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Question: An electron moving at the right angle to a uniform magnetic field completes a circular orbit in 1 mi...

An electron moving at the right angle to a uniform magnetic field completes a circular orbit in 1 microsecond. Find the magnetic field.

Explanation

Solution

The charge in a magnetic field, moving with a velocity causes a force, which is called Lorentz force. The charged particle to complete a circular motion, it needs a centripetal force as well. So, you should identify the forces properly in this problem.

Formula Used:
The Lorentz force F\vec F is defined as
F=q(v×B)\vec F = q\left( {\vec v \times \vec B} \right)
where, qq is the charge of the particle, v\vec v is the velocity of the particle and B\vec B is the uniform magnetic field.
If a particle with mass mm moves with a velocity vv through a circular path with radius rr then the centripetal force is defined to be
F=mv2rF = \dfrac{{m{v^2}}}{r}

Complete step by step answer:
Given:
The electron completes a circular orbit in 1 microsecond.
To get: The magnetic field.
Step 1:
Let the electron moves with a velocity vv in the uniform field BB
The electron moves at a right angle to the uniform magnetic field BB.
Hence calculate the Lorentz force from eq (1)
F=qvBsinθ F=qvBsin90 F=qvB  F = qvB\sin \theta \\\ \Rightarrow F = qvB\sin {90^ \circ } \\\ \Rightarrow F = qvB \\\
Step 2:
Let the electron moving along a circular path of radius rr.
Let the mass of the electron is m.
Calculate the centripetal force to keep it in a circular orbit.
F=mv2rF = \dfrac{{m{v^2}}}{r}

Step 3:
Now you can see that the Lorentz force supplies the required centripetal force to keep it in a circular motion.
Now find the expression of the magnetic field
F=qvB=mv2r B=mvqr  F = qvB = \dfrac{{m{v^2}}}{r} \\\ \Rightarrow B = \dfrac{{mv}}{{qr}} \\\
Step 4:
By the problem, the electron completes one circular orbit.
So, you can calculate the angular velocity
ω=2π1×106rad.s1\omega = \dfrac{{2\pi }}{{1 \times {{10}^{ - 6}}}}rad.{s^{ - 1}}

Step 5:
The mass of the electron is m=9.11×1031kgm = 9.11 \times {10^{ - 31}}kg and the charge is q=1.6×1019Cq = 1.6 \times {10^{ - 19}}C.
By definition, we know that the angular velocity can be represented as
ω=vr\omega = \dfrac{v}{r}
Hence, now put the values together to get the value of the magnetic field
B=mvqr B=mqvr B=mqω B=9.11×10311.6×1019×2π1×106T B=9.11×2×3.14×10311.6×1019×106T=3.53×105T B=3.53×105T  B = \dfrac{{mv}}{{qr}} \\\ \Rightarrow B = \dfrac{m}{q}\dfrac{v}{r} \\\ \Rightarrow B = \dfrac{m}{q}\omega \\\ \Rightarrow B = \dfrac{{9.11 \times {{10}^{ - 31}}}}{{1.6 \times {{10}^{ - 19}}}} \times \dfrac{{2\pi }}{{1 \times {{10}^{ - 6}}}}T \\\ \Rightarrow B = \dfrac{{9.11 \times 2 \times 3.14 \times {{10}^{ - 31}}}}{{1.6 \times {{10}^{ - 19}} \times {{10}^{ - 6}}}}T = 3.53 \times {10^{ - 5}}T \\\ \therefore B = 3.53 \times {10^{ - 5}}T \\\

If an electron moving at right angle to a uniform magnetic field completes a circular orbit in microsecond, then the magnetic field is 3.53×105T3.53 \times {10^{ - 5}}T.

Note:
The Lorentz force is to be completely equal to the centripetal force as there are no other sources in the system. When the electron completes a circular orbit, that means it traverses 2πrad2\pi rad angular distance. You need to carefully notice that this angular distance is traversed in the said 11 microsecond time interval.