I'm peeping the NIST thermo tables for $\text{H}$ and $\text{H}_2$, and I'm perplexed.
Seems to me that using
$$G=[\Delta H^\circ_f+H-H^\circ(T_r)]-T\cdot S^\circ$$ (well, actually correcting the entropy for partial pressures in a mixture of ideal gases) obtains some bewildering values for simple reactions.
Consider $\text{H}_2 \rightarrow 2\text{H}$ at standard pressure and standard temperature. If I'm calculating it correctly (which I am sure I am not), using the values at $298.15^\circ K$ in columns 2 ($S^\circ$), 4 ($H-H^\circ(T_r)$), and 5 ($\Delta H^\circ_f$) from the links above, I find that
$$G_{\text{H}_2}=0\frac{\text{kJ}}{\text{mol}}−298.15^\circ \text{K}\cdot130.680\frac{\text{kJ}}{^\circ \text{K}\;\text{mol}}\approx-38962\frac{\text{kJ}}{\text{mol}}$$
And
$$G_\text{H}=217.999\frac{\text{kJ}}{\text{mol}}−298.15^\circ \text{K}\cdot114.716\frac{\text{kJ}}{^\circ \text{K}\;\text{mol}}\approx-33984\frac{\text{kJ}}{\text{mol}}$$
Which is great, the reaction isn't spontaneous. Except... if I recall correctly,
$$G_\text{mixture} = \sum^\text{species}_j \mu_j n_j$$
Where $n_j$ is the number of mols of that species and for ideal gases at constant pressure & temperature,
$$\mu_j = H_j-TS_j = G_j$$
That would imply the mixture of one mol of $\text{H}_2$ has a total gibbs of the aformentioned $-38962\frac{\text{kJ}}{\text{mol}}$, but the mixture of two mols of $\text{H}$ (pressure neglected) would be $2\times(-33984\frac{\text{kJ}}{\text{mol}})=-67969\frac{\text{kJ}}{\text{mol}}$, and now supposedly I've found that hydrogen gas spontaneously decomposes at standard temperature. That's clearly wrong.
(I've even done the calculations for a reaction considering pressure, and the doubling of mols of mixture post-reaction isn't enough to drive it into non-spontaneity except at absurdly high pressures)
So my question is: do I misunderstand how the Gibbs works for mixture of gases, how to read values off of the NIST themo tables, or both?
Thank you!