Magnetic Resonance Imaging Flashcards
MRI principles
- use property of nuclear magnetic resonance NMR to image nuclei of atoms inside the body → magnetic nuclei in a magnetic field absorb & re-emit electromagnetic radiation
MRI application
investigate human body, using non-ionizing radio frequency (RF) waves → waves are generated in the body, need a lot of water
- MRI examines magnetic properties of atomic nuclei
→ atomic nuclei with odd atomic weight possess a spin
→ nucleus with charge & spin produced small magnetic field (behave like a bar magnet)
Precession
= slow movement of the axis of a spinning body around another axis due to a torque acting to change the direction of the first axis
example for precession
hyrogen atom in a magnetic field
- protons not perfectly aligned
- nuclei percess about the direction of the field
- precession frequency = Larmour Frequency
Spin states
- protons align with/against field
- aligned against field → anti-parallel → higher energy state
- transition (parallel → anti-parallel) induced via electromagnetic radiation excitement → RF pulse
Larmour frequency
frequency of percession of magnetic moments
- f = gamma * B0
net magnetization vector
- no RF pulse → parallel state → net magnetization parallel to magnetic field
- RF pulse → protins flip to anti-parallel state
- RF pusle stops → protons flip back to parallel state → M in z-plane
radio frequency pulse
RF pulse at Larmour frequency will cause net magnetisation vector M to rotate about B1 in the rotating frame of reference
Flip angle alpha
flip angle alpha of M determined by
- magnetic field induced by RF pulse (B1)
- duration of applied pulse tp
alpha = 90° → RF pulse rotates M into transverse plane (xy) → induces signal in receiver coil at Larmour frequency (same freqeuncy)
→ magnitude of signal depends on M(x-y)
recovery of Mz
when is B1 released → M rebounds back to its original value
→ described by Free Iduction Decay FID
T1 = time constant; point where 63% of magnetization Mz has recovered from alignment with B0
→ measures how quickly protons realign with main magnetic field
recovery of Mxy (after 90° FR pulse)
difference between T2 and T2* relaxation
T2- relaxation: defined by spin-spin interaction → dephasing of spin → loss of phase coherence
- RF pulse → protons rotate in-phase
- after RF pulse → protons de-phase → Mxy magnetisation decreases → signal decay
T2* relaxation: overall term of observed loss of phase coherence
- combines T2 relaxation & additional de-phasing caused by local variations
- more rapid decay of the signal
T2 & T2* relaxation
= time at which magnetization has decayed to 37% of its initial value immediately after 90° RF pulse
T1 & T2 difference
are tissue dependent
- T1 weighted: more homogenous → overall geometry observable; one tissue type is bright – FAT
- T2 weighted: different types of tissue visible; FAT and WATER are bright
spatial localization of MRI signal
goal: received signal depends on position
solution: creating a gradient in exeternal magnetic field
- e.g. gradient in z-direction: causes resonant frequency to be different at each z location → RF pulse tuned to frequeny → only spins in slice corresponding to that frequency will flip
steps for localization of MRI signal
- slice selection (z-gradient)
- frequency encoding (x-gradient)
- phase encoding (y-gradient)