Eduqas A-Level Physics A420QS
Basic Physics
Kinematics
Dynamics
Energy Concepts
Circular Motion
Vibrations
Kinetic Theory
Thermal Physics
Conduction of Electricity
Resistance
D.C. Circuits
Capacitance
Solids Under Stress
Electrostatic and Gravitational Fields of Force
Using Radiation to Investigate Stars
Orbits and the Wider Universe
The Nature of Waves
Wave Properties
Refraction of Light
Photons
Lasers
Nuclear Decay
Particles and Nuclear Structure
Nuclear Energy
Magnetic Fields
Electromagnetic Induction
Option A: Alternating CurrentsOption A
Option B: Medical PhysicsOption B
Option C: The Physics of SportsOption C
Option D: Energy and the EnvironmentOption D
Mathematical Requirements (Appendix C)
Option B: Medical Physics
Attenuation of X-rays and half-value thickness
- 3 things to know
- Component 3
Overview
Half-value thickness of a material for X-rays and plotted to turn attenuation data into a straight line.
What you need to know
Answer each one before you reveal it.
What fraction of an X-ray beam remains after passing through three half-value thicknesses?
Why does the linear attenuation coefficient of a material depend on the photon energy of the beam?
Questions from this subtopic
Each one with the model answer underneath.
- 1
State the attenuation equation for a parallel beam of X-rays passing through matter.
Model answer
The transmitted intensity is I = I₀e^(−μx), where I₀ is the incident intensity in W m⁻², μ is the linear attenuation coefficient in m⁻¹ and x is the thickness in m.
- 2
What does the linear attenuation coefficient of a material represent?
Model answer
It is the fraction of the beam intensity removed per unit thickness of the material. Its unit is m⁻¹, or mm⁻¹ where thicknesses are quoted in millimetres.
- 3
Define the half-value thickness of a material for X-rays.
Model answer
The half-value thickness is the thickness that reduces the transmitted intensity of a beam to one half of its incident value. It is measured in metres or millimetres.
- 4
Derive the relationship between the half-value thickness and the linear attenuation coefficient.
Model answer
Setting I = I₀/2 in I = I₀e^(−μx) gives e^(−μx½) = 0.5, so μx½ = ln 2. The half-value thickness is therefore x½ = ln 2/μ = 0.693/μ.
- 5
A tissue has a linear attenuation coefficient of 0.25 mm⁻¹ at a given photon energy. Calculate its half-value thickness.
Model answer
x½ = 0.693/0.25 = 2.8 mm. Working back, e^(−0.25 × 2.77) = e^(−0.693) = 0.500, exactly one half of the incident intensity.
- 6
A beam passes through 3.0 mm of a material with μ = 0.20 mm⁻¹. Calculate the fraction of the intensity transmitted.
Model answer
I/I₀ = e^(−0.20 × 3.0) = e^(−0.60) = 0.55, so 55% is transmitted. Working back, ln 0.549 = −0.600, which divided by 0.20 mm⁻¹ gives 3.0 mm.
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