Two Magnetic Fields

In the x y xy -plane , the region y > 0 y>0 has a uniform magnetic field B 1 k B_1 \vec{k} and the region y < 0 y<0 has another uniform magnetic field B 2 k B_2 \vec{k} . A positively charged particle is projected from the origin along the positive y y -axis with speed v 0 = π m s 1 v_0=πms^{-1} at t = 0 t=0 as shown in the figure .

Let t = T t=T be the time when the particle crosses the x x axis from below for the first time. If B 2 = 4 B 1 B_2=4B_1 , the average speed of the particle, in m s 1 ms^{-1} , along the x x -axis in the time interval T T is ?

Details and Assumptions
1) Neglect gravity

The problem is not original.


The answer is 2.

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1 solution

In the region with magnetic flux density B 1 \vec B_1 , the differential equations of motion of the particle are

d v x d t = q B 1 m v y , d v y d t = q B 1 m v x \dfrac{dv_x}{dt}=\dfrac{qB_1}{m}v_y, \dfrac{dv_y}{dt}=-\dfrac{qB_1}{m}v_x .

Solving these using initial conditions we get v x = v 0 sin ( q B 1 t m ) v_x=v_0\sin (\frac{qB_1t}{m}) .

In the region where the magnetic flux density is B 2 B_2 , the x x -component of velocity is similarly

v 0 sin ( q B 2 t m ) v_0\sin (\frac{qB_2t}{m}) .

The time period in the first case is 2 π m q B 1 \dfrac{2πm}{qB_1} and in the second case is 2 π m q B 2 \dfrac{2πm}{qB_2} .

Hence the average speed of the particle in the x x direction is

q v 0 π m ( 1 B 1 + 1 B 2 ) × 2 m q ( 1 B 1 + 1 B 2 ) = 2 v 0 π = 2 \dfrac{qv_0}{πm(\frac{1}{B_1}+\frac{1}{B_2})}\times \dfrac{2m}{q}(\frac{1}{B_1}+\frac{1}{B_2})=\dfrac {2v_0}{π}=\boxed 2 ms 1 ^{-1} .

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