Q.In Exercise 4.11 obtain the frequency of revolution of the electron in its circular orbit. Does the answer depend on the speed of the electron? Explain.
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Charged Particle in a Magnetic Field
When a charged particle moves through a magnetic field, the field grabs it sideways. Unlike an electric field, which can speed a charge up or slow it down, a magnetic field only bends the path — it never changes the particle's speed. Understanding why leads directly to circular and helical motion, the basis of cyclotrons, mass spectrometers and the aurora.
The force: always sideways
A particle of charge q moving with velocity v in a magnetic field B feels the magnetic (Lorentz) force:
F=q(v×B)
Because of the cross product, F is perpendicular to both v and B. Its magnitude is
F=∣q∣vBsinθ
where θ is the angle between v and B.
Since F⊥v, the force does no work: F⋅v=0. Therefore the kinetic energy and the speed stay constant — the field only changes the direction of motion, never the magnitude.
Case 1: velocity perpendicular to the field → a circle
If v⊥B (θ=90∘), the force F=qvB stays constant in size and always points toward one central point. That is exactly the condition for uniform circular motion, with the magnetic force acting as the centripetal force:
qvB=rmv2
Solving for the radius:
r=qBmv
The time period of one revolution is
T=v2πr=qB2πm
The period T (and the frequency f=qB/2πm, the cyclotron frequency) does not depend on the speed or the radius. A faster particle traces a bigger circle but takes exactly the same time per loop. This speed-independence is what makes the cyclotron work.
Case 2: velocity at an angle → a helix
If v makes an angle θ with B, split it into two parts:
- Perpendicular component v⊥=vsinθ — feels the magnetic force and drives circular motion of radius r=qBmv⊥.
- Parallel component v∥=vcosθ — feels no force (since v∥×B=0) and carries the particle steadily along the field line.
Combining a circle with a steady drift gives a helix. The distance advanced along the field in one full turn is the pitch:
p=v∥T=vcosθ⋅qB2πm
A quick example
An electron (m=9.1×10−31 kg, q=1.6×10−19 C) enters a 0.02 T field at 106 m/s, perpendicular to B:
r=qBmv=(1.6×10−19)(0.02)(9.1×10−31)(106)≈2.8×10−4 m …
Why this formula?
Charged Particle in a Magnetic Field — Why the Key Formulas Hold
Let's build this from first principles. The core idea is that a magnetic field exerts a force only on a moving charge, and that force is always perpendicular to both the velocity and the field.
1. The Fundamental Force Law: Lorentz Force
The starting point is the Lorentz force for a charge q moving with velocity v in a magnetic field B:
Fm=q(v×B)
Why this form?
- Cross product v×B means the force is perpendicular to both v and B.
- Magnitude: Fm=∣q∣vBsinθ, where θ is the angle between v and B.
- Direction: given by the right-hand rule (for positive q).
Key insight: Because Fm⊥v, the magnetic force does no work — it changes only the direction of velocity, not its speed.
2. Circular Motion in a Uniform Magnetic Field
Consider a charge q moving with speed v perpendicular to a uniform B (so θ=90∘, sinθ=1).
Step 1: Force provides centripetal acceleration
The magnetic force is the only radial force:
Fm=qvB
This must equal the centripetal force required for circular motion:
Fc=rmv2
Step 2: Equate and solve for r
qvB=rmv2
Cancel one v (assuming v=0):
qB=rmv
Thus:
r=qBmv
This is the radius of the circular path (cyclotron radius).
Why this makes sense:
- Larger mass m → harder to turn → larger r
- Larger charge q or stronger B → stronger force → tighter turn → smaller r
- Faster speed v → more momentum → larger r
3. Angular Frequency (Cyclotron Frequency)
From the circular motion relation:
ω=rv
Substitute r=qBmv:
ω=qBmvv=mqB
Thus:
ωc=mqB
Why this is remarkable:
- ωc is independent of speed v — all particles with same q/m have the same angular frequency, regardless of how fast they move.
- This is the principle behind cyclotrons (particle accelerators).
4. General Motion: Helical Path …
The key idea is that a charged particle moving perpendicular to a uniform magnetic field experiences a centripetal force, giving circular motion with a frequency independent of speed.
Reasoning:
- For an electron of mass m and charge magnitude e moving with speed v perpendicular to a field B, the magnetic force evB supplies the centripetal force:
evB=rmv2⟹r=eBmv
- The period of one revolution is
T=v2πr=eB2πm
- The frequency is
f=T1=2πmeB
Notice v has cancelled out completely -- f depends only on e, B, and m, never on the electron's speed. …
The frequency of revolution of the electron is f=2πmeB≈1.82×107 Hz (≈18 MHz) -- the cyclotron frequency -- and it is independent of the electron's speed.
Why This Works: The Concept
When a charged particle like an electron moves perpendicular to a uniform magnetic field, the magnetic force acts as a centripetal force, bending the path into a circle. The magnetic force depends on speed (evB), but so does the centripetal requirement (mv2/r) -- these two speed-dependences cancel when solving for the period, leaving a frequency that depends only on the charge-to-mass ratio and the field strength. This is exactly why cyclotrons work: particles of different speeds still complete one revolution in the same time.
Step-by-Step Solution
- Set up the force balance. For an electron of mass m and charge magnitude e moving with speed v perpendicular to a uniform field B, the magnetic force supplies the centripetal force:
evB=rmv2
- Solve for the radius.
r=eBmv
A faster electron traces a larger circle.
- Find the period T.
T=v2πr=v2π⋅eBmv=eB2πm
The speed v cancels out completely.
- Obtain the frequency.
f=T1=2πmeB
f=2πmeB
- Compute the numeric value, continuing the earlier exercise's data. That exercise gives B=6.5 G=6.5×10−4 T, with e=1.6×10−19 C and me=9.1×10−31 kg:
f=2π(9.1×10−31)(1.6×10−19)(6.5×10−4)=5.72×10−301.04×10−22≈1.82×107 Hz
So the electron completes about 1.82×107 revolutions every second (roughly 18 MHz).
- Does the answer depend on speed? …
Method: Centripetal Force Equals Magnetic Lorentz Force
This is the standard method for finding the cyclotron frequency (or gyrofrequency) of a charged particle moving perpendicular to a uniform magnetic field.
Steps
- Identify the force providing centripetal acceleration For an electron moving in a circle of radius r with speed v, the centripetal force required is:
Fc=rmv2
where m is the electron's mass.
- Identify the magnetic force on the moving charge For a charge q moving with velocity v perpendicular to a uniform magnetic field B, the magnetic Lorentz force is:
FB=∣q∣vB
(The direction is given by the right-hand rule, but magnitude is what matters here.)
- Set the forces equal (since the magnetic force provides the centripetal force):
rmv2=∣q∣vB
- Solve for the radius (optional, but helps find frequency):
r=∣q∣Bmv
- Relate speed to angular frequency For circular motion, v=ωr, where ω is the angular frequency (in rad/s). Substitute into the radius equation:
r=∣q∣Bm(ωr)
- Cancel r (assuming r=0) and solve for ω:
ω=m∣q∣B
- Convert to frequency of revolution (cycles per second):
f=2πω=2πm∣q∣B
Final Answer
For an electron, ∣q∣=e (magnitude of electron charge), so: …
Common Mistakes: Charged Particle in Magnetic Field (Exercise 4.11)
Mistake #1: Forgetting the Formula for Frequency
The error: Students often confuse frequency (ν) with angular frequency (ω) or use the wrong expression.
Correct approach:
For a charged particle moving in a uniform magnetic field:
- Centripetal force is provided by magnetic force:
qvB=rmv2
- Radius of orbit:
r=qBmv
-
Time period (T) = v2πr=qB2πm
-
Frequency of revolution:
ν=T1=2πmqB
Key insight: The frequency depends only on q, B, and m — not on speed v.
Mistake #2: Thinking Frequency Depends on Speed
The error: Many students assume that a faster electron means more revolutions per second.
Why it's wrong:
- A faster electron has a larger radius (r∝v), so it travels a longer circumference in the same time.
- The increase in path length exactly cancels the increase in speed.
- Result: Time period (and frequency) is independent of speed.
How to avoid: Always derive T=qB2πm and notice v cancels out.
Mistake #3: Using Wrong Units or Constants
The error:
- Using mass of electron in grams instead of kg
- Forgetting q=1.6×10−19 C
- Mixing up m (mass) with m (metres)
How to avoid:
- Write all quantities in SI units before substituting
- Double-check: mass in kg, charge in C, magnetic field in Tesla
Mistake #4: Confusing Frequency with Angular Frequency
The error: Stating ω=2πmqB instead of ω=mqB
Correct relationships:
| Quantity | Symbol | Formula |
|---|---|---|
| Angular frequency | ω | mqB |
| Frequency | ν (or f) | 2πmqB |
How to avoid: Remember ω=2πν, so if you derive ω, divide by 2π to get ν.
--- …
- KEAM 2025Set pha-2025-0424F4 marksMCQQ.When a proton moves in a uniform magnetic field such that its velocity has a component along the direction of magnetic field, its trajectory will be a (A) circle (B) straight line (C) helix (D) parabola (E) ellipse
›Reveal solutionSolution
The parallel velocity component moves the proton uniformly along B while the perpendicular component makes it circle; together these produce a helix.
The magnetic force F=qv×B acts only on the velocity component perpendicular to B, causing circular motion in that plane. The component of velocity along B experiences no force and stays constant, giving uniform …
- KEAM 2025Set pha-2025-0429F4 marksMCQQ.If an electron moves with a velocity v in a magnetic field B, the magnetic force on the electron is maximum when the angle between v and B is (A) 30º (B) 180º (C) 60º (D) 90º (E) 0º
›Reveal solutionSolution
The Lorentz magnetic force magnitude is F=qvBsinθ, which is greatest when the velocity is perpendicular to the field, i.e. θ=90∘.
The force on a charge moving in a magnetic field is
F=qv×B,∣F∣=qvBsinθ. …
- KEAM 2024Set eng-2024-06054 marksMCQQ.If a charged particle enters a uniform magnetic field B, with a velocity v such that v has a component along B, then the charged particle describes (A) a circular path (B) an elliptical path (C) a straight line (D) a helical path (E) a parabolic path
›Reveal solutionSolution
The perpendicular velocity component makes a circle while the parallel component moves uniformly along B — the combination is a helix.
Resolve v into components parallel and perpendicular to B:
- The perpendicular component gives uniform circular motion (magnetic force qv⊥B). …
- KEAM 2024Set pha-2024-06104 marksMCQQ.The magnetic force acting on a charged particle carrying a charge 3μC in a magnetic field of 5 T acting in the y-direction, when the particle velocity is i^+j^×105ms−1 is (A) 0.5 N in +x direction (B) 0.2 N in +y direction (C) 2 N in −x direction (D) 1.5 N in −z direction (E) 1.5 N in +z direction
›Reveal solutionSolution
Compute the Lorentz force qv×B.
Given q=3μC=3×10−6 C, v=(i^+j^)×105 m/s, B=5j^ T.
v×B=105(i^+j^)×5j^=5×105(i^×j^+j^×j^)=5×105k^. …
- KEAM 2023Set eng-2023-P1-A14 marksMCQQ.A magnetic field of (10−4k^)T exerts a force of (4i^−3j^)×10−12N on a particle having a charge of 10−9C. The speed of the particle is: (A) 40m/s (B) 402m/s (C) 50m/s (D) 503m/s (E) 1002m/s
›Reveal solutionSolution
With F perpendicular to B, v = F/(qB) = (5 x 10^-12)/(10^-9 x 10^-4) = 50 m/s.
Concept and Intuition
The magnetic force is F = q v x B. Here B is along z and the force lies in the x-y plane, so the velocity component producing the force is perpendicular to B; the magnitude relation reduces to F = q v B.
Step-by-Step Solution
- Magnitude of force: |F| = sqrt(4^2 + 3^2) x 10^-12 = 5 x 10^-12 N.
- B = 10^-4 T, q = 10^-9 C, and v is perpendicular to B. …
- KEAM 2022Set eng-2022-P1-A14 marksMCQQ.An electron and a proton moving with same velocity v enter into a uniform perpendicular magnetic field. Then (A) proton alone moves in straight line path (B) electron alone moves in straight line path (C) both move in straight line paths (D) both move in elliptical paths (E) both move in circular paths
›Reveal solutionSolution
Both the electron and proton move perpendicular to B, so each follows a circular path.
Concept and Intuition
A charged particle entering a uniform magnetic field with velocity perpendicular to the field feels a force F=qv×B that is always perpendicular to the velocity and constant in magnitude. This is a centripetal force, producing uniform circular motion. Both the electron and proton are charged and moving perpendicular to B.
Step-by-Step Solution
- Force magnitude F=qvB (since v⊥B), always perpendicular to v.
- A constant perpendicular force gives circular motion of radius r=mv/qB. …
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