Step 1: First law of thermodynamics.
From the first law of thermodynamics, we know:
\[
\Delta Q = \Delta U + \Delta W
\]
For a diatomic gas at constant pressure:
\[
\Delta Q = n C_p \Delta T
\]
\[
\Delta U = n C_v \Delta T
\]
\[
\Delta W = p \Delta V = n R \Delta T
\]
Where:
- \( C_p \) and \( C_v \) are the specific heats at constant pressure and volume, respectively.
- For a diatomic gas, \( C_p = \frac{7}{5} R \) and \( C_v = \frac{5}{3} R \).
Step 2: Applying the relation.
We know that:
\[
\Delta W : \Delta U : \Delta Q = 2 : 5 : 7
\]
Thus, the correct answer is (C) 2:5:7.