Introducing MRI: Introduction to Magnetic Susceptibility (14 of 56)
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- Опубликовано: 22 сен 2014
- www.einstein.yu.edu - The fourteenth chapter of Dr. Michael Lipton's MRI course covers Introduction to Magnetic Susceptibility T2' and T2*. Dr. Lipton is associate professor radiology at Albert Einstein College of Medicine and associate director of its Gruss Magnetic Resonance Research Center.
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I'm a bit confused - back at the beginning dr Lipton said the NMV is antiparallel to B0 and defended that position in a comment under part 5 despite some books stating otherwise. But here he's drawn the NMV parallel to B0. Was it done on purpose or is it just a mistake?
I agree even I read NVM as parallel to B0 and here the Professor said in last few lectures that 6 out of 10000 protons are anti parallel to B0.
I think it is a mistake as he has clearly said in the past that the ONLY time NMV is parallel to B0 is in a perfectly homogenous field with nothing else inside it. When you have a patient or some other diamagnetic matter in the field then the lower energy state actually is the ANTI-parallel direction and that's why in a real life clinical situation, the resting state of the NMV is anti-parallel. At least that's my understanding of the content so far
In T2 relaxatiom, how can spins dephase, if they have the same Lamour frequency? In T2 prime they dephase because their frequency is different, as Iunderstand.
The T2 is due to spin-spin interaction which leads to the same effect: spins will have different precession frequencies. In T2* you have both, the magnetic field inhomogeneity + the spin to spin interaction which both cause variations in precession frequency (which then cause the spins dephasing)
In gradient echo image why don’t we use even a shorter TE to get a better contrast
And thank you very much for the great lectures
Helen Q. Watch the contrast video he explained this point very clearly
sweet tota thank you very much
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