Q.The number density of free electrons in a copper conductor estimated in Example 3.1 is 8.5×1028 m−3. How long does an electron take to drift from one end of a wire 3.0 m long to its other end? The area of cross-section of the wire is 2.0×10−6 m2 and it is carrying a current of 3.0 A.
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Drift Velocity: The Slow March of Electrons
Electrons in a metal are always moving — but randomly. At room temperature they zip around at roughly 106 m/s, colliding with the lattice ions every few trillionths of a second. Without an electric field this motion cancels out: for every electron heading left another heads right, so the net velocity is zero.
Apply a battery and the field gives every electron a tiny, steady push in one direction. Between collisions the electron accelerates only briefly before smashing into an ion and losing its directed motion. What survives is a very small average velocity along the field — the drift velocity.
The random thermal speed is about 105 m/s, but the drift velocity is only about 10−4 m/s — about a billion times slower. An electron drifts slower than a snail, yet a lamp lights instantly, because the electric field (not the electrons) propagates at nearly the speed of light and starts every electron drifting almost at once.
The precise definition
Drift velocity (vd) is the average velocity acquired by the charge carriers in a conductor under an applied electric field:
vd=meEτ
where:
- e = electron charge (1.6×10−19 C)
- E = electric field inside the conductor (V/m)
- τ = average relaxation time — the mean time between collisions (s)
- m = electron mass (9.1×10−31 kg)
vd=meEτ
Linking to current
Drift velocity connects the microscopic motion of electrons to the current an ammeter reads:
I=neAvd
where n is the free-electron number density and A the cross-sectional area. A larger vd means more current, but vd stays tiny because τ is tiny (about 10−14 s in copper).
For a copper wire carrying 1 A with area 1 mm² and n≈8.5×1028 m−3:
vd=neAI≈(8.5×1028)(1.6×10−19)(10−6)1≈7×10−5 m/s …
Why this formula?
Drift Velocity: Why the Formula Holds
Let's build this from first principles — understanding why electrons drift the way they do, not just memorizing the formula.
1. The Core Idea: What is Drift Velocity?
In a conductor, free electrons are constantly moving randomly (thermal motion, speeds ~105 m/s). Without an electric field, their net displacement is zero — they're like a swarm of bees buzzing in all directions.
When we apply an electric field E, it gently nudges each electron in the opposite direction (since electrons are negatively charged). This small, steady net velocity superimposed on the random motion is drift velocity (vd).
Key insight: Drift velocity is not the speed of individual electrons — it's the average velocity of the entire electron cloud.
2. The Derivation: Step by Step
Step 1: Force on a single electron
An electron of charge −e in an electric field E experiences:
F=−eE
The magnitude of acceleration (opposite to E) is:
a=mF=meE
where m is the electron's mass.
Step 2: What happens between collisions?
Electrons don't accelerate forever — they keep colliding with atoms/ions in the metal lattice. Let the average time between collisions be τ (relaxation time). Just after a collision an electron's velocity is essentially random (zero average in the field direction); it then accelerates for time τ before the next collision.
Step 3: Drift velocity
Averaging the field-driven velocity over the relaxation time τ gives the net drift:
vd=meEτ
Here τ is the average time since the last collision, so this expression already averages over electrons at every stage between collisions — it is the standard result used in the NCERT treatment.
3. Connecting to Current: The Big Picture
Drift velocity directly gives us current density J:
J=nevd
where n = number of free electrons per unit volume. …
Concept: Drift Velocity — relates current to the average velocity of charge carriers: vd=neAI.
Given I=3.0A, n=8.5×1028m−3, e=1.6×10−19C, A=2.0×10−6m2, L=3.0m:
vd=(8.5×1028)(1.6×10−19)(2.0×10−6)3.0=2.72×1043.0≈1.10×10−4m/s …
Using vd=I/(neA), the drift speed is vd≈1.10×10−4m/s, so the time to drift the 3.0m wire is t=L/vd≈2.72×104s, which is about 7.6 hours.
Why drift velocity is the key
A current is carried by the net drift of free electrons superimposed on their much faster random thermal motion. The relation linking current to that drift speed is
I=neAvd⇒vd=neAI.
Once vd is known, the time to cross the wire's length L is simply t=L/vd.
vd=neAI,t=vdL
Step-by-step solution
1. Known quantities
- n=8.5×1028m−3
- L=3.0m
- A=2.0×10−6m2
- I=3.0A
- e=1.6×10−19C
2. Drift velocity
vd=neAI=(8.5×1028)(1.6×10−19)(2.0×10−6)3.0
Computing the denominator: ne=(8.5×1028)(1.6×10−19)=1.36×1010C/m3, and neA=(1.36×1010)(2.0×10−6)=2.72×104C/(m\cdots). So
vd=2.72×1043.0≈1.10×10−4m/s.
Check units: [n][e][A][vd]=m−3⋅C⋅m2⋅m/s=C/s=A, matching I — confirming the formula is dimensionally consistent.
3. Drift time …
Method: Drift Velocity Formula
This problem uses the drift velocity relation that connects current, charge carrier density, cross-sectional area, and drift speed.
Step-by-step solution
Step 1: Recall the formula for current in terms of drift velocity
The current I in a conductor is given by:
I=neAvd
where:
- n = number density of free electrons (8.5×1028 m−3)
- e = charge of an electron (1.6×10−19 C)
- A = cross-sectional area (2.0×10−6 m2)
- vd = drift velocity of electrons
Step 2: Solve for drift velocity vd
Rearranging:
vd=neAI
Substitute the values:
vd=(8.5×1028)(1.6×10−19)(2.0×10−6)3.0
vd=2.72×1043.0
vd=1.10×10−4 m/s
Step 3: Find the time to drift the given length
Time t is distance divided by drift velocity:
t=vdL=1.10×10−43.0
t=2.72×104 s …
Common Mistakes Students Make on Drift Velocity Problems
Mistake 1: Confusing Drift Speed with Actual Electron Speed
The error: Students often think electrons zoom through wires at near light speed. They calculate a tiny drift velocity and panic, thinking something is wrong.
Why it happens: The signal speed (≈ 3×108 m/s) is confused with drift speed (≈ 10−4 m/s). Electrons actually drift very slowly — like a snail's pace — but the electric field propagates almost instantly.
How to avoid: Remember:
- Drift velocity (vd) = net average velocity of electrons under an electric field
- Signal speed = speed at which current starts flowing (near light speed)
- A slow drift velocity is correct — expect answers in mm/s or μm/s
Mistake 2: Using Wrong Formula or Misplacing Variables
The error: Students write I=neAvd but solve for the wrong quantity, or forget that n is number density (not number of electrons).
Correct formula:
I=neAvd
where:
- I = current (A)
- n = number density (m−3)
- e = charge of electron (1.6×10−19 C)
- A = cross-sectional area (m2)
- vd = drift velocity (m/s)
How to avoid: Write the formula before plugging numbers. Solve for vd explicitly:
vd=neAI
Mistake 3: Forgetting to Convert Units
The error: Using area in cm2 or length in km without converting to SI units.
Example: 2.0×10−6 m2 is already in SI — but if given as 2.0 mm2, students forget 1 mm2=10−6 m2.
How to avoid: Always convert to metres, seconds, amperes before calculation. Write units beside every number.
Mistake 4: Stopping at Drift Velocity Instead of Finding Time
The error: The question asks: "How long does an electron take to drift from one end to the other?" Students calculate vd and stop.
What's needed: After finding vd, use:
t=vdL
where L=3.0 m.
How to avoid: Read the question twice. Underline what is being asked — here it's time, not velocity.
Mistake 5: Arithmetic Errors with Powers of 10
The error: Mismanaging exponents when dividing:
vd=(8.5×1028)(1.6×10−19)(2.0×10−6)3.0
Students often add/subtract exponents incorrectly. …
- JKBOSE Class 12 Annual Regular Examination 2024Set SZ3 marksQ.A 10 C charge flows through a wire in 5 minutes. The radius of the wire is 1 mm. It contains 5 x 10^22 electrons per centimeter^3. Calculate current and drift velocity.
›Reveal solutionSolution
Current is charge divided by time (I = Q/t); drift velocity then follows from I = nAev_d using the given electron density and wire cross-section.
Given: Q = 10 C, t = 5 min = 300 s, radius of wire r = 1 mm = 1×10⁻³ m, free-electron density n = 5×10²² per cm³.
Step 1 — Current:
I = Q/t = 10 / 300 = 0.0333 A = 3.33 × 10⁻² A
Step 2 — Convert electron density to per m³:
n = 5×10²² cm⁻³ = 5×10²² × 10⁶ m⁻³ = 5×10²⁸ m⁻³
Step 3 — Cross-sectional area:
A = πr² = π × (1×10⁻³)² = π × 1×10⁻⁶ ≈ 3.1416×10⁻⁶ m²
Step 4 — Drift velocity, from I = nAev_d:
v_d = I / (nAe)
= 0.0333 / (5×10²⁸ × 3.1416×10⁻⁶ × 1.6×10⁻¹⁹)
= 0.0333 / (2.513×10⁴)
≈ 1.33 × 10⁻⁶ m/s
…
- JKBOSE Class 12 Annual Regular Examination 2022Set SZ3 marksQ.Derive relation between Current and Drift velocity. OR Find the resistivity of wire of length 2 m, diameter 0.01 m and resistance 50 mOhm.
›Reveal solutionSolution
Either derive I=neAvd from the motion of free electrons, or use ρ=RA/L to find the resistivity of the given wire.
Part 1 — Relation between current and drift velocity
Consider a conductor of cross-sectional area A with n free electrons per unit volume, each of charge e, moving with average drift velocity vd under an applied electric field (opposite to E since electrons are negative, but we consider magnitude here).
In a small time interval Δt, each electron moves a distance vdΔt. So all electrons within a cylindrical volume of length vdΔt and cross-section A will cross a given cross-section of the conductor in this time.
Volume of this region =AvdΔt
Number of free electrons in it =nAvdΔt
Total charge crossing the cross-section in time Δt:
Δq=(nAvdΔt)e
Current is charge per unit time:
I=ΔtΔq=neAvd
…
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