I am probably not the kind of expert you need here. But look at this page which I found very interesting:
http://www.hagtech.com/loading.html
The first section deals specifically with loading MM cartridges with capacitance. However, the formula Fr = 1 / (2*PI*SQRT(L * C)) works equally for MC and MM cartridges. This formula defines the cart’s resonant frequency based on its inherent inductance and the downstream (cable) capacitance. The resonance is often accompanied by a sharp peak and followed by rolloff. Generally you want this frequency as high as possible, well out of the audible band (> 20kHz). This generally requires low capacitance OR low inductance (as per the formula). MC cartridges get the low inductance (that’s the L in the formula) for "free". Normally this is enough that they need not concern themselves with phono cable capacitance. HOWEVER with a SUT reflecting the output cable’s capacitance times the square of its turns ratio (look this up elsewhere), capacitance could suddenly become large enough to drop the resonant frequency back near or into audible range and become a concern. For example: say you (unwisely) choose a fat audiophile interconnect run with 200 pF capacitance. And your SUT is a 30x. 30 * 30 * 200pF = 180,000 pF. Wow. Say your MC has an inductance of 1mH. Using the calculator in that Hagerman page I linked, the resonance is now at 3,800 Hz. You’re gonna have a bad time! Choose a cable with 40pF and now it’s at 26,000 Hz. Much better!