show us your effort/s to solve this problem.
This is a very complicated problem. Rigorous understanding of Magnetism is necessary. Besides that we have to understand the geometry of the problem. If we have a long straight current-carrying wire, we know that it produces a magnetic field near it equal to:
B=2πRμ0I=2πyμ0I
If a particle is moving in this magnetic field, a magnetic force will act on it equal to:
F=qvB=evB
Since the electron is moving in the same plane of the wire, the magnetic field must be in a plane perpendicular to this plane which means that the velocity and the force are perpendicular to each other in the same plane of the wire. Because of this geometry, the magnitude of the velocity will not change, it is only that its components will change.
From elementary physics, we know that the force is equal to:
F=ma
This force has two components.
Fx=max=mdtdvx
Fy=may=mdtdvy
We don't have enough information in the
x direction, so we will work in the
y direction. As the electron gets closer to the wire, its velocity in the
y direction decreases and its velocity in the
x direction increases. Therefore, at
y=1 cm,vy=0 and v=vx=3.4×106 m/s. In fact
∣v∣=3.4×106 m/s at any point.
This information is very important and it is the key to solve this problem. Let us work on the force in the
y direction.
Fy=mdtdvy
Fcosθ=mdtdvy
evBcosθ=mdtdvy
We know that
vy=vsinθ then
dvy=vcosθ dθ and from the chain rule, we get:
dtdvy=dydvydtdy=dyvcosθ dθvy=v2sinθcosθdydθ
evBcosθ=mdtdvy
ev(2πyμI)cosθ=mv2sinθcosθdydθ
∫0.50.01e(2πyμI) dy =∫4π0mvsinθ dθ
e(2πμI)lny∣∣∣∣∣0.50.01 =−mvcosθ∣∣∣∣∣4π0
e(2πμI)(ln0.5−ln0.01) =mv(cos0−cos4π)
I=eμ(ln0.5−ln0.01)2πmv(cos0−cos4π)=(1.6×10−19)(4π×10−7)(ln0.5−ln0.01)2π(9.11×10−31)(3.4×106)(cos0−cos4π)≈7.2 A