Question 705034

SCQMEDIUM

The region y>0y > 0 has a constant electrostatic potential V1V_1 and y<0y < 0 has a constant electrostatic potential V2V1V_2 \neq V_1. A charged particle with momentum p1\vec{p_1} is incident at an angle θ1\theta_1 on the interface of the two regions. If the particle has momentum p2\vec{p_2} in the region y<0y < 0, then the angle θ2\theta_2 is given by

Question
(A)

cos1(p2p1cosθ1)\cos^{-1}(\frac{p_2}{p_1} \cos \theta_1)

(B)

cos1(p1p2cosθ1)\cos^{-1}(\frac{p_1}{p_2} \cos \theta_1)

(C)

sin1(p2p1sinθ1)\sin^{-1}(\frac{p_2}{p_1} \sin \theta_1)

(D)

sin1(p1p2sinθ1)\sin^{-1}(\frac{p_1}{p_2} \sin \theta_1)

Detailed Solution

Since the potential is constant in each region, the force (which is the gradient of potential) is zero everywhere except at the interface (a delta-function potential). The tangential component of momentum parallel to the interface (xx-axis) is conserved.

Thus, p1sinθ1=p2sinθ2p_1 \sin \theta_1 = p_2 \sin \theta_2.

Solving for θ2\theta_2, we get

θ2=sin1(p1sinθ1p2)\theta_2 = \sin^{-1}(\frac{p_1 \sin \theta_1}{p_2}).

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