Consider a gas with density \[\rho \] and \[\overline{c}\] as the root mean square velocity of its molecules contained in a volume. If the system moves as whole with velocity, then the pressure exerted by the gas is

\[\frac{1}{3}\rho {{\left( c+\nu \right)}^{2}}\]

\[\frac{1}{3}\rho {{\bar{c}}^{2}}\]

\[\frac{1}{3}\rho {{\left( \bar{c}-\nu \right)}^{2}}\]

\[\frac{1}{3}\rho {{\left( {{{\bar{c}}}^{2}}-\nu \right)}^{2}}\]

Consider a gas with density \[\rho \] and \[\overline{c}\] as the root

1.	Consider a gas with density \[\rho \] and \[\overline{c}\] as the root mean square velocity of its molecules contained in a volume. If the system moves as whole with velocity, then the pressure exerted by the gas is
A.	\[\frac{1}{3}\rho {{\bar{c}}^{2}}\]
B.	\[\frac{1}{3}\rho {{\left( c+\nu \right)}^{2}}\]
C.	\[\frac{1}{3}\rho {{\left( \bar{c}-\nu \right)}^{2}}\]
D.	\[\frac{1}{3}\rho {{\left( {{{\bar{c}}}^{2}}-\nu \right)}^{2}}\]
Answer» B. \[\frac{1}{3}\rho {{\left( c+\nu \right)}^{2}}\]