Adapted from an amazing book entitled Introduction to Functional Magnetic Resonance Imaging: Principles and Techniques (2nd Ed) by Richard B. Buxton (one of my MRI professors at UCSD!):
T2
- The individual dipoles that sum up to produce the transverse magnetization are not precessing at precisely the same rate
- As a water molecule tumbles due to thermal motions, each H nucleus feels a small, randomly varying magnetic field in addition to B0 due primarily to the other H nucleus in the molecule.
- When the random field adds to B0, the dipole precesses a little faster, and when it subtracts from B0, it precesses a little slower.
- For each nucleus the pattern of random fields is different, so as time goes on the dipoles get progressively more out of phase with one another, and as a result no longer add coherently.
- The net precessing magnetization then decays away exponentially, and the time constant for this decay to 63% of its original value is called T2.
T2*
- The source of this T2* effect is magnetic field inhomogeneity.
- Because the precession frequency of the local transverse magnetization is proportional to the local magnetic field, any field inhomogeneity will lead to a range of precession rates.
- Over time the precessing magnetization vectors will get out of phase with one another so that they no longer add coherently to form the net magnetization.
- As a result, the net signal is reduced because of this destructive interference.
- The T2* effect, is due to static field offsets rather than fluctuating fields (as in T2).
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In my words (hopefully this helps somebody):
While both T2 and T2* decay occur because of inconsistent magnetic fields causing differences in precession rates leading to spins growing out of phase and ending in destructive interference, the difference between T2 and T2* is that in T2 the source of the magnetic field inhomogeneity is the random motion of water molecules moving hydrogen nuclei near each other and in T2* the source is static magnetic field inhomogeneities within the MRI itself in addition to T2 effects. This is why T2* is always shorter than T2. Reasoning that T2 is a theoretical constant and that T2* is an observed measure is not alone sufficient for explaining this difference, however it should be noted that T2* is always faster than T2 decay. Some sources also say that T2 is measured over 5-10 microns and that T2* is measured in the millimeter range, but im not sure if thats useful.
