\(\frac{2}{T}\)
\(\frac{3}{T}\)
\(\frac{1}{2T}\)
\(\frac{1}{T}\)
Given:
\[ \frac{dV}{V} = \alpha \frac{dT}{T} \]
For a constant \( P T^2 \), we have:
\[ \frac{dV}{dT} = \left( C \right) \frac{3}{T^2} \]
So, the volume expansion coefficient is:
\[ \frac{dV}{V} = \frac{3}{T^2} \cdot dT \]
List - I | List -II | ||
---|---|---|---|
a | Isothermal | i | Pressure constant |
b | Isobaric | ii | Temperature constant |
c | Adiabatic | iii | Volume constant |
d | Isobaric | iv | Heat content is constant |