AQA · A-Level · Physics

    Course version: 7408 · Version from Sept 2016

    Absorption of X-rays (A-level only): Exponential attenuation.

    When a narrow beam of X-rays passes through matter, photons are removed by absorption and scattering, so the beam intensity falls.

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

    • 4 key terms

    Study notes

    From the checked teaching notes for this specification point.

    The idea

    When a narrow beam of X-rays passes through matter, photons are removed by absorption and scattering, so the beam intensity falls. Because each thin layer removes a constant fraction of the photons still present, the decrease is exponential rather than linear. The transmitted intensity I after thickness x is I = I₀e^(−μx), where I₀ is the incident intensity and μ is the attenuation coefficient, measured in m⁻¹. A larger μ or a thicker absorber gives a smaller I. Taking natural logarithms gives ln I = ln I₀ − μx, so a graph of ln I against x is a straight line of gradient −μ. The half-value thickness x½, where I = I₀/2, is related to μ by x½ = ln 2 / μ. This explains why radiographers choose photon energies and shielding thicknesses carefully.

    What earns the marks

    • States that intensity decreases exponentially with absorber thickness because each equal layer removes the same fraction of the photons remaining.
    • Recalls and applies I = I₀e^(−μx), identifying I₀ as incident intensity, I as transmitted intensity, μ as attenuation coefficient and x as thickness.
    • Uses the linear form ln I = ln I₀ − μx to find μ from the gradient of a graph of ln I against x.
    • Calculates half-value thickness from x½ = ln 2 / μ and explains that it is independent of the initial intensity.
    • Explains that μ depends on the material and on photon energy, so comparison of absorbers requires like-for-like conditions.
    • Interprets a steeper exponential curve or larger gradient as a larger attenuation coefficient and therefore a more strongly attenuating material.

    Common mistakes and how to put them right

    • Treating attenuation as linear and subtracting a fixed intensity for each centimetre.

      Put it right: The correct model is a constant fractional decrease, giving an exponential curve.

    • Using logarithms to base ten when the equation is written with e.

      Put it right: Either use natural logarithms throughout or convert the coefficient consistently.

    • Forgetting to convert thickness to metres before dividing by μ, which gives a value of μ in the wrong unit.

      Put it right: Convert mm or cm to m first.

    • Assuming half-value thickness depends on I₀.

      Put it right: It is fixed by μ alone, so doubling the incident intensity does not change x½.

    Exam tips

    • Write the exponential equation before substituting numbers, then rearrange symbolically so the examiner can follow your method.
    • When a graph of ln I against x is given, read the gradient from well-separated points on the line of best fit and quote μ with the unit m⁻¹.
    • Check that your answer for transmitted intensity is less than the incident intensity; a value greater than I₀ signals a sign or rearrangement error.
    • Link each calculation back to the physical situation, for example stating that a larger μ means more photons are removed per metre.

    Try the lesson

    The start of the Absorption of X-rays (A-level only): Exponential attenuation. lesson, made from checked teaching notes for this specification point.

    Have a go first

    A parallel beam of X-rays passes through a uniform absorber. Which statement describes how the intensity of the beam changes as the thickness of the absorber increases?

    Listen

    When a narrow beam of X-rays passes through matter, photons are removed by absorption and scattering, so the beam intensity falls. Because each thin layer removes a constant fraction of the photons still present, the decrease is exponential rather than linear. The transmitted intensity I after thickness x is I = I₀e^(−μx), where I₀ is the incident intensity and μ is the attenuation coefficient, measured in m⁻¹. A larger μ or a thicker absorber gives a smaller I. Taking natural logarithms gives ln I = ln I₀ − μx, so a graph of ln I against x is a straight line of gradient −μ. The half-value thickness x½, where I = I₀/2, is related to μ by x½ = ln 2 / μ. This explains why radiographers choose photon energies and shielding thicknesses carefully. A strong answer earns marks for these points. States that intensity decreases exponentially with absorber thickness because each equal layer removes the same fraction of the photons remaining. Recalls and applies I = I₀e^(−μx), identifying I₀ as incident intensity, I as transmitted intensity, μ as attenuation coefficient and x as thickness. Uses the linear form ln I = ln I₀ − μx to find μ from the gradient of a graph of ln I against x. Calculates half-value thickness from x½ = ln 2 / μ and explains that it is independent of the initial intensity. Exam tip: Write the exponential equation before substituting numbers, then rearrange symbolically so the examiner can follow your method.

    See it

    A top-down flowchart. The first node is incident intensity I₀, which leads to a narrow X-ray beam entering the absorber. This leads to photons being removed by absorption and scattering, then to each thin layer removing a constant fraction of the remaining photons, and then to the intensity falling exponentially rather than linearly. That leads to the transmitted intensity I = I₀e^(−μx). From this equation three branches emerge: a larger μ or a thicker absorber gives a smaller I; ln I = ln I₀ − μx means a graph of ln I against x is a straight line with gradient −μ; and the half-value thickness is x½ = ln 2 / μ.
    It shows how a narrow X-ray beam is attenuated exponentially through an absorber, leading to the exponential equation, the logarithmic graph and the half-value thickness.

    Key words

    Say what each word means before you turn the card.

    Exponential attenuation

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    Attenuation coefficient

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    Half-value thickness

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    Graphical analysis using natural logarithms

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    See every definition
    Exponential attenuation
    The decrease in beam intensity is exponential rather than linear because each thin layer removes a constant fraction of the photons still present.
    Attenuation coefficient
    The quantity μ in I = I₀e^(−μx), measured in m⁻¹, where a larger value or a thicker absorber gives a smaller transmitted intensity.
    Half-value thickness
    The thickness x½ at which I = I₀/2, related to μ by x½ = ln 2 / μ and independent of the initial intensity.
    Graphical analysis using natural logarithms
    Taking natural logarithms gives ln I = ln I₀ − μx, so a graph of ln I against x is a straight line of gradient −μ.

    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 node is incident intensity I₀, which leads to a narrow X-ray beam entering the absorber. This leads to photons being removed by absorption and scattering, then to each thin layer removing a constant fraction of the remaining photons, and then to the intensity falling exponentially rather than linearly. That leads to the transmitted intensity I = I₀e^(−μx). From this equation three branches emerge: a larger μ or a thicker absorber gives a smaller I; ln I = ln I₀ − μx means a graph of ln I against x is a straight line with gradient −μ; and the half-value thickness is x½ = ln 2 / μ.
    • 1Box 1

    • 2Box 2

    • 3Box 3

    0 of 3 labelled

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