Concept:
- At the molecular level, the average kinetic energy of a gas molecule depends only on the absolute temperature, not on the identity of the gas: $\dfrac{1}{2}mv_{rms}^2 = \dfrac{3}{2}k_BT$, where $m$ is the mass of a single molecule and $k_B$ is the Boltzmann constant.
- Setting the $v_{rms}$ of the two gases equal at their respective temperatures links temperature and molecular mass directly, since the Boltzmann constant cancels out.
Step 1: Write the per molecule kinetic energy relation for each gas.
For hydrogen: $\dfrac{1}{2}m_Hv_{rms}^2 = \dfrac{3}{2}k_BT_H \Rightarrow v_{rms}^2 = \dfrac{3k_BT_H}{m_H}$
For oxygen: $v_{rms}^2 = \dfrac{3k_BT_O}{m_O}$
Step 2: Equate the two expressions since the r.m.s velocities are equal.
$\dfrac{3k_BT_H}{m_H} = \dfrac{3k_BT_O}{m_O}$
The Boltzmann constant cancels, leaving:
$\dfrac{T_H}{m_H} = \dfrac{T_O}{m_O}$
The ratio of molecular masses equals the ratio of molar masses, so $\dfrac{m_H}{m_O} = \dfrac{M_H}{M_O} = \dfrac{2}{32}$
Step 3: Substitute known values and solve for $T_H$.
$T_O = 47 + 273 = 320\ \text{K}$
$T_H = T_O\times\dfrac{M_H}{M_O} = 320\times\dfrac{2}{32} = 20\ \text{K}$
Final Answer: 20 K