MRI Flashcards
Describe the magnetic moment of atoms
A proton can be considered as a sphere of +ve charge, that is spinning on its axis
Moving electric charge creates a magnetic moment µ
The direction of µ is given by the right hand grip rule
Hydrogen has the highest magnetic moment
Why are hydrogen atoms the best for MRI?
Hydrogen has the highest magnetic moment, hence provide a strong MRI signal. ( 1H1 contains only one
proton and there is no neutron to cancel or mask the proton spin value )
Hydrogen is the most abundant atom in the body
Which atoms have net spin?
Nuclei are made of protons and neutrons
Both have spin (1/2)
Pairs of spins tend to cancel
So only atoms with an odd number of protons or neutrons have a net spin
Good MRI nuclei are 1H, 13C, 19F, 23Na, 31P
What happens when an external magnetic field is applied?
In an external magnetic field B0 ( >1 Tesla), protons will either line up its µ parallel or antiparallel to an external
magnetic field – no other orientation is possible
The parallel state (blue sphere) has a lower energy (ground state) than antiparallel (orange) (excited state)
This splitting in the spin energy level of a nucleus when placed in an external B field is known as Zeeman effect
The energy difference between parallel and antiparallel state is Eflip
The energy difference Eflip is proportional to the strength of external magnetic field B0
What is Eflip?
The energy difference between parallel and antiparallel state is Eflip
The energy difference Eflip is proportional to the strength of external magnetic field B
Eflip = Eantiparallel- Eparallel
Describe the excess of protons in one state in comparison to the other
At room temperature, the number of protons in the lower state ≠ protons in higher state
Slightly more than half of the protons are in lower energy state (i.e. aligned with B0
)
For a 1 Tesla field, the relative excess is ~3 per million
In a typical voxel in MRI, there are about 1021 protons and hence the excess protons in the lower energy state ~1015
Hence, there is a net magnetisation (Mz) in the direction of external magnetic field
Larger the Magnetic field B0 the …..
- Larger the difference in energy levels
* Larger the excess number aligned with field , i.e stronger Mz
What happens when a RF frequency is applied?
If we deliver a photon of energy (hf = Eflip ), protons in the lower energy state may move to higher energy state
What is precessional motion?
When placed in an external magnetic field, the proton also precess around the external magnetic field
This precessional motion is due to the torque acting on proton due to external magnetic field
This behaviour is similar to a spinning top, which wobbles due to force of gravity
What is the Larmor frequency?
The frequency of precessional motion is given by Larmor relationship
Larmor frequency; f = (γ/2π) B0
γ/2 π is known as gyromagnetic ratio, which is unique to each element
Gyromagnetic ratio is expressed in MHz/T
For hydrogen protons, the precessional frequency is 42.6MHz/T
i.e. at 1T the protons precess at around 42 million times per second
Irradiating the sample with an RF pulse of Larmor frequency will promotes
protons from lower energy state to higher energy state
Calculate the frequency of precession of 1H at 0.5, 1.5 and 3.0 Tesla?
frequency of precession @ 0.5 T = 42.58 x 0.5 = 21.29 MHz
frequency of precession @ 1.5 T = 42.58 x 1.5 = 63.87 MHz
frequency of precession @ 3 T = 42.58 x 3.0 = 127.MHz
What is the gyromagnetic ratio?
γ/2 π is known as gyromagnetic ratio, which is unique to each element
Gyromagnetic ratio is expressed in MHz/T
For hydrogen protons, the precessional frequency is 42.6MHz/T
i.e. at 1T the protons precess at around 42 million times per second
What is T2 relaxation?
Decay of transverse magnetization
With the 900 RF pulse, a maximum net magnetization Mxy is generated in the transverse direction
The transverse magnetic field Mxy induces a signal in the receiver coil (due to Faraday’s induction)
This damped sinusoidal signal is known as Free Induction Decay (FID)
After the RF signal applied, Mxy decays due to loss of coherence
Loss of phase coherence is due to intrinsic micrcomagnetic inhomogeneities in the sample
Due to the loss of phase coherence, the transverse magnetization Mxy decays
T2 relaxation time is the time for the transverse magnetization to reduce to 37% of its initial value
T2 relaxation is also known as spin-spin relaxation
What is T2* decay
Extrinsic magnetic inhomogeneities (imperfect main magnetic field, presence of magnetic material
as contrast agents) add to the loss of phase coherence from intrinsic inhomogeneities and further
reduces the decay constant known as T2* decay
What is spin-spin relaxation?
T2 relaxation
Why T2 relaxation time is different for different tissues?
T2 relaxation is due to the loss of phase coherence as a result of intrinsic micro magnetic inhomogeneities,
whereby individual protons precess at different frequencies arising from the slight changes in local magnetic field
strength
T2 values depend on the molecular structure of the sample
Amorphous structures (CSF, edemous tissue, water) contain mobile molecules with fast and rapid motion. These
tissues do not support intrinsic magnetic field inhomogeneity, hence exhibit long T2
Large macromolecules(bone) are non-moving and have large intrinsic field, hence very short T2
T2 relaxation time doesn’t depend on field strength (very small dependence)
What is T1 relaxation?
growth of longitudinal magnetization
Longitudinal magnetization Mz begins to recover simultaneously with transverse(Mxy) decay
T1 relaxation time is the time needed for the recovery of 63% of Mz after 900 pulse
T1 is also known as Spin-lattice relaxation time
T1 value is affected by external magnetic field - higher B0 higher T1
What is spin lattic relaxation time?
T1 relaxation time
Why T1 relaxation time is different for different tissues?
T1 relaxation time depends on the rate of energy dissipation into the surrounding molecular lattice
Molecules are tumbling through space with certain frequencies
Energy transfer is most efficient, when this tumbling frequencies(vibrational frequencies) are comparable to
Larmour frequency
Small molecule (water, CSF) have a broad distribution of motional frequencies with poor matching with Larmour
frequencies, hence shows long T1 values
Medium sized molecules (proteins, fatty tissues) have a narrow distribution of tumbling frequencies and good
matching with Larmour frequencies. Hence short T1 values
Large sized molecules tumble too slowly and almost no matching with Larmour frequency, hence very long T1
A- Large stationary molecules Longest T1
C- Small aqueous molecules (water, CSF ) Long T1
B- Medium Viscous molecules(proteins, fatty tissues) Short T1