AQA · A-Level · Physics

    Course version: 7408 · Version from Sept 2016

    No work done moving charge along an equipotential surface.

    Full specification wording

    Electric potential (A-level only): No work done moving charge along an equipotential surface.

    An equipotential surface is a surface on which the electric potential is constant.

    Checked against the AQA 7408 specification (opens in a new tab) on .

    • Point 3 of 3
    • 3 key terms

    Study notes

    From the checked teaching notes for this specification point.

    The idea

    An equipotential surface is a surface on which the electric potential is constant. Since potential difference ΔV between any two points on the surface is zero, the work done W = QΔV is also zero. This is because the electric force is always perpendicular to the equipotential surface, so the component of force along the direction of motion is zero. For example, moving a charge around a circular equipotential centred on a point charge requires no work, even though the charge experiences a force. This principle is used in understanding conductors in electrostatic equilibrium, where the surface is an equipotential, and in the design of particle accelerators where particles move along equipotentials without energy change.

    What earns the marks

    • State that on an equipotential surface, the potential difference between any two points is zero (ΔV = 0).
    • Apply W = QΔV to show that if ΔV = 0, then W = 0, regardless of the magnitude of Q.
    • Explain that the electric force is perpendicular to the equipotential surface, so the force has no component along the displacement.
    • Relate this to the definition of work done: W = Fs cosθ, where θ = 90°, so cos90° = 0 and W = 0.
    • Give a practical example, such as a charge moving on a spherical equipotential around a point charge, or a charge moving along the surface of a charged conductor.

    Common mistakes and how to put them right

    • Assuming that because a force acts on the charge, work must be done.

      Put it right: Work depends on the component of force along the displacement; perpendicular forces do no work.

    • Thinking that moving along an equipotential changes the potential energy of the charge.

      Put it right: Potential energy depends on potential, which is constant, so it does not change.

    • Confusing equipotential surfaces with electric field lines.

      Put it right: Equipotentials are perpendicular to field lines and represent constant potential, while field lines show the direction of force on a positive charge.

    Exam tips

    • When asked why no work is done, explicitly state that ΔV = 0 and that the electric force is perpendicular to the displacement.
    • Use the equation W = QΔV to justify the zero work done, and mention that Q is not zero but ΔV is zero.
    • If a diagram is given, identify the equipotential surface and show that the path lies along it, then explain the perpendicularity of force and motion.

    Try the lesson

    The start of the Electric potential (A-level only): No work done moving charge along an equipotential surface. lesson, made from checked teaching notes for this specification point.

    Have a go first

    A charge is moved from one point to another on the same equipotential surface. What is the work done in moving the charge?

    Listen

    An equipotential surface is a surface on which the electric potential is constant. Since potential difference ΔV between any two points on the surface is zero, the work done W = QΔV is also zero. This is because the electric force is always perpendicular to the equipotential surface, so the component of force along the direction of motion is zero. For example, moving a charge around a circular equipotential centred on a point charge requires no work, even though the charge experiences a force. This principle is used in understanding conductors in electrostatic equilibrium, where the surface is an equipotential, and in the design of particle accelerators where particles move along equipotentials without energy change. A strong answer earns marks for these points. State that on an equipotential surface, the potential difference between any two points is zero (ΔV = 0). Apply W = QΔV to show that if ΔV = 0, then W = 0, regardless of the magnitude of Q. Explain that the electric force is perpendicular to the equipotential surface, so the force has no component along the displacement. Relate this to the definition of work done: W = Fs cosθ, where θ = 90°, so cos90° = 0 and W = 0. A common slip: Assuming that because a force acts on the charge, work must be done. Instead, work depends on the component of force along the displacement; perpendicular forces do no work. Exam tip: When asked why no work is done, explicitly state that ΔV = 0 and that the electric force is perpendicular to the displacement.

    See it

    A top-down flowchart. The top node reads 'Charge moves along an equipotential surface' and branches into two nodes. The left branch node reads 'Potential difference between any two points is zero (ΔV = 0)' and leads to 'W = QΔV gives W = 0, regardless of the magnitude of Q'. The right branch node reads 'Electric force is perpendicular to the equipotential surface' and leads to 'No component of force along the displacement', which leads to 'W = Fs cosθ with θ = 90°, so cos90° = 0 and W = 0'. Both the W = QΔV node and the W = Fs cosθ node lead to a final node reading 'No work done'.
    Two routes to the same conclusion that no work is done on a charge moving along an equipotential surface: through ΔV = 0 in W = QΔV, and through the electric force being perpendicular to the displacement.

    Key words

    Say what each word means before you turn the card.

    Equipotential surfaces

    Try answering aloud or in your head before turning the card.

    Work done in electric fields

    Try answering aloud or in your head before turning the card.

    Perpendicularity of force and displacement

    Try answering aloud or in your head before turning the card.

    See every definition
    Equipotential surfaces
    A surface on which the electric potential is constant, so the potential difference between any two points on it is zero.
    Work done in electric fields
    Given by W = QΔV, so it is zero when ΔV is zero, regardless of the magnitude of Q.
    Perpendicularity of force and displacement
    The electric force is always perpendicular to the equipotential surface, so the force has no component along the displacement.

    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 top node reads 'Charge moves along an equipotential surface' and branches into two nodes. The left branch node reads 'Potential difference between any two points is zero (ΔV = 0)' and leads to 'W = QΔV gives W = 0, regardless of the magnitude of Q'. The right branch node reads 'Electric force is perpendicular to the equipotential surface' and leads to 'No component of force along the displacement', which leads to 'W = Fs cosθ with θ = 90°, so cos90° = 0 and W = 0'. Both the W = QΔV node and the W = Fs cosθ node lead to a final node reading 'No work done'.
    • 1Box 1

    • 2Box 2

    • 3Box 3

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