Turns out it’s actually extremely easy to make certain types of charge-controlled memristors in spintronics just by using a pair of noncircular gears. The torque ratio (which changes the effective resistance of the resistor) varies as a function of gear position, which is coupled to length of chain aka spintronics charge. So if one of the noncircular gears is hooked up to a regular resistor, the other noncircular gear displays memristance. The downside of this is that with gears, the effective resistance as a function of charge can vary only a few-fold, as opposed to hundreds or thousands fold like is required for certain applications of memristors. You could also chain several noncircular gears together to get a greater peak ratio, but that probably comes with some problems in real life use.
The idea of noncircular gears also made me consider how to describe just the gears themselves, without necessarily linking one side to a resistor to make a memristor. I tried searching online to see if the framework for this has been established before but I didn’t find anything. I would call it a memformer, because it is analogous to a transformer in the same way a memristor is analogous to a resistor. In a transformer, restrictions are imposed on the relationship between V1 and V2, as well as I1 and I2. In a memformer, restrictions are imposed on the relationship between Φ1 and Φ2, as well as between Q1 and Q2.
Exactly as you would expect logically from the spintronics circuit, an ideal memristor in electronics could just as well be described by a memformer where one port is connected to a regular resistor. The only problem is figuring out how to actually make a practical memformer in electronics . Good thing it’s easy with spintronics though.