360221 Consider an ideal gas confined in an isolated closed chamber. As the gas undergoes an adiabatic expansion the average time of collision between molecules increases as \(V^{q}\), where \(V\) is the volume of the gas. The value of \(q\) is : \(\left( {\gamma = \frac{{{C_p}}}{{{C_v}}}} \right)\)
360221 Consider an ideal gas confined in an isolated closed chamber. As the gas undergoes an adiabatic expansion the average time of collision between molecules increases as \(V^{q}\), where \(V\) is the volume of the gas. The value of \(q\) is : \(\left( {\gamma = \frac{{{C_p}}}{{{C_v}}}} \right)\)
360221 Consider an ideal gas confined in an isolated closed chamber. As the gas undergoes an adiabatic expansion the average time of collision between molecules increases as \(V^{q}\), where \(V\) is the volume of the gas. The value of \(q\) is : \(\left( {\gamma = \frac{{{C_p}}}{{{C_v}}}} \right)\)
360221 Consider an ideal gas confined in an isolated closed chamber. As the gas undergoes an adiabatic expansion the average time of collision between molecules increases as \(V^{q}\), where \(V\) is the volume of the gas. The value of \(q\) is : \(\left( {\gamma = \frac{{{C_p}}}{{{C_v}}}} \right)\)