Module 6 §5: Medical Imaging · Year 2
Radioactive Tracers and PET
Revision notes on Radioactive Tracers and PET for the OCR A-level Physics specification (H556). Free to read, with 4 practice questions in the app.
Module 6 §5: Medical Imaging · Year 2
Revision notes on Radioactive Tracers and PET for the OCR A-level Physics specification (H556). Free to read, with 4 practice questions in the app.
X-rays show structure. Nuclear medicine shows function — which tissue is active, not merely where it is. That is the distinction the whole topic turns on.
A tracer is a radioactive isotope attached to a molecule the body uses, introduced into the patient and tracked from outside by the radiation it emits.
What makes a good tracer
A gamma emitter, since only gamma escapes the body to reach the detector. Alpha and beta would deposit their energy in tissue and cause harm without producing an image.
A short half-life, long enough to complete the scan but short enough to limit dose — typically hours.
Chemically suitable, so the body carries it to the organ under investigation.
Technetium-99m meets all three: a pure gamma emitter with a six-hour half-life, and it can be attached to a wide range of molecules. It is far and away the most-used medical isotope.
The gamma camera — a lead collimator admits only gamma photons travelling perpendicular to it, so each detector position corresponds to one point in the patient. Behind it, a scintillator converts each photon into a flash of light, and photomultiplier tubes convert the flash into an electrical pulse. A computer assembles the pulses into an image.
The collimator is why the image is spatially meaningful — without it, a photon arriving at a detector could have come from anywhere, and the picture would be a uniform blur.
PET — positron emission tomography
A positron-emitting tracer is used, most often fluorine-18 attached to glucose.
Each emitted positron travels a very short distance before meeting an electron, and the two annihilate.
The annihilation produces two gamma photons of 0.511 MeV travelling in exactly opposite directions, as momentum conservation requires.
A ring of detectors registers both arrivals. The tiny difference in arrival times locates the annihilation along the line between the two detectors.
Example: attaching the tracer to glucose is what makes PET so useful. Tissue that consumes glucose rapidly lights up, so active brain regions and fast-growing tumours both stand out. The image shows metabolism itself — biochemistry made visible from outside the body.
Why 0.511 MeV — it is the rest energy of an electron, from E = mc². The two annihilating particles have equal mass, and their energy is shared equally between the two photons.
Multiple choice and calculations for this topic are in the app, one question at a time. Written answers are marked against the specification and you get the mark scheme with the feedback.
Practise Radioactive Tracers and PET