Using the first law of thermodynamics:
\[\Delta Q = \Delta U + W\]
\[31\]
Given:
\[+48 = n C_V \Delta T + W\]
For helium (a monoatomic gas), \( C_V = \frac{3R}{2} \):
\[48 = (1) \left( \frac{3R}{2} \right) (2) + W\]
Simplifying:
\[W = 48 - 3 \times R\]
Substitute \( R = 8.3 \):
\[W = 48 - 3 \times (8.3)\]
\[W = 23.1 \, \text{Joule}\]
List-I | List-II | ||
(A) | Isothermal process | (I) | No heat exchange |
(B) | Isochoric process | (II) | Carried out at constant temperature |
(C) | Isobaric process | (III) | Carried out at constant volume |
(D) | Adiabatic process | (IV) | Carried out at constant pressure |