Consider an ideal gas confined in an isolated closed chamber. As the gas undergoes an adiabatic expansion, the average time of collision between molecules increase as `V^q`, where V is the volume of the gas. The value of q is : `(gamma=(C_p)/(C_v))`
A. `(gamma+1)/(2)`
B. `(gamma-1)/(2)`
C. `(3gamma+5)/(6)`
D. `(3gamma-5)/(6)`