This is something you can see just by sticking a grain focuser under the negative and looking at the grain as you change f stop. It start mushy, sharpens up, and then becomes mushy again. Unless you have something like the 45mm f4 APO Componon, which starts sharp, and eventually goes mushy, probably due to starting with a less ambitious aperture. Thats the secret to the APO bit....they just dont allow f2.8
However, physics can answer this, from a diffraction perspective, where destructive interference of light calculations can be calculated, by considering geometry and wavelength. You get total destructive interference when the distance travelled between one light ray and another is equal to half a wavelength. This leads to some algebra which tells you for a given wavelength, what the aperture can be.
If the negative has say 80lpm on it, then thats the limit the enlarging lens can see, as there is no more image detail than 80lpmm. Even if the enlarging lens is capable of 500lpmm, if there is no more detail than 80lpmm, thats all you are going to get down on the paper. At f11, the Rayleigh diffraction limited resolution is 136lpmm. This means there is no contrast for 136lpmm. So contrast should still be good for detail at 80lpmm. Contrast at 80lpmm on the film will be low, anyway, as thats approaching the limit of what a taking lens can record. If you were to consider the same arguments for 40lpmm instead, then f22 would be ok. 80lpmm will allow a 10x print to have 8lpmm on the print, which is practically perfect.
So for 10x enlargement, f11 is still fine. Really, adjustment of f stop enables setting of printing times.