AQA · A-Level · Physics

    Course version: 7408 · Version from Sept 2016

    LC resonance filters (A-level only): Inductance as mass analogy.

    In an LC circuit, the inductor opposes changes in current, just as mass opposes changes in velocity.

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

    • Point 2 of 4
    • 4 key terms

    Study notes

    From the checked teaching notes for this specification point.

    The idea

    In an LC circuit, the inductor opposes changes in current, just as mass opposes changes in velocity. Energy stored in the magnetic field of an inductor, ½LI², plays the role of kinetic energy, ½mv². A larger inductance L means a slower build-up or decay of current for a given potential difference, mirroring how a larger mass accelerates less under the same force. This analogy helps explain why the angular frequency of free oscillations is ω = 1/√(LC): the inductor behaves like the inertial mass and the capacitor like the spring. When analysing a circuit, treat current as the analogue of velocity and charge as the analogue of displacement, so the inductor's back e.m.f. corresponds to inertia.

    What earns the marks

    • States that an inductor opposes change of current, analogous to mass opposing change of velocity.
    • Links magnetic field energy ½LI² to kinetic energy ½mv².
    • Explains that larger L gives slower current change for a given p.d., as larger mass gives smaller acceleration for a given force.
    • Uses the analogy to justify ω = 1/√(LC) for free oscillations in an ideal LC circuit.
    • Identifies current as the analogue of velocity and charge as the analogue of displacement.

    Common mistakes and how to put them right

    • Treating inductance as a source of energy rather than a store.

      Put it right: The magnetic field stores energy and returns it to the circuit.

    • Confusing the mass analogy with resistance.

      Put it right: Resistance dissipates energy, whereas mass and inductance store it.

    • Assuming the analogy means the inductor has literal mass.

      Put it right: It is a mathematical and conceptual correspondence only.

    Exam tips

    • Use the analogy to explain why increasing L lowers the resonant frequency.
    • When deriving ω, compare the energy expressions ½LI² and ½mv² to show the parallel.
    • State clearly that the analogy is between electrical and mechanical oscillators, not a physical identity.

    Try the lesson

    The start of the LC resonance filters (A-level only): Inductance as mass analogy. lesson, made from checked teaching notes for this specification point.

    Have a go first

    In the mass–spring analogy for an LC circuit, which electrical quantity plays the role of the mass?

    Listen

    In an LC circuit, the inductor opposes changes in current, just as mass opposes changes in velocity. Energy stored in the magnetic field of an inductor, ½LI², plays the role of kinetic energy, ½mv². A larger inductance L means a slower build-up or decay of current for a given potential difference, mirroring how a larger mass accelerates less under the same force. This analogy helps explain why the angular frequency of free oscillations is ω = 1/√(LC): the inductor behaves like the inertial mass and the capacitor like the spring. When analysing a circuit, treat current as the analogue of velocity and charge as the analogue of displacement, so the inductor's back e.m.f. corresponds to inertia. A strong answer earns marks for these points. States that an inductor opposes change of current, analogous to mass opposing change of velocity. Links magnetic field energy ½LI² to kinetic energy ½mv². Explains that larger L gives slower current change for a given p.d., as larger mass gives smaller acceleration for a given force. Uses the analogy to justify ω = 1/√(LC) for free oscillations in an ideal LC circuit. A common slip: Treating inductance as a source of energy rather than a store. Instead, the magnetic field stores energy and returns it to the circuit. Exam tip: Use the analogy to explain why increasing L lowers the resonant frequency.

    See it

    A top-down flowchart with six parallel pairings. The first pairs the inductor opposing change of current with mass opposing change of velocity. The second pairs magnetic field energy ½LI² with kinetic energy ½mv². The third pairs a larger L giving slower current change for a given p.d. with a larger mass giving smaller acceleration for a given force. The fourth pairs current with velocity. The fifth pairs charge with displacement. The sixth pairs the inductor as inertial mass and capacitor as spring with the angular frequency ω = 1/√(LC).
    It shows the correspondence between the electrical LC circuit and the mechanical mass–spring oscillator, including the energy and frequency parallels.

    Key words

    Say what each word means before you turn the card.

    Energy storage in magnetic fields

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

    Inertia and opposition to change

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

    Simple harmonic motion analogy

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

    Resonance in LC circuits

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

    See every definition
    Energy storage in magnetic fields
    The magnetic field of an inductor stores energy as ½LI², which plays the role of kinetic energy ½mv².
    Inertia and opposition to change
    An inductor opposes changes in current, just as mass opposes changes in velocity, and its back e.m.f. corresponds to inertia.
    Simple harmonic motion analogy
    The inductor behaves like the inertial mass and the capacitor like the spring, with current the analogue of velocity and charge the analogue of displacement.
    Resonance in LC circuits
    The angular frequency of free oscillations is ω = 1/√(LC), justified by treating the inductor as inertial mass and the capacitor as the spring.

    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 with six parallel pairings. The first pairs the inductor opposing change of current with mass opposing change of velocity. The second pairs magnetic field energy ½LI² with kinetic energy ½mv². The third pairs a larger L giving slower current change for a given p.d. with a larger mass giving smaller acceleration for a given force. The fourth pairs current with velocity. The fifth pairs charge with displacement. The sixth pairs the inductor as inertial mass and capacitor as spring with the angular frequency ω = 1/√(LC).
    • 1Box 1

    • 2Box 2

    • 3Box 3

    0 of 3 labelled

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