Step 1: Recall the equipartition of energy theorem.
The equipartition of energy theorem states that for a system in thermal equilibrium, the total energy is shared equally among all its degrees of freedom.
Specifically, the average kinetic energy associated with each translational degree of freedom is $\frac{1}{2}k_B T$, where $k_B$ is the Boltzmann constant and $T$ is the absolute temperature.
Step 2: Determine the average translational kinetic energy of a molecule.
A gas molecule in three-dimensional space has three translational degrees of freedom (corresponding to motion along the x, y, and z axes).
According to the equipartition theorem, the total average translational kinetic energy of a single molecule is:
\[
KE_{avg, trans} = 3 \times \left(\frac{1}{2}k_B T\right) = \frac{3}{2}k_B T.
\]
Step 3: Analyze the dependence of translational kinetic energy.
The formula $KE_{avg, trans} = \frac{3}{2}k_B T$ shows that the average translational kinetic energy depends only on the absolute temperature $T$.
It does not depend on the mass of the molecule, the type of gas (monatomic, diatomic, etc.), or any other property of the gas.
Step 4: Calculate the ratio for hydrogen and oxygen.
We are given that the hydrogen ($H_2$) and oxygen ($O_2$) gases are at the same temperature.
Since the average translational kinetic energy depends only on temperature, the molecules of both gases will have the same average translational kinetic energy.
\[
(KE_{avg, trans})_{H_2} = \frac{3}{2}k_B T.
\]
\[
(KE_{avg, trans})_{O_2} = \frac{3}{2}k_B T.
\]
The ratio is therefore:
\[
\frac{(KE_{avg, trans})_{H_2}}{(KE_{avg, trans})_{O_2}} = \frac{\frac{3}{2}k_B T}{\frac{3}{2}k_B T} = 1.
\]
The ratio is 1:1.