Electrons don't have legs, but the concept might. How does the electron wavelength compare to the incidence of the geometry? Gamma = h bar/ momentum Where, m

Electrons don't have legs, but the concept might. How does the electron wavelength compare to the incidence of the geometry? Gamma = h bar/ momentum Where, m = m*v In a DC circuit the momentum can be held fairly stable once in a state of superconductance, but v is increasing up to the breakover point. Which in turn is decreasing wavelength. Bit of a trouble for a static 'circuit'. None of that is quantum anything, but it gets you thinking.