Q.An electron falls through a distance of 1.5cm in a uniform electric field of magnitude 2.0×104N C−1 [Fig. 1.10(a)]. The direction of the field is reversed keeping its magnitude unchanged and a proton falls through the same distance [Fig. 1.10(b)]. Compute the time of fall in each case. Contrast the situation with that of 'free fall under gravity'.
Concept understanding — Charge To Mass Ratio
Charge to Mass Ratio: The First Meeting
Imagine you have two identical-looking balls. One is made of cork, the other of lead. If you blow on them with the same fan, the cork ball flies away easily, while the lead ball barely moves. The difference isn't in the force you applied — it's in how much mass each ball has. Now imagine that instead of blowing air, you're using an electric field to push a charged particle. The same idea applies: the particle's response depends on both its charge (how strongly the field pushes it) and its mass (how much inertia it has to overcome).
The charge to mass ratio (e/m for an electron, often written as q/m in general) is simply the charge of a particle divided by its mass. It tells you how much "electric responsiveness" a particle has per unit of its inertia.
Why This Ratio Matters
Two particles can have the same charge but very different masses. A proton and a positron both have charge +e, but the proton is about 1836 times heavier. If you put them in the same electric field, the positron accelerates 1836 times more. The charge-to-mass ratio captures this difference in a single number.
For an electron:
mee≈1.76×1011C/kg
For a proton:
mpe≈9.58×107C/kg
The electron's ratio is nearly 2000 times larger. That's why electrons are so much more mobile in circuits and beams — they respond far more dramatically to electric and magnetic fields.
The Precise Definition
mq=mass of the particlecharge of the particle
Its SI unit is coulombs per kilogram (C/kg). For any charged particle, this ratio determines:
- How much it accelerates in an electric field: a=mqE
- How tightly it curves in a magnetic field: radius r=qBmv
- The frequency of its circular motion: ω=mqB
How It Was Discovered
J.J. Thomson measured this ratio for cathode rays in 1897. He didn't know what the particles were — he just knew they were charged and had mass. By balancing electric and magnetic forces, he found that the ratio was over a thousand times larger than for any known ion. This told him the particles (which we now call electrons) were either extraordinarily charged or extraordinarily light. We now know it's the latter: the electron is the lightest charged particle with a non-zero rest mass.
The charge-to-mass ratio is a fundamental property of each type of particle. It cannot be changed — it's as intrinsic as the particle's spin or its rest mass.
A Common Confusion
Students sometimes think a larger charge means a larger ratio. Not necessarily. A particle with charge +2e and mass 4mp (like an alpha particle) has a ratio half that of a proton. The ratio depends on both numbers, not just the charge.
The Takeaway
The charge-to-mass ratio is the particle's "agility" in electromagnetic fields. It's the bridge between the electric force it feels and the inertia it carries. Whenever you see a charged particle bending in a magnetic field or accelerating between plates, this single number governs everything.
The charge-to-mass ratio of a particle is q/m — the charge divided by the mass, measured in C/kg, and it determines how strongly the particle responds to electric and magnetic fields.
"Charge to mass ratio of electron formula" and "Thomson experiment class 12 physics" are common search queries, and this concept connects the Moving Charges and Magnetism chapter of the NCERT/CBSE Class 12 Physics curriculum with the historical discovery of the electron. It's also a recurring topic in JEE Main and NEET questions on charged-particle motion in fields.
Why this formula?
Charge to Mass Ratio (e/m) — Why the Formula Holds
The charge-to-mass ratio (e/m) is a fundamental property of charged particles. For the electron, its measurement was a landmark experiment by J.J. Thomson (1897). Let's understand why the key formula emerges from the physics.
1. The Core Idea: Balancing Forces
The experiment uses a velocity selector — a region with perpendicular electric (E) and magnetic (B) fields.
What happens to a charged particle?
A particle with charge q and mass m moving with velocity v experiences:
- Electric force: FE=qE (direction: along E)
- Magnetic force: FB=q(v×B) (direction: perpendicular to both v and B)
The key insight:
If we arrange E and B perpendicular to each other and to v, the two forces act in opposite directions.
2. Deriving the Velocity Condition
For the particle to pass undeflected through the crossed fields:
FE+FB=0
Since forces are opposite:
qE=qvB
Cancel q (non-zero for a charged particle):
v=BE
Why this matters: This gives us the particle's speed without knowing its mass or charge. The velocity selector picks out only particles with this specific speed.
3. Measuring e/m — The Circular Path
After the velocity selector, the particle enters a region with only magnetic field (B). Here:
- Magnetic force provides centripetal force
- The particle moves in a circular path of radius r
Force balance:
qvB=rmv2
Rearranging:
mq=Brv
Substituting v=E/B from step 2:
mq=B2rE
4. Why This Formula Holds — The Physical Logic
| Step | Physics Principle | What it gives us |
|---|---|---|
| 1 | Force balance in crossed fields | Speed v=E/B |
| 2 | Centripetal force in magnetic field | Radius r depends on q/m |
| 3 | Combine both | Direct measurement of q/m |
Key assumptions (exam-relevant):
- Uniform E and B fields
- No other forces (gravity negligible for electrons)
- Particle enters perpendicular to both fields
5. For the Electron: The Famous Result
Thomson found:
mee≈1.76×1011C/kg
Why this was revolutionary: It showed that the electron's e/m was ~2000 times larger than that of hydrogen ions — meaning either the electron had a tiny mass or a huge charge. This proved the electron was a subatomic particle.
Quick Exam Tip
When asked to derive e/m:
- Start with force balance in crossed fields → get v
- Use circular motion in pure B → get q/m=v/(Br)
- Substitute v → final formula
Never skip the cancellation of q in step 1 — that's the conceptual key!
In a uniform field the electric force F=qE is constant, so each particle has constant acceleration a=qE/m and, starting from rest, falls through s in t=2s/a.
Data: s=1.5cm=0.015m, E=2.0×104N/C, e=1.6×10−19C.
Electron (me=9.11×10−31kg):
ae=meeE=9.11×10−31(1.6×10−19)(2.0×104)=3.51×1015m/s2,
te=3.51×10152(0.015)=2.92×10−9s.
Proton (mp=1.67×10−27kg):
ap=mpeE=1.67×10−27(1.6×10−19)(2.0×104)=1.92×1012m/s2,
tp=1.92×10122(0.015)=1.25×10−7s.
Contrast: in gravity a=g≈9.8m/s2 is the same for every body, whereas here a=qE/m depends on the charge-to-mass ratio, so the light electron falls much faster than the proton, and both times are far shorter than a gravitational fall (≈0.055s).
te=2.92×10−9s (electron) and tp=1.25×10−7s (proton).
Both particles undergo constant acceleration a=qE/m, so t=2s/a: the electron takes 2.92×10−9s and the proton 1.25×10−7s. Unlike free fall (where a=g is mass‑independent), here the time depends on q/m, and both are far shorter than a gravitational fall.
A uniform field exerts a constant force F=qE, hence a constant acceleration by Newton's second law. Starting from rest, kinematics gives s=21at2, so t=2s/a.
Given: s=1.5cm=0.015m, E=2.0×104N/C, e=1.6×10−19C, me=9.11×10−31kg, mp=1.67×10−27kg. In (a) the field points up and the electron (negative) is pushed down; in (b) the field is reversed and the proton (positive) is also pushed down — so each falls through the same s.
Electron.
ae=meeE=9.11×10−31(1.6×10−19)(2.0×104)=3.51×1015m/s2,
te=ae2s=3.51×10152(0.015)=8.55×10−18=2.92×10−9s.
Proton. The force magnitude eE=3.2×10−15N is the same, but the proton is about 1836 times heavier:
ap=mpeE=1.67×10−27(1.6×10−19)(2.0×104)=1.92×1012m/s2,
tp=ap2s=1.92×10122(0.015)=1.57×10−14=1.25×10−7s.
Contrast with free fall under gravity. In free fall the acceleration is g≈9.8m/s2, identical for every body regardless of mass. Here the acceleration a=qE/m is enormous (∼1012–1015m/s2) and depends on the charge‑to‑mass ratio, so electron and proton fall in very different times. A purely gravitational fall through the same 0.015m would take tg=2s/g≈0.055s — millions of times longer, which is why gravity is negligible for charged particles in such fields.
te=2.92×10−9s (electron) and tp=1.25×10−7s (proton).
Method: Newton’s Second Law + Kinematics (Uniform Acceleration)
This method uses the electric force to find acceleration, then applies equations of motion for constant acceleration.
Step 1 — Identify the force and acceleration
For a charge q in a uniform electric field E:
F=qE
By Newton’s second law:
a=mF=mqE
- For the electron: q=−e, so ae=me−eE (magnitude ae=meeE)
- For the proton: q=+e, so ap=mpeE
Step 2 — Apply kinematics for constant acceleration
The particle falls from rest (u=0) through distance s=1.5 cm=0.015 m.
Using s=ut+21at2:
t=a2s
Step 3 — Compute times
Given:
E=2.0×104 N C−1
e=1.6×10−19 C
me=9.1×10−31 kg
mp=1.67×10−27 kg
For electron:
ae=9.1×10−31(1.6×10−19)(2.0×104)=3.52×1015 m s−2
te=3.52×10152×0.015=8.52×10−18=2.92×10−9 s
For proton:
ap=1.67×10−27(1.6×10−19)(2.0×104)=1.92×1012 m s−2
tp=1.92×10122×0.015=1.56×10−14=1.25×10−7 s
Step 4 — Contrast with free fall under gravity
- Free fall acceleration: g≈9.8 m s−2 Time to fall 1.5 cm:
tg=9.82×0.015=0.055 s
- Key differences:
- Electric acceleration is huge compared to g (by factors of 1011 to 1014)
- Electron falls ~43 times faster than proton (because me≪mp)
- In free fall, all objects fall with same acceleration (independent of mass) — here, acceleration depends on charge-to-mass ratio q/m
Final results:
| Particle | Time of fall |
|---|---|
| Electron | 2.92×10−9 s |
| Proton | 1.25×10−7 s |
| Free fall | 0.055 s |
Common Mistakes & How to Avoid Them
Mistake 1: Forgetting the Mass Difference Between Electron and Proton
The error: Students often assume both particles have the same mass, or they plug in the electron mass for the proton (or vice versa).
Why it happens: The problem asks for "time of fall" for both, and it's easy to rush and use the same mass value.
How to avoid:
- Always write the mass explicitly before substituting:
- Electron: me=9.1×10−31kg
- Proton: mp=1.67×10−27kg
- Note that the proton is ~1836 times heavier — this alone tells you the proton will take much longer to fall the same distance.
Mistake 2: Ignoring the Sign of Charge When Field Reverses
The error: Students treat the reversed field as if it still pushes the proton in the same direction as the electron.
Why it happens: The problem says "direction of the field is reversed" — but the proton is positively charged, so the force direction flips relative to the electron.
How to avoid:
- Force on a charge: F=qE
- Electron (q=−e): force is opposite to E
- Proton (q=+e): force is along E
- When the field reverses, the electron would reverse direction too — but here the electron falls before reversal, and the proton falls after reversal.
- Key insight: In both cases, the particle is accelerated downward (toward the lower plate). The reversal ensures the proton also falls, not rises.
Mistake 3: Using g Instead of Electric Acceleration
The error: Students treat this as free fall under gravity and use t=2h/g.
Why it happens: The problem explicitly asks to "contrast with free fall under gravity," but students sometimes mix the two.
How to avoid:
- The acceleration here is NOT g. It comes from the electric force:
a=mF=mqE
- For the electron: ae=meeE
- For the proton: ap=mpeE
- Then use s=21at2 → t=a2s
Mistake 4: Forgetting That Both Charges Have Magnitude e
The error: Students think the proton has charge +e and the electron −e, but then use different magnitudes of charge in the force equation.
Why it happens: The sign matters for direction, but the magnitude of charge is the same: e=1.6×10−19C.
How to avoid:
- Write: ∣qe∣=∣qp∣=e
- The force magnitude is eE for both — only the mass differs.
Mistake 5: Not Contrasting with Free Fall Properly
The error: Students compute the times but don't explain why the comparison matters.
Why it happens: The question says "Contrast the situation," but students treat it as an afterthought.
How to avoid:
- Free fall under gravity:
tfree fall=g2h(g≈9.8m/s2)
- Electric case:
telectric=eE2hm
- Key contrast:
- In free fall, all objects fall with same acceleration g (ignoring air resistance).
- In an electric field, acceleration depends on mass — the electron falls ~1836× faster than the proton.
- Also, gravity always pulls downward; electric force direction depends on charge sign.
Quick Checklist to Avoid These Mistakes
| Step | What to Check |
|---|---|
| 1 | ✓ Write me and mp separately |
| 2 | ✓ Confirm force direction using F=qE |
| 3 | ✓ Use a=qE/m, not g |
| 4 | ✓ Use $ |
| 5 | ✓ Explain: same E → different a → different t |
Final Answer (for reference)
Electron:
ae=meeE=9.1×10−31(1.6×10−19)(2.0×104)≈3.52×1015m/s2
te=3.52×10152×0.015≈2.92×10−9s
Proton:
ap=mpeE=1.67×10−27(1.6×10−19)(2.0×104)≈1.92×1012m/s2
tp=1.92×10122×0.015≈1.25×10−7s
Contrast: Under gravity, both would take 2h/g≈0.055s — much slower than the electron, but faster than the proton. The electric field discriminates by mass, while gravity does not.
- COMEDK 2024Set 2024-A1 markMCQQ.An electron starting from rest and moving with the velocity v through a potential difference V is shown by the graphs below. Identify the correct graph. (A) (B) (C) (D)
›Reveal solutionSolution
[!TLDR]
Energy conservation gives v∝V, whose graph is a concave-down curve from the origin — option (C).
Concept
An electron accelerated from rest through a potential difference V gains kinetic energy equal to the work done on it: eV=21mv2 (CBSE Class 12 electrostatic potential).
Solution
From energy conservation:
eV=21mv2⟹v=m2eV∝V.
So v increases as the square root of V. A V curve:
- passes through the origin (at V=0, v=0),
- rises steeply at first,
- then bends over with a decreasing slope (concave downward), flattening at large V.
This matches option (C). Option (A) is concave-up (wrong curvature), while (B) and (D) are straight lines (a linear v–V relation, which is incorrect).
[!ANSWER]
(C) the concave-down curve from the origin (square-root shape)
NoteThis solution was worked out by our team and independently cross-checked by a second solve. The official answer key on record for this question could not be confirmed, so please cross-verify with the official paper where possible.
- KCET 2023Set A-31 markMCQQ.A charged particle is subjected to acceleration in a cyclotron as shown. The charged particle undergoes increase in its speed (A) Only inside D2 (B) Inside D1, D2 and the gaps (C) Only inside D1 (D) Only in the gap between D1 and D2
›Reveal solutionSolution
Magnetic forces do no work, and the dees are field-free conductors inside — so the particle can only gain speed in the electric field across the gap.
Step 1 — What happens inside a dee
The dees D1 and D2 are hollow metal (conducting) chambers. Inside a conductor's cavity the electric field is zero — the alternating potential difference exists only across the gap between the dees. So inside a dee the only force on the particle is the magnetic force.
Step 2 — Magnetic force does no work
The magnetic force is
F=qv×B,
which is always perpendicular to v. Hence the power delivered is
P=F⋅v=q(v×B)⋅v=0.
Zero work ⇒ zero change in kinetic energy ⇒ the speed is constant inside each dee. The magnetic field only bends the path into a semicircle of radius r=qBmv.
Step 3 — What happens in the gap
Each time the particle crosses the gap, the oscillating source (tuned to the cyclotron frequency f=2πmqB) has reversed polarity so that the electric field always accelerates it. Work done per crossing:
W=qV⇒Δ(21mv2)=qV>0.
This is the only place the speed increases — after each crossing the radius r=mv/(qB) is larger, giving the familiar spiral of ever-widening semicircles.
Step 4 — Conclusion
Speed increases only in the gap between D1 and D2; inside both dees the speed is unchanged (only the direction changes).
✓Final answerThe correct option is (D) — Only in the gap between D1 and D2.
ANSWER: D
- KCET 2020Set A-11 markMCQQ.A cyclotron is used to accelerate protons (11H), Deuterons (12H) and α-particles (24He). While exiting under similar conditions, the minimum K.E. is gained by (A) α-particle (B) proton (C) deuteron (D) same for all
›Reveal solutionSolution
Cyclotron exit energy is K=q2B2R2/2m, so for the same machine the answer is decided purely by the charge-squared-to-mass ratio q2/m — smallest for the deuteron.
Step 1 — Derive the exit kinetic energy.
Inside a cyclotron the magnetic force supplies the centripetal force:
qvB=Rmv2 ⟹ v=mqBR
The particle leaves at the outermost radius R (the dee radius), so its exit speed is that v. Therefore
K=21mv2=21m(mqBR)2
K=2mq2B2R2
Step 2 — Identify what varies.
"Similar conditions" means the same cyclotron: the same B and the same exit radius R. So
K ∝ mq2
This is why the answer is not simply "the heaviest" or "the most charged" — charge enters squared, mass only to the first power.
Step 3 — Tabulate q2/m (charge in units of e, mass in units of u).
Particle q m q2/m K (relative) Proton 11H 1 1 1/1=1.0 1.0 Deuteron 12H 1 2 1/2=0.5 0.5 α-particle 24He 2 4 4/4=1.0 1.0 Step 4 — Read off the minimum.
The proton and the α-particle happen to tie (q2/m=1 for both — the α's doubled charge is exactly cancelled by its quadrupled mass). The deuteron is the odd one out with q2/m=0.5, so it gains only half their kinetic energy.
✓Final answerThe correct option is (C) — deuteron.
ANSWER: C
- KCET 2019Set A-11 markMCQQ.In a cyclotron a charged particle (A) undergoes acceleration all the time (B) speeds up between the dees because of the magnetic field. (C) speeds up in dee (D) slows down within a dee and speeds up between dees
›Reveal solutionSolution
In a cyclotron, the electric field between the dees accelerates the particle, while the magnetic field inside each dee bends it into a circular path — so the particle undergoes acceleration all the time, both in direction (magnetic force) and in speed (electric field between dees).
The key to this question is understanding what causes acceleration in a cyclotron. Acceleration is any change in velocity — either in magnitude (speed) or direction. A charged particle moving in a magnetic field experiences a force perpendicular to its velocity, which changes only its direction, not its speed. Inside the dees (the hollow D-shaped electrodes), the magnetic field is uniform and the electric field is zero, so the particle moves in a circular arc at constant speed. Between the dees, there is a rapidly alternating electric field that gives the particle a kick, increasing its kinetic energy each time it crosses the gap.
So the particle is always accelerating:
- Inside a dee: centripetal acceleration due to the magnetic field (direction changes, speed constant).
- Between the dees: linear acceleration due to the electric field (speed increases).
Now let’s examine each option.
-
Option (A): "undergoes acceleration all the time"
This is true. Inside the dee, the magnetic force provides centripetal acceleration (changing direction). Between the dees, the electric field provides tangential acceleration (changing speed). There is no point in the cyclotron where the particle moves with constant velocity.
-
Option (B): "speeds up between the dees because of the magnetic field"
This is false. The magnetic field never changes the speed of a charged particle — it only changes its direction. The speed increase between the dees is due to the electric field, not the magnetic field.
-
Option (C): "speeds up in dee"
This is false. Inside a dee, the electric field is zero (the dees are shielded conductors). The particle coasts at constant speed along its circular arc. No speeding up happens inside.
-
Option (D): "slows down within a dee and speeds up between dees"
This is false. Within a dee, the particle does not slow down — it moves at constant speed. The only change in speed occurs in the gap between dees, where it speeds up.
Watch outA common mistake is to think that because the particle moves in a circle inside the dee, it must be accelerating only there. But acceleration includes both change in speed and change in direction — the magnetic field gives the former, the electric field gives the latter. The phrase "undergoes acceleration" covers both.
TipRemember the cyclotron's division of labour:
- Magnetic field → bends the path (centripetal acceleration)
- Electric field → boosts the speed (tangential acceleration) The particle is always under one or the other, so it is always accelerating.
✓Final answerThe correct option is (A) — the particle undergoes acceleration all the time.
- KCET 2019Set A-11 markMCQQ.Which one of the following nuclei has shorter mean life?
(A) A (B) B (C) C (D) Same for all
›Reveal solutionSolution
The activity curve that decays fastest has the largest decay constant λ, and since the mean life is τ=1/λ, that curve (A) has the shortest mean life.
Step 1 — the law being plotted.
Radioactive decay gives N=N0e−λt, so the activity plotted on the vertical axis is
dtdN=λN0e−λt.
All three curves start from the same point on the dN/dt axis, i.e. they have the same initial activity.
Step 2 — read the graph.
At any later time t, curve A lies lowest (it drops off most rapidly) and curve C lies highest (it decays most slowly). Since
(dN/dt)C(dN/dt)A=e−(λA−λC)t,
A being below C for all t>0 requires λA>λB>λC.
Step 3 — connect λ to the mean life.
The mean (average) life of a nucleus is
τ=λ1.
So the largest λ corresponds to the shortest mean life. Since λA is the largest, τA is the smallest:
τA<τB<τC.
Step 4 — conclude. Nucleus A has the shortest mean life.
✓Final answerThe correct option is (A) — A.
ANSWER: A
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