For an ideal gas, the relation between the heat capacities at constant pressure (\(C_P\)) and constant volume (\(C_V\)) is given by: \[ C_P - C_V = R \] where \( R \) is the universal gas constant. Therefore, the correct relation between \( C_P \) and \( C_V \) is: \[ C_P = C_V + R \]
The correct option is (B) : \(C_p=C_v+R\)
For one mole of an ideal gas, the correct relation between the molar specific heats at constant pressure (Cp) and constant volume (Cv) is given by the equation: Cp = Cv + R Where R is the universal gas constant. This is derived from the first law of thermodynamics and the definitions of specific heat capacities.
A piston of mass M is hung from a massless spring whose restoring force law goes as F = -kx, where k is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature T) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $ L_0 $ to $ L_1 $, the total energy delivered by the filament is (Assume spring to be in its natural length before heating) 