Q.In a chamber, a uniform magnetic field of 6.5 G (1 G=10−4 T) is maintained. An electron is shot into the field with a speed of 4.8×106 m s−1 normal to the field. Explain why the path of the electron is a circle. Determine the radius of the circular orbit. (e=1.5×10−19 C, me=9.1×10−31 kg).
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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 …
Concept: charged particle in a ⊥ magnetic field — circular motion.
Why a circle: the force F=q(v×B) is always perpendicular to v, so it does no work — the speed is constant. With v⊥B this constant-magnitude force always points to one centre, i.e. it is centripetal, giving uniform circular motion.
Radius: from evB=rmev2, r=eBmev. With B=6.5 G=6.5×10−4 T and the stated e=1.5×10−19 C: …
The magnetic force is perpendicular to the velocity, does no work and acts as a centripetal force, so the electron moves in a circle of radius r=eBmev≈4.48×10−2 m (using the stated e=1.5×10−19 C).
Why the path is a circle
The electron feels only the magnetic force F=q(v×B), which is always perpendicular to the velocity. A force perpendicular to v does no work, so the kinetic energy — and hence the speed — never changes. Since the electron enters normal to B, this force has constant magnitude evB and always points toward one fixed centre: exactly the condition for uniform circular motion.
Determining the radius
The magnetic force provides the centripetal force:
evB=rmev2 ⇒ r=eBmev.
Convert the field: B=6.5 G=6.5×10−4 T. Substituting the stated data (me=9.1×10−31 kg, v=4.8×106 m s−1, e=1.5×10−19 C):
r=(1.5×10−19)(6.5×10−4)(9.1×10−31)(4.8×106).
Numerator: 9.1×4.8=43.68, so 43.68×10−25. Denominator: 1.5×6.5=9.75, so 9.75×10−23. Hence …
Method: Lorentz Force & Centripetal Force Equivalence
Why the path is a circle
When a charged particle moves perpendicular to a uniform magnetic field:
- The magnetic force Fm=q(v×B) acts perpendicular to both velocity and field
- Since v⊥B, the force magnitude is Fm=∣q∣vB
- This force is always perpendicular to velocity → it changes only the direction, not the speed
- A constant perpendicular force causes uniform circular motion
Steps to find the radius
Step 1: Equate forces
The magnetic force provides the centripetal force:
∣q∣vB=rmv2
Step 2: Solve for radius
Cancel v from both sides:
r=∣q∣Bmv
Step 3: Convert units
B=6.5 G=6.5×10−4 T
Step 4: Substitute values
me=9.1×10−31 kg, v=4.8×106 m/s, e=1.5×10−19 C
r=(1.5×10−19)(6.5×10−4)(9.1×10−31)(4.8×106)
Step 5: Calculate
Numerator: 9.1×4.8×10−25=43.68×10−25 …
Common Mistakes & How to Avoid Them
Mistake 1: Forgetting to Convert Gauss to Tesla
The error: Students plug B=6.5 G directly into formulas, forgetting the conversion factor.
Why it happens: The problem gives B in Gauss but all standard formulas use Tesla. The conversion hint (1 G=10−4 T) is easy to miss under time pressure.
How to avoid: Always write the conversion step explicitly:
B=6.5 G=6.5×10−4 T
Pro tip: Circle or underline the conversion factor in the question before starting calculations.
Mistake 2: Using Wrong Charge Value
The error: Using e=1.6×10−19 C (the standard value) instead of the given e=1.5×10−19 C.
Why it happens: Students memorize the standard electron charge and automatically substitute it without checking the problem's data.
How to avoid: Always use the values provided in the question, even if they differ from standard textbook values. The problem deliberately gives 1.5×10−19 C — use it.
Mistake 3: Confusing the Reason for Circular Motion
The error: Saying "the electron moves in a circle because the magnetic force is perpendicular to velocity" — but not explaining why this produces a circle.
Why it happens: Students memorize the result without understanding the mechanism.
How to avoid: Explain step-by-step:
- Magnetic force F=q(v×B) acts perpendicular to both v and B
- Since v⊥B, the force magnitude is F=qvB
- This perpendicular force provides centripetal acceleration ac=v2/r
- The force changes only the direction of velocity, not its magnitude
- Result: uniform circular motion
Mistake 4: Sign Errors in Force Direction
The error: Forgetting that the electron has negative charge, so the force direction is opposite to that for a positive charge.
Why it happens: Students apply the right-hand rule for positive charges without flipping the direction for electrons.
How to avoid: Remember: For electrons, use left-hand rule or apply the right-hand rule and then reverse the direction. The magnitude calculation is unaffected, but conceptual questions about direction will be wrong.
Mistake 5: Formula Confusion — Radius Expression
The error: Writing r=qBmv incorrectly as r=qBmv2 or r=mvqB.
Why it happens: Mixing up centripetal force (mv2/r) with magnetic force (qvB).
How to avoid: Derive it quickly:
- Centripetal force = Magnetic force
- rmv2=qvB
- Cancel one v: rmv=qB …
- GSEB Higher Secondary Certificate (HSC) Examination 2025Set ANNUAL1 markMCQQ.An electron enters with a speed of 3 x 10^7 m/s into a uniform magnetic field of 6 x 10^-4 T at an angle of 60°. What is the pitch of the helical path? (me = 9.1 x 10^-31 kg, e = 1.6 x 10^-19 C)(a) 0.12 cm(b) 100 m(c) 89.3 cm(d) 20 m
›Reveal solutionSolution
An electron entering a magnetic field at an angle traces a helix: the velocity component along B (v‖) is unaffected and produces uniform translation, while the perpendicular component (v⊥) produces circular motion with period T = 2πm/(qB); the pitch is v‖T.
v‖ = v cos60° = (3 × 10⁷)(0.5) = 1.5 × 10⁷ m/s.
…
- GUJCET 2023Set 091 markMCQQ.An electron is projected with uniform velocity along the axis of current carrying long solenoid. Which of the following is true? (A) The electron path will be circular about the axis (B) The electron will be accelerated along the axis (C) The electron will experience a force at 45° to the axis and hence execute a helical path (D) The electron will continue to move with uniform velocity along the axis of the solenoid
›Reveal solutionSolution
[!TLDR]
Velocity parallel to the axial field gives zero magnetic force, so the electron moves undeviated at uniform velocity.
Concept
The magnetic force on a charge is F=qv×B. Its magnitude is qvBsinθ, which vanishes when v and B are parallel (θ=0).
Solution …
- GSEB Higher Secondary Certificate (HSC) Examination 2018Set ANNUAL1 markMCQQ.An electron performs circular motion of radius r, perpendicular to a uniform magnetic field B. The kinetic energy gained by this electron in one revolution is ___.(a) (1/2) mv^2(b) (1/4) mv^2(c) zero(d) pi r B e V
›Reveal solutionSolution
The magnetic force qv x B is always perpendicular to the velocity, so it does no work; the speed (and hence kinetic energy) is unchanged over any path, including a full revolution.
The magnetic force on a moving charge is F = q v x B, which is always perpendicular to v.
Work done W = integral of F . dl = 0 because F is perpendicular to the displacement at every instant.
…
- GSEB Higher Secondary Certificate (HSC) Examination 2018Set ANNUAL1 markMCQQ.A charged particle is moving with velocity v (vector) in a uniform magnetic field B (vector). The magnetic force acting on it, will be maximum when ___.(a) v and B are in same direction(b) v and B are in opposite direction(c) v and B are mutually perpendicular(d) v and B make an angle of 45 degree with each other
›Reveal solutionSolution
Magnetic force F = qvB sin(theta) is largest when theta = 90 degree, i.e. when v and B are perpendicular.
The magnitude of the magnetic force is F = q v B sin(theta), theta being the angle between v and B.
sin(theta) is maximum (= 1) at theta = 90 degree.
…
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