In short, then
(1) a conductor begins to move in the magnetic field
"E=\\frac{d\\Phi}{dt}=-\\frac{B(dS\\cdot l)}{dt}=-Bv_0l (v_0=const)". It is clear. But when "t=0" then "v=0" ,
and "t=\\tau" then "v=v_0". That is "v=at\\to t\\approx\\frac{v}{a}.".
(2) a conductor outside homogeneous magnetic field. In this case based on classic ideas I got (for wire 1 mm x 1 mm)
"U\\approx \\frac{q\\cdot n\\cdot x\\cdot v\\cdot t}{4\\pi\\epsilon_0}\\to t\\approx 8\\cdot10^{-18} s"
where
q - the charge of electron;
n - the concentration of electrons in the conductor;
x - thickness of the conductor (I assumed that the conductor was rectangular and made of copper).
Comments
Dear Vitezslav Havelek, please check updated solution
Great, but what is the meaning of q,n,x and other params of the second formula? Any reference to this equation to understand it?
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