It is possible in concept for the frequency of current to be different than the frequency of the voltage. You would need a kind of load that distorts the shape of the voltage waveform for this to happen. Usually, there is at least some kind of relationship between the current and voltage waveform frequencies. A circuit may also attenuate, or amplify a certain range of frequencies, or it may produce harmonics of the original fundamental. I can't think of any example that would produce completely different frequencies, that aren't directly determined by the frequency of the voltage waveform.
As an example, an ideal full wave rectifier will turn a simple sine wave of voltage, V(t)=sin(ω*t), into the following Fourier series, when applied to a unit resistance load:
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This is what the circuit looks like, with the load resistor being 1 ohm:
Here's a plot that shows how this evolves as more cosine waves are added (I've deliberately drawn offsets, so you can see them separately):
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For an ~0.16 Hz voltage source, the original ω=1 rad/s. Constructing the first few terms of this sum:
I(t) = 0.6366 - 0.4244*cos(2*t) - 0.08488*cos(4*t) - 0.03638*cos(6*t) - 0.02021*cos(8*t)
This produces all kinds of different frequencies from the original 0.16 Hz. First being 2ω, then 4ω, then 6ω, and so forth. But they are all whole multiples of the fundamental (ω), and are all related to it. The current has frequencies of 0.32 Hz, 0.64 Hz, 0.96 Hz, etc, while the voltage only has an 0.16 Hz frequency.
When I somehow managed to pass the class on Fourier transform / series I hoped to never use it again…