Current, charge flow and drift velocity
Key idea: Current measures charge flow rate. The drift model connects that circuit-scale quantity to the slow average motion of many charge carriers.
Continue where you stopped
The core idea
H1 Physics 8867 · Lesson 1 of 3
Check your understandingBy the end of this lesson, you should be able to
- Use I = Q/t for steady or average current.
- Derive I = nAvq from a carrier model.
- Distinguish carrier drift speed from the much faster establishment of an electric field around a circuit.
Learn the idea
Big question: If electrons drift slowly, why does a lamp respond almost as soon as the switch closes?
Define current at a chosen cross-section
Current is charge crossing a chosen section per unit time: I = Q/t for a steady or average current. Conventional current follows the direction positive charge would move; electron drift in a metal is opposite.
Current is not used up by a component. In a steady series circuit, charge does not build up inside a lamp, so the same charge per second enters and leaves it.
Check your understanding: A current of 2 A enters a lamp steadily. How much current leaves it?
2 A. Energy is transferred in the lamp, but charge flow is conserved.
Build the drift equation
In time t, carriers with drift speed v move distance vt. The cylinder of carriers crossing area A has volume Avt, contains nAvt carriers and carries charge nAvtq. Dividing by time gives I = nAvq, with q as carrier-charge magnitude.
Drift can be slow because the carrier density is enormous. The lamp responds quickly because an electric field is established around the whole circuit; it does not wait for one electron to travel from switch to lamp.
Check your understanding: If wire area doubles while current, n and q stay fixed, what happens to drift speed?
It halves because v = I/(nAq).
Key ideas
- Current is not used up by a component.
- Convert mm² to m² before using the drift equation.
- State whether q is charge magnitude when discussing electrons.
Relationships to know
I = Q/tQ = nAvtqI = nAvq
Follow the reasoning
Worked example
Find drift speed with a careful area conversion
Question: A 1.8 A current flows in a metal wire of diameter 0.80 mm. The electron number density is 8.5 × 10²⁸ m⁻³. Find drift speed using e = 1.60 × 10⁻¹⁹ C.
Step 1: Convert radius and area
Why: The equation requires area in m², and diameter must first be halved.
Working: r = 0.40 mm = 4.0 × 10⁻⁴ m; A = πr² = 5.03 × 10⁻⁷ m².
Step 2: Rearrange the carrier equation
Why: All contributing carriers are represented by n, A and q.
Working: v = I/(nAq).
Step 3: Substitute
Why: Keeping powers of ten visible avoids confusing mm with mm².
Working: v = 1.8/[(8.5 × 10²⁸)(5.03 × 10⁻⁷)(1.60 × 10⁻¹⁹)] = 2.63 × 10⁻⁴ m s⁻¹.
Answer: The electron drift speed is about 2.6 × 10⁻⁴ m s⁻¹, opposite to conventional current.
Check: The very small speed is plausible because about 10²⁹ carriers occupy each cubic metre.
Now try it with support
Practise with support
A steady current of 0.80 A flows for 3.0 min. Find the charge that passes.
Hints
- Convert minutes to seconds.
- Rearrange I = Q/t.
View the guided answer
t = 180 s, so Q = It = 0.80(180) = 144 C.
Your turn
Practise independently
Find the drift speed in a 1.0 mm² wire carrying 2.0 A if n = 8.5 × 10²⁸ m⁻³ and q = 1.60 × 10⁻¹⁹ C.
Check your answer
A = 1.0 mm² = 1.0 × 10⁻⁶ m². v = I/(nAq) = 2.0/[(8.5 × 10²⁸)(1.0 × 10⁻⁶)(1.60 × 10⁻¹⁹)] = 1.47 × 10⁻⁴ m s⁻¹.
Common mistakes and exam guidance
Watch out for
- Using 1 mm² = 10⁻³ m².
- Equating drift speed with the speed at which the circuit responds.
In an exam
- Show the carrier-volume step when asked to derive I = nAvq.
- Include the area conversion explicitly; it is a frequent source of powers-of-ten errors.
Put the ideas together
Exam-style practice [6 marks]
A copper wire of cross-sectional area 1.2 mm² carries 3.0 A. Take n = 8.5 × 10²⁸ m⁻³ and e = 1.60 × 10⁻¹⁹ C. Calculate electron drift speed and the charge passing in 4.0 min. Explain why the circuit can respond much faster than the drift time along the wire.
Plan before you answer
- Convert mm² and minutes separately.
- Use I = nAvq and Q = It.
- Distinguish field establishment from carrier drift.
View the marking points and model answer
Marking points
- Uses A = 1.2 × 10⁻⁶ m².
- Obtains v ≈ 1.84 × 10⁻⁴ m s⁻¹.
- Uses t = 240 s.
- Obtains Q = 720 C.
- States the electric field/signal is established around the circuit rapidly.
- States individual electrons need not travel from source to component.
Model answer
v = 3.0/[(8.5 × 10²⁸)(1.2 × 10⁻⁶)(1.60 × 10⁻¹⁹)] = 1.84 × 10⁻⁴ m s⁻¹. In 4.0 min, Q = It = 3.0(240) = 720 C. Closing the switch establishes an electric field around the circuit rapidly, so nearby carriers everywhere begin drifting; no electron has to cross the whole circuit first.
Finish from memory
Three-question recap
Define electric current.
Check
Rate of flow of charge through a cross-section.
How does electron drift direction compare with conventional current?
Check
It is opposite.
What does n mean in I = nAvq?
Check
Number of mobile charge carriers per unit volume.
Continue with the next resource in this course.
Course and syllabus information
- Course
- GCE A-Level H1 Physics
- Edition
- GCE A-Level H1 Physics 2027