(a) The condition for particle to continue along x-axis is:
qE = q vB sin 90°
or v = \(\frac{E}{B}\)
When the electric field is switched off, the trajectory of the charge will become helical about the direction of the magnetic field.

(b) At any point P magnetic field intensity due to current I2 in CD
B = \(\frac{\mu_0I_2}{2\pi r}\)
Its direction is perpendicular to the plane of the paper and downwards.
Force per unit length experienced by conductor AB is given by
\(\frac{F}{h} \) = B, I1 = \(\frac{\mu_0I_1I_2}{2\pi r}\)
At equilibrium
\(\frac{\mu_0I_1I_2}{2\pi r} = \frac{mg}{h}\)