundings on the system => 'Endothermic' to the System. => Work = PΔV = P(V
final - V
initial) => Work = P(0V
m - 2V
m) = - 2V
m. Substituting into ΔU = ΔH - (P(-2V
m) = ΔH + 2PΔV = ΔH + (Work done on system by compression) = (ΔH) + (m⋅ΔH
v) = (0) + (2 moles N
2)(5.56 Kj/mole) = + 11.12 Kj.