A dielectric slab of thickness d is inserted in a parallel plate capacitor whose negative plate is at x = 0 and positive plate is at x = 3d . The slab is equidistant from the plates. The capacitor is given some charge. As one goes from 0 to 3d
the direction of the electric field remains of the same
the electric potential decreases continuously from x = 0 to x = 3d
the magnitude of the electric field remains the same
the electric potential increases at first, then decreases and again increases
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