OCR · A-Level · Physics

    Course version: H556 · Version from Sept 2015

    Mean drift velocity: (a) mean drift velocity of charge carriers

    In a conductor, charge carriers move randomly with high speeds but with no net displacement until an electric field is applied.

    Checked against the OCR H556 specification (opens in a new tab) on .

    • Point 1 of 3
    • 4 key terms

    Study notes

    From the checked teaching notes for this specification point.

    The idea

    In a conductor, charge carriers move randomly with high speeds but with no net displacement until an electric field is applied. The field gives each carrier a small average velocity along the conductor, called the mean drift velocity v. The current is I = nAvq, where n is the number density of charge carriers, A is the cross-sectional area, v is the mean drift velocity and q is the charge on each carrier. For copper, n is about 8.5 × 10²⁸ m⁻³, so a current of 1 A in a wire of cross-sectional area 1 × 10⁻⁶ m² gives v = I ÷ (nAq) ≈ 7 × 10⁻⁵ m s⁻¹, a fraction of a millimetre per second. The random thermal speeds are much larger, around 10⁵ m s⁻¹, but average to zero.

    What earns the marks

    • Mean drift velocity is the average velocity of charge carriers along a conductor due to an applied electric field.
    • The relationship is I = nAvq, where n is the number density of charge carriers, A is the cross-sectional area, v is the mean drift velocity and q is the charge on each carrier.
    • Carriers also have much larger random thermal speeds, but these average to zero and do not contribute to the current.
    • For a given current, a smaller cross-sectional area or a smaller number density gives a larger mean drift velocity.
    • Typical values of mean drift velocity in metals are of the order of 10⁻⁵ to 10⁻⁴ m s⁻¹, far smaller than the random thermal speeds.

    Common mistakes and how to put them right

    • Confusing mean drift velocity with the speed at which the electrical signal travels.

      Put it right: The signal propagates much faster than the carriers drift.

    • Using the cross-sectional area in cm² without converting to m².

      Put it right: The equation requires SI units, so convert 1 cm² to 1 × 10⁻⁴ m².

    • Forgetting that n is the number density of charge carriers per cubic metre, not the total number of carriers in the wire.

    Exam tips

    • Rearrange I = nAvq for the quantity required before substituting values, and check that all units are SI.
    • Remember that for electrons q = 1.60 × 10⁻¹⁹ C, and use the magnitude when calculating v.
    • If a question gives the number of carriers per unit volume, use it directly as n; if it gives the total number, divide by the volume of the conductor.

    Try the lesson

    The start of the Mean drift velocity: (a) mean drift velocity of charge carriers lesson, made from checked teaching notes for this specification point.

    Listen

    In a conductor, charge carriers move randomly with high speeds but with no net displacement until an electric field is applied. The field gives each carrier a small average velocity along the conductor, called the mean drift velocity v. The current is I = nAvq, where n is the number density of charge carriers, A is the cross-sectional area, v is the mean drift velocity and q is the charge on each carrier. For copper, n is about 8.5 × 10²⁸ m⁻³, so a current of 1 A in a wire of cross-sectional area 1 × 10⁻⁶ m² gives v = I ÷ (nAq) ≈ 7 × 10⁻⁵ m s⁻¹, a fraction of a millimetre per second. The random thermal speeds are much larger, around 10⁵ m s⁻¹, but average to zero. A strong answer earns marks for these points. Mean drift velocity is the average velocity of charge carriers along a conductor due to an applied electric field. The relationship is I = nAvq, where n is the number density of charge carriers, A is the cross-sectional area, v is the mean drift velocity and q is the charge on each carrier. Carriers also have much larger random thermal speeds, but these average to zero and do not contribute to the current. For a given current, a smaller cross-sectional area or a smaller number density gives a larger mean drift velocity. Exam tip: Rearrange I = nAvq for the quantity required before substituting values, and check that all units are SI.

    See it

    A top-down flowchart. The first box says charge carriers move randomly at high speed. An arrow leads down to a box saying no net displacement. An arrow leads to a box saying electric field applied. An arrow leads to a box saying small average velocity along conductor. An arrow leads to a box saying mean drift velocity v. An arrow leads to a box saying current I = nAvq. An arrow leads to a box saying smaller area or smaller n gives larger v. Separately, an arrow from the first box leads to a box saying random thermal speeds average to zero, and an arrow from that box also leads to the current I = nAvq box.
    It shows how random carrier motion with no net displacement becomes a mean drift velocity when an electric field is applied, leading to the current equation I = nAvq.

    Key words

    Say what each word means before you turn the card.

    Mean drift velocity

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    Number density of charge carriers

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    Relationship between current and drift velocity

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    Random thermal motion versus drift motion

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    See every definition
    Mean drift velocity
    The average velocity of charge carriers along a conductor due to an applied electric field.
    Number density of charge carriers
    The number of charge carriers per cubic metre, denoted n in the equation I = nAvq.
    Relationship between current and drift velocity
    The current is I = nAvq, where n is the number density of charge carriers, A is the cross-sectional area, v is the mean drift velocity and q is the charge on each carrier.
    Random thermal motion versus drift motion
    Carriers have much larger random thermal speeds, but these average to zero and do not contribute to the current, whereas the field gives each carrier a small average velocity along the conductor.

    Label the diagram

    Some boxes have lost their names. Pick the right name for each number.

    The diagram again, with 3 boxes numbered instead of named. A top-down flowchart. The first box says charge carriers move randomly at high speed. An arrow leads down to a box saying no net displacement. An arrow leads to a box saying electric field applied. An arrow leads to a box saying small average velocity along conductor. An arrow leads to a box saying mean drift velocity v. An arrow leads to a box saying current I = nAvq. An arrow leads to a box saying smaller area or smaller n gives larger v. Separately, an arrow from the first box leads to a box saying random thermal speeds average to zero, and an arrow from that box also leads to the current I = nAvq box.
    • 1Box 1

    • 2Box 2

    • 3Box 3

    0 of 3 labelled

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