11 Magnetic Resonance Flashcards
Which nuclei have no nuclear
magnetization?
Nuclei with an even number of protons and an even number of neutrons.
–Even numbers of protons pair up with their magnetization aligned in opposite directions and cancel each other (as do even numbers of neutrons).
Which nuclei have the largest nuclear magnetization?
Hydrogen nuclei.
Why H nuclei the basis of most clinical magnetic resonance (MR) imaging?
The abundance of hydrogen in the body, together with the large nuclear magnetization,
Give me one reason that MR signals are weak?
So few nuclei contribute to the MR signal.
Define the Larmor frequency (fL)?
–The precession frequency (MHz) of nuclei in a magnetic
field (Bo).
–The Larmor frequency is directly proportional to the magnetic field strength.
–Larmor frequency (fL) for protons is 42 MHz at 1 T.
Radiofrequency (RF) electromagnetic fields are generated using what?
volume or surface coil.
Define Resonance?
This occurs when an applied RF field interacts with the net nuclear magnetization.
Define the longitudinal magnetization?
–The component of the net magnetization vector parallel to the main magnetic field.
–By convention, the longitudinal magnetization is taken to point in the z-axis.
–Grows exponentially from the initial value of zero to the equilibrium value of Mz with a time constant T1
Define the transverse magnetization?
–The component perpendicular to the main magnetic field.
–By convention, the transverse magnetization is taken to be in the x-y plane.
Define the free induction decay (FID) signal?
–The detected voltage.
–The FID signal is an oscillating voltage at the Larmor frequency (fL).
–The induced FID is obtained in a receiver coil placed around the sample.
–FID signals are detected, digitized, and used to produce MR images.
T1 relaxation
–At a time equal to T1, 63% of the magnetization has formed.
–Full magnetization is normally taken to occur after a time interval of approximately 4 × T1.
–Longitudinal magnetization decays as Mz× e−t/T1 where t is the elapsed time.
–T1 relaxation is called longitudinal relaxation and spin-lattice relaxation.
T1 and tissue
–T1 is long in liquid materials & in solids (hair).
–T1 is short in medium-viscosity materials and in fat.
–Contrast agents such as gadolinium-DTPA cause T1 to be shortened.
–For tissues, T1 increases with increasing magnetic field strength.
–Doubling the magnetic field strength increases tissue T1 by approximately 2^0.5.
Define repetition time TR?
–Generating a N2 matrix MR image requires the acquisition of N sequential signal acquisitions that are obtained with a repetition time TR.
–Short TR times are less than ∼300 ms at 1.5 T and less than ∼450 ms at 3T.
transverse relaxation(T2 relaxation), also spin-spin relaxation
–After a 90-degree pulse, the magnetization vector rotates at the Larmor frequency in the transverse (x-y).
–The induced FID signal decays as e−t/T2 where t is the time.
–At a time equal to T2, the signal has decayed to 37% of its original value.
–After a time ∼4 T2, the transverse magnetization signal is negligible.
–T2 decreases with increasing viscosity and decreasing molecular mobility.
–Tissue T2 values are approximately independent of magnetic field strength.
TE (time to echo)
–MR signals are most often obtained in the form of echoes from transverse magnetization.
–Short TE values will result in little loss of transverse magnetization (i.e., little T2 decay).
–Short TE values therefore produce no differences (contrast) between tissues that have different T2 values.
–T2-weighted images are obtained with a long TE.
–Long TE values are typically greater than 60 ms.
(T2inhomogeneity)*
–Given by 1/T2∗ = 1/T2 + 1/T2inhomogeneity
–For tissues, T2∗ ≤ T2 ≤ T1.
Magnetic shimming
Used to make small corrective changes to the main field to improve the magnetic field uniformity.
Magnetic shimming with passive techniques
Pieces of iron at specific locations.
Magnetic shimming with active techniques
Electrically energized coils.
Permanent magnets
–Have low operating costs and small fringe fields.
–Limitations: heavy and generate fields only up to ∼0.35 T.
Resistive magnets
–It can generate magnetic fields up to ∼0.5 T.
–Resistive magnets can be turned on and off, but consume a large amount of power and need cooling because of the heat generated.
Superconducting magnets
–Field strengths higher than those of resistive and permanent magnets.
–Use a wire-wrapped cylinder (i.e., a solenoid) to generate the uniform magnetic field.
–Superconducting magnets must be kept very cold using liquid helium (4◦ K) as a refrigerant.
–A perpetually circulating electric current of hundreds of amps creates the magnetic field.
–The magnetic field is always on.
Superconductivity
–It is the ability of certain materials to conduct electrical current without any resistance.