$A$ vessel of volume $V \ L$ contains an ideal gas at $T \ K$. The vessel is partitioned into two equal parts. The volume (in $L$) and temperature (in $K$) in each part is respectively
- A$V, \frac{T}{2}$
- B$\frac{V}{2}, T$
- C$V, T$
- D$\frac{V}{2}, \frac{T}{2}$
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