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

  • A
    $\frac{1}{3}\rho\bar{c}^2$
  • B
    $\frac{1}{3}\rho(\bar{c} + v)^2$
  • C
    $\frac{1}{3}\rho(\bar{c} - v)^2$
  • D
    $\frac{1}{3}\rho(\bar{c}^{-2} - v)^2$

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