Physics

Physics

Problem

The region between y=0y = 0 and y=dy = d contains a magnetic field B⃗=Bz^\vec{B} = B\hat{z} . A particle of mass mm and charge qq enters the region with a velocity v⃗=vi^\vec{v} = v\hat{i} . if d=mv2qBd = \frac{mv}{2qB} , the acceleration of the charged particle at the point of its emergence at the other side is : a. qvBm(12i^−32j^)\frac{qvB}{m} \left( \frac{1}{2}\hat{i} - \frac{\sqrt{3}}{2}\hat{j} \right) b. qvBm(32i^+12j^)\frac{qvB}{m} \left( \frac{\sqrt{3}}{2}\hat{i} + \frac{1}{2}\hat{j} \right) c. qvBm(−j^+i^2)\frac{qvB}{m} \left( -\frac{\hat{j} + \hat{i}}{\sqrt{2}} \right) d. qvBm(i^+j^2)\frac{qvB}{m} \left( \frac{\hat{i} + \hat{j}}{\sqrt{2}} \right)

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