In MRI: Is the Larmor frequency represents the rate of proton precession?
(TRUE) It describes the ‘spinning top’ motion of protons in a magnetic field.
In MRI: Is the Larmor frequency proportional to the field strength B0?
(TRUE) Frequency increases linearly with magnetic field strength (f = γB0).
In MRI: Does T1 relaxation time determine the Larmor frequency?
(FALSE) Larmor frequency is a function of the field and the nucleus; T1 is a measure of tissue recovery time.
In MRI: Is frequency inversely proportional to the gyromagnetic ratio?
(FALSE) It is directly proportional; different nuclei precess at different speeds in the same field.
In MRI: Does the Larmor frequency drop as the signal decays?
(FALSE) The signal strength (amplitude) decays, but the frequency of precession stays the same.
In MR imaging: Does the bulk magnetisation vector (Mo) represent a single proton?
(FALSE) Mo is the ‘Net Magnetisation Vector,’ which is the mathematical sum of millions of individual proton magnetic moments. Individual protons precess at an angle, but their net effect points along the Bo axis.
In MR imaging: Is the magnitude of Mo independent of the strength of Bo?
(FALSE) Mo is directly proportional to Bo. A stronger magnetic field aligns a higher percentage of protons in the ‘parallel’ state, creating a larger net magnetisation and higher Signal-to-Noise Ratio (SNR).
In MR imaging: Are the longitudinal and transverse magnetisation vectors equal in size after a 90 degree RF pulse?
(FALSE) A 90° pulse tips the entire longitudinal vector (Mz) into the transverse plane (Mxy). Immediately after the pulse, longitudinal magnetisation is ZERO and transverse magnetisation is at its MAXIMUM (Mo).
In MR imaging: Is the nuclear spin population inverted after a 180 degree RF pulse?
(TRUE) This is an ‘inversion pulse.’ It flips the net magnetisation vector 180 degrees, putting the majority of protons into the higher-energy ‘anti-parallel’ state (pointing against Bo).
In MR imaging: Does the rotation of the magnetisation vector in the x-y plane give rise to the MR signal?
(TRUE) Only precessing transverse magnetisation induces a current in the receiver coil (Faraday’s Law). Magnetisation along the longitudinal (z) axis does not rotate around the coil and cannot produce a signal.
During the spin echo pulse sequence: After the 90 degree RF pulse, magnetic field inhomogeneities cause the protons to lose phase coherence.
(TRUE) This is the cause of T2* decay. Because the magnetic field isn’t perfectly uniform, some protons precess slightly faster and some slower, causing them to ‘fan out’ and lose signal.
During the spin echo pulse sequence: The 180 degree RF pulse rephases the spins.
(TRUE) The 180° pulse acts like a ‘pancake flip.’ It reverses the positions of the fast and slow protons so that the fast ones are now behind the slow ones; they eventually catch up, creating a rephased ‘echo’.
During the spin echo pulse sequence: The spin echo signal appears at a time TE after the 180 degree pulse.
(FALSE) The echo appears at time TE (Echo Time). However, the 180° pulse is delivered at TE/2. Therefore, the echo appears at a time TE/2 after the 180° pulse, not a full TE after it.
During the spin echo pulse sequence: It can be used to generate either T1 or T2 weighted images.
(TRUE) By adjusting the TR (Repetition Time) and TE (Echo Time), you can emphasize different tissue properties. Short TR/Short TE = T1; Long TR/Long TE = T2.
During the spin echo pulse sequence: Multiple sequential 180 degree pulses can be applied after the 90 degree pulse to improve contrast in T1-weighted images.
(FALSE) Multiple 180° pulses are used in ‘Turbo’ or ‘Fast’ Spin Echo to create a train of echoes for T2 weighting (improving speed). They do not improve T1 contrast; T1 contrast is primarily controlled by the TR.
Gradient recalled echo pulse sequences: Frequently use flip angles < 90 degrees.
(TRUE) GRE sequences often use small flip angles (Alpha angles) to allow for faster imaging. Since not all longitudinal magnetization is tipped, recovery is faster, allowing for a very short TR.
Gradient recalled echo pulse sequences: Apply a 180 degree RF pulse to generate the MR signal.
(FALSE) GRE sequences do NOT use a 180° refocusing pulse. Instead, they use a gradient magnetic field reversal to rephase the spins and create the echo.
Gradient recalled echo pulse sequences: Can be used to generate T2-weighted images.
(FALSE) Because there is no 180° refocusing pulse, GRE sequences cannot compensate for field inhomogeneities. Therefore, they produce T2* (T2-star) weighted images, not pure T2.
Gradient recalled echo pulse sequences: Are often used for MR angiography.
(TRUE) GRE is excellent for MRA because it is very sensitive to flow. Moving blood enters the slice with ‘fresh’ spins that haven’t been saturated, making the vessels appear very bright (Inflow effect/TOF).
Gradient recalled echo pulse sequences: Are affected by main field inhomogeneities.
(TRUE) This is the defining characteristic of GRE. Without the 180° pulse to ‘cancel out’ fixed magnetic field errors, the signal decays quickly according to T2*.
In MR imaging: The frequency of electromagnetic radiation needed to excite nuclei is independent of the static magnetic field strength.
(FALSE) The resonance frequency (Larmor frequency)** is directly proportional to the magnetic field strength** (f = γB0). A 3T scanner requires double the frequency of a 1.5T scanner for excitation.
In MR imaging: The direction of the static magnetic field must be parallel to the long axis of the body.
(FALSE) While this is true for traditional closed-bore (superconducting) magnets, open MRI systems often use a vertical magnetic field that is perpendicular to the long axis of the body.
In MR imaging: A magnetic field gradient is used to define the slice to be imaged.
(TRUE) The slice-select gradient creates a linear variation in the magnetic field. Only the thin ‘slice’ where the Larmor frequency matches the RF pulse frequency will be excited.
In MR imaging: Gadolinium-based contrast agents shorten both T1 and T2 of tissues.
(TRUE) Gadolinium is paramagnetic and provides an additional pathway for protons to lose energy and dephase. However, at clinical doses, the T1-shortening effect is more dominant, making tissues appear bright on T1-weighted images.