
To match the columns and find the correct numerical values, we will need to analyze each item in Column-I and relate it to the appropriate value from Column-II using the properties of gases and their specific heat capacities.
For a monatomic ideal gas, such as helium or argon, the change in internal energy (ΔU) is given by:
\(ΔU = \frac{3}{2}nRΔT\).
Since the gas is undergoing a change involving 1 mole, we have:
\(ΔU = 1 \times \frac{3}{2}RΔT = \frac{3}{2}RΔT.\)
Matching this with options, we find (R) 480R fits as it aligns with the calculated form: (A) → R.
For heat supplied to a gas, the formula is:
\(Q = nC_vΔT\) for constant volume.
For an ideal diatomic gas:
\(C_v = \frac{5}{2}R\).
Thus,
\(Q = 2 \times \frac{5}{2}RΔT = 5RΔT.\)
So, option (P) 650R is a match: (B) → P.
For diatomic gases, internal energy change is:
\(ΔU = \frac{5}{2}nRΔT.\)
When n = 1, it is simply:
\(ΔU = \frac{5}{2}RΔT.\)
Matching with options, (Q) 800R matches the proportionality: (C) → Q.
Thus, the correct matching is: A → R; B → P; C → Q.