N molecules , each of mass m, of gas A and 2 N molecules , each of mass 2m, of gas B are contained in the same vessel which is maintained at a temperature T. The mean square velocity of molecules of B type is denoted by ` V_(2)` and the mean square velocity of A type is denoted by `V_(1)` then `(V_(1))/(V_(2))` is

N molecules, each of mass m of gas A and 2 N molecules each of mass 2m of gas B are containted in the same vessel which is maintained at temperature T. The mean square velocity of molecules of B type is denoted by v^(2) and the mean square velocity of A type is denoted by (omega)^(2) . the omega^(2)//v^(2) is:

N molecules each of mass m of gas A and 2 N molecules each of mass 2m of gas B are contained in the same vessel which is maintined at a temperature T. The mean square of the velocity of the molecules of B type is denoted by v^(2) and the mean square of the x-component of the velocity of a tye is denoted by omega^(2) . What is the ratio of omega^(2)//v^(2) = ?

N molecules each of mass m of gas A and 2 N molecules each of mass 2m of gas B are contained in the same vessel which is maintined at a temperature T. The mean square of the velocity of the molecules of B type is denoted by v^(2) and the mean square of the x-component of the velocity of a tye is denoted by omega^(2) . What is the ratio of omega^(2)//v^(2) = ?

2N molecules of an ideal gas X, each of mass m, and 4N molecules of another ideal gas, Y, each of mass 3m are maintained at the same absolute temperature in the same vessel. The root mean square speed of molecules of X type is v and the root mean square of the component of velocity of molecules of gas Y, along the X axis is u, then v : u ​ is

At a given temperature if V_(rms) is the root mean square velocity of the molecules of a gas and V_(s) be the velocity of sound in it, then these are related as (gamma=(C_(p))/(C_(v)))