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We obtain bounds to show that the pressure of a two-body, mean-field spinglass is a Lipschitz function of the underlying distribution of the randomcoupling constants, with respect to a particular semi-norm. This allows us tore-derive a result of Carmona and Hu, on the universality of the SK model, by adifferent proof, and to generalize this result to the Viana-Bray model. We alsoprove another bound, suitable when the coupling constants are not independent,which is what is necessary if one wants to consider ``canonical'' instead of``grand canonical'' versions of the SK and Viana-Bray models. Finally, wereview Viana-Bray type models, using the language of L\'evy processes, which isnatural in this context.

Some Observations for Mean-Field Spin Glass Models