To find the heat given to a diatomic gas that undergoes isobaric expansion, we use the first law of thermodynamics, which is expressed as:
ΔQ = ΔU + W
where:
ΔQ is the heat added to the system,
ΔU is the change in internal energy, and
W is the work done by the system.
Given, W = 100 J and the specific heat ratio γ = 1.4 for a diatomic gas, the relationship between the molar heat capacities is:
Cp = γCv
For an isobaric process, Cp is used, and ΔU for a diatomic gas is:
ΔU = nCvΔT
We know:
Cv = R/(γ-1)
For diatomic gases, Cv = (5R/2) and Cp = (7R/2), hence:
ΔU = (5R/2)ΔT and
W (At constant pressure) = nRΔT
For the work done, 100 J = nRΔT
Therefore, we rewrite ΔU:
ΔU = (5/2)(100 J)/(RΔT)/nR = (5/2) × 100
Now back to:
ΔQ = (5/2) × 100 + 100 = 250 + 100 = 350 J
Conclusively, the heat given to the gas is 350 J, which fits perfectly within the expected range of 350 to 350 J.