Robin288 said:
Summary:: I been stuck on this problem from past 4 months. I am completely done. I am getting no idea. Even my professor couldn't have helped me. Can anyone please help me?
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The circuit resembles an EMF connected in parallel with a capacitor, which is then connected also in parallel with a resistor.
The voltage on the capacitor is equal to the applied EMF voltage.
The capacitor resembles a parallel plate capacitor. Its capacitance (per unit length) is readily available on any textbook (depends on the geometry of the plates and on the dielectric material between the plates, which in this case is air).
So far we've got voltage and capacitance per unit length on the capacitor, from there we can find out the charge per unit length (check any textbook for the appropriate formula).
The electric field E between the plates can be found provided we know the voltage and distance between the plates (which we already know).
So we have the electric field E between the plates, and the charge per unit length.
It would be straightforward to believe that by multiplying the electric field E by the charge per unit length we would get the force per unit length acting on the capacitor's plates; but we would be lead astray because the electric field that we had found corresponds to the electric field inside the capacitor (in the gap), whereas the force on any plate is equal to the charge on that plate multiplied by the electric field exerted by the
other plate (the field has to be external to the charge, not generated by the same charge - otherwise it would be seen as trying to lift yourself by pulling up your shoelaces) . It is not difficult to check that the electric field of one of the plates is equal to half of the electric field which is in the gap between the plates.
So far we can find the electric force per unit length acting on any of the capacitor plates (as per Newton's third law they are equal).
What do you think so far?
Do you think you can handle to find the remaining magnetic force per unit length (it should correspond to a same magnitude than the electric force per unit length provided the net force is to vanish, wouldn't you agree)?
If you can catch up, you could deduce the current I from the magnetic force per unit lenght, and from there the resistance R. What follows should be a piece of cake.
Regards,
Alex