OCR · A-Level · Physics

    Course version: H556 · Version from Sept 2015

    (b) a one-to-one interaction between a photon and a surface electron

    Full specification wording

    The photoelectric effect: (b) a one-to-one interaction between a photon and a surface electron

    The photoelectric effect is explained by treating light as a stream of photons, each carrying energy E = hf, where h is the Planck constant and f the frequency.

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    • Point 3 of 7
    • 3 key terms

    Study notes

    From the checked teaching notes for this specification point.

    The idea

    The photoelectric effect is explained by treating light as a stream of photons, each carrying energy E = hf, where h is the Planck constant and f the frequency. Emission occurs when a single photon is absorbed by a single electron at or near the metal surface in a one-to-one interaction. All the photon energy is transferred to that electron; it is not shared among many electrons and does not accumulate over time. The electron uses energy equal to the work function φ to escape the surface, and any surplus becomes kinetic energy. If hf is below φ, no emission occurs however intense the beam, because intensity means more photons, not more energetic ones. A useful check is to compare hf with φ for one photon and one electron.

    What earns the marks

    • A photon is a quantum of electromagnetic radiation carrying energy E = hf, where h is the Planck constant and f is the frequency.
    • In the photoelectric effect one photon interacts with one surface electron, so the interaction is one-to-one rather than spread over many electrons.
    • The whole photon energy hf is transferred to that single electron; energy is not shared or accumulated over time.
    • Emission requires hf to be at least the work function φ; surplus energy appears as kinetic energy of the emitted electron.
    • Increasing intensity increases the number of photons per second, so it increases the rate of emission, not the energy delivered per photon.

    Common mistakes and how to put them right

    • Thinking that many photons can combine their energies to release one electron.

      Put it right: The interaction is one-to-one, so a single photon must supply at least the work function.

    • Believing that a very intense low-frequency beam will eventually cause emission.

      Put it right: If hf is less than φ, no single photon has enough energy, so no emission occurs at any intensity.

    • Assuming the electron gradually absorbs energy from the wave until it escapes.

      Put it right: Absorption is a single instantaneous photon-electron event, not a gradual build-up.

    Exam tips

    • State explicitly that one photon interacts with one electron, then use E = hf to justify whether emission is possible.
    • When a question mentions intensity, translate it into photons per second and link that to emission rate rather than to electron energy.
    • Check the frequency against the threshold before discussing kinetic energy, so your reasoning follows the one-to-one condition.

    Try the lesson

    The start of the The photoelectric effect: (b) a one-to-one interaction between a photon and a surface electron lesson, made from checked teaching notes for this specification point.

    Listen

    The photoelectric effect is explained by treating light as a stream of photons, each carrying energy E = hf, where h is the Planck constant and f the frequency. Emission occurs when a single photon is absorbed by a single electron at or near the metal surface in a one-to-one interaction. All the photon energy is transferred to that electron; it is not shared among many electrons and does not accumulate over time. The electron uses energy equal to the work function φ to escape the surface, and any surplus becomes kinetic energy. If hf is below φ, no emission occurs however intense the beam, because intensity means more photons, not more energetic ones. A useful check is to compare hf with φ for one photon and one electron. A strong answer earns marks for these points. A photon is a quantum of electromagnetic radiation carrying energy E = hf, where h is the Planck constant and f is the frequency. In the photoelectric effect one photon interacts with one surface electron, so the interaction is one-to-one rather than spread over many electrons. The whole photon energy hf is transferred to that single electron; energy is not shared or accumulated over time. Emission requires hf to be at least the work function φ; surplus energy appears as kinetic energy of the emitted electron. A common slip: Thinking that many photons can combine their energies to release one electron. Instead, the interaction is one-to-one, so a single photon must supply at least the work function. Exam tip: State explicitly that one photon interacts with one electron, then use E = hf to justify whether emission is possible.

    See it

    A top-down flowchart. A single photon arrives with energy E = hf, which leads to a one-to-one interaction with one surface electron. The whole photon energy hf is transferred to that electron. A decision then asks whether hf is at least the work function φ. If yes, the electron escapes the surface and the surplus energy becomes kinetic energy. If no, there is no emission, however intense the beam. Separately, increasing intensity means more photons per second, which increases the rate of emission, not the energy per photon.
    Shows the one-to-one photon-electron interaction and how comparing hf with the work function decides whether emission occurs.

    Key words

    Say what each word means before you turn the card.

    Photon

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    One-to-one interaction

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    Work function

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    See every definition
    Photon
    A quantum of electromagnetic radiation carrying energy E = hf, where h is the Planck constant and f is the frequency.
    One-to-one interaction
    A single photon is absorbed by a single electron at or near the metal surface, rather than the interaction being spread over many electrons.
    Work function
    The energy φ that the electron uses to escape the surface, with any surplus becoming kinetic energy.

    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. A single photon arrives with energy E = hf, which leads to a one-to-one interaction with one surface electron. The whole photon energy hf is transferred to that electron. A decision then asks whether hf is at least the work function φ. If yes, the electron escapes the surface and the surplus energy becomes kinetic energy. If no, there is no emission, however intense the beam. Separately, increasing intensity means more photons per second, which increases the rate of emission, not the energy per photon.
    • 1Box 1

    • 2Box 2

    • 3Box 3

    0 of 3 labelled

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