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
Key words
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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.
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