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.

  • GCE A-Level H1 Physics 2027

H1 Physics 8867 · Lesson 1 of 3

Check your understanding

By 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/t
  • Q = nAvtq
  • I = 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.

  1. 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.

  2. Step 2: Rearrange the carrier equation

    Why: All contributing carriers are represented by n, A and q.

    Working: v = I/(nAq).

  3. 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

  1. Convert minutes to seconds.
  2. 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

  1. Uses A = 1.2 × 10⁻⁶ m².
  2. Obtains v ≈ 1.84 × 10⁻⁴ m s⁻¹.
  3. Uses t = 240 s.
  4. Obtains Q = 720 C.
  5. States the electric field/signal is established around the circuit rapidly.
  6. 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

  1. Define electric current.

    Check

    Rate of flow of charge through a cross-section.

  2. How does electron drift direction compare with conventional current?

    Check

    It is opposite.

  3. What does n mean in I = nAvq?

    Check

    Number of mobile charge carriers per unit volume.

Try this next

Move from charge per second to energy per coulomb in the potential-difference lesson.

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