A wire of mass m and length l can slide freely on a pair of smooth, vertical rails (figure 38-E31). A magnetic field B exists in the region in the direction perpendicular to the plane of the rails. The rails are connected at the top end by a capacitor of capacitance C. Find the acceleration of the wire neglecting any electric resistance.
Let the rod has a velocity 'θ' at any instant, then, at that point,
e=Blθ
Now, q=c×potential=ce=cBlθ
Current=dqdt=cBlθ
=cBldθdt=cBla
(where a→ acceleration)
From given figure force due to magnetic field and gravity are opposite to each other.
So, mg−ilB=ma
⇒ mg−cBla×lB=ma
⇒ ma+cB2l2a=mg
⇒ a(m+cB2l2)=mg
⇒ a=mgm+cB2l2