MRI Flashcards
(128 cards)
What sort of nuclei possess spin angular momentum, J
Nuclei with odd number of protons, neutrons or both
Magenetic moment equation,Mu
Mu = (gyrometric ratio)(spin angular momentum)
Precession torque equation
tau = mu x B = (mu)Bsin(theta)
Why does precession occur
nuclear magnetic moment in a magnetic field experiences torque
Larmor equation
Frequency of precession
w= (gyrometric ratio)(Applied magnetic field - B0)
Magnitude of spin angular momentum
|J| = hbar [I(I+1)]^(1/2)
Where I is spin quantum number
How many spin states denototed by spin quantum number
(2I+1)
Potential energy of magnetic moment
work done rotatinf magnetic moment in B-field
E = -(mu).B = -(gyrometeric ratio)(J in Z direction)(B0)
How is spin state distributed in thermal equilibrium
seperated by deltaE according to Boltzman distribution
ndown/ nup = exp(-deltaE/ KbT)
Spin state distribution in the high temperature limit
ndown/ nup = 1-([(hbar)(gyrometric const)(B0)]/KbT)
Why can magnetisation within a material be detected by NMR
Population differences arisen by small excess of spins in the low energy state causes a net bulk magnetaisation in a material - can a;sp be increased by using a static magnetic field to polarise nuclear spins
At what angle fo spins precess to the Z-axis at random phase
54degrees
What is the bulk magnetisation in NMR
M = sum of spin magnetic moments
Safety issues of static field
Projectile effect
Moving in spatial static fields causes the body to experience varying fields causing dizziness, metallic taste and flashing light sensation
What is the Larmor frequency at 1T
42.57MHz
How RF excitation occur in NMR (QM)?
- Applying RF energy spins tips spins and brings into phase Causing MO to be tipped from the longitudinal plant to the transverse plant
What does a 90degree pulse do?
equalizes the population of spin states and brings spins into phase
How RF excitation occur in NMR (CM)?
Apply B field oscillating at frequency ~ Larmor frequency and oriented in Bz direction
What is the purpose of applying a magnetic field oscillating at a frequency in NMR or MRI experiments?
To excite the magnetization in the sample, particularly by aligning with the Larmor frequency.
What is the total B1 field expression, and why is the anticlockwise rotating component neglected?
The total
B1(t) = 2B1cos(wt)i
cos(ωt)i, and the anticlockwise component Ba(t) is neglected due to being off-resonance.
How does the rotating frame of reference simplify the analysis of the B1 field in NMR or MRI experiments?
It allows for the consideration of the B1 field as stationary for the component at
+ω1
+ω1, simplifying the analysis while the component at −ω1rotates at −ω2 and can be ignored due to being off-resonance.
How do you relate the lab frame and kav frame
- z’ = z
- x’ rotating at frequency with respect to x.
- y’ rotating at frequency with respect to y
What is the relationship between the rate of change of a vector in the lab frame and rotating frame?
The relationship is given by
dr/dt =
(w × r) +(∂r/∂t)
How is the magnetization described in the rotating frame?
In the rotating frame, the magnetization is described by
dM/dt = Gyrometeric ratio(M x (B+(w/t))