139307 A perfect gas of ' $N$ ' molecules, each of mass ' $m$ ', moving with velocities ' $C_{1}$ ', ' $C_{2}$ ', ' $\mathrm{C}$ $\mathrm{N}$ ' is enclosed in a cubical vessel of volume ' $\mathrm{V}$ '. The pressure exerted by the gas on the walls of the vessel is (' $\rho$ ' = density of gas)
139307 A perfect gas of ' $N$ ' molecules, each of mass ' $m$ ', moving with velocities ' $C_{1}$ ', ' $C_{2}$ ', ' $\mathrm{C}$ $\mathrm{N}$ ' is enclosed in a cubical vessel of volume ' $\mathrm{V}$ '. The pressure exerted by the gas on the walls of the vessel is (' $\rho$ ' = density of gas)
139307 A perfect gas of ' $N$ ' molecules, each of mass ' $m$ ', moving with velocities ' $C_{1}$ ', ' $C_{2}$ ', ' $\mathrm{C}$ $\mathrm{N}$ ' is enclosed in a cubical vessel of volume ' $\mathrm{V}$ '. The pressure exerted by the gas on the walls of the vessel is (' $\rho$ ' = density of gas)
139307 A perfect gas of ' $N$ ' molecules, each of mass ' $m$ ', moving with velocities ' $C_{1}$ ', ' $C_{2}$ ', ' $\mathrm{C}$ $\mathrm{N}$ ' is enclosed in a cubical vessel of volume ' $\mathrm{V}$ '. The pressure exerted by the gas on the walls of the vessel is (' $\rho$ ' = density of gas)