ABMP MRI Physics flashcards
ABMP MRI Physics · Build recall with a focused review session.
32 cards. Read the term and the definition here. The deck at the top of this page is optional.
- Larmor equation
- The precession frequency of a spin is f0 = (γ/2π)B0. For hydrogen-1 at 1.5 T, f0 is approximately 63.9 MHz; at 3 T, approximately 127.7 MHz.
- Gyromagnetic ratio
- The constant γ relating magnetic moment to angular momentum and Larmor frequency to field. For 1H, γ/2π is about 42.58 MHz/T, determining resonance frequency at a given B0.
- Net magnetization M0
- The equilibrium vector sum of nuclear magnetic moments aligned with B0. It arises from a small Boltzmann population excess and is proportional to proton density and B0.
- Bloch equation
- An equation of motion describing precession and relaxation of macroscopic magnetization: dM/dt = γM × B − (Mx i + My j)/T2 − (Mz − M0)k/T1.
- Flip angle
- The angle by which an RF pulse rotates magnetization, given by θ = ∫γB1(t)dt. A 90° pulse places M0 into the transverse plane; a 180° pulse inverts Mz.
- T1 relaxation
- Longitudinal (spin-lattice) recovery of Mz toward equilibrium, described by Mz(t) = M0(1 − e^(−t/T1)). T1 is always longer than or equal to T2 in tissue.
- T2 relaxation
- Transverse (spin-spin) decay of Mxy described by Mxy(t) = Mxy(0)e^(−t/T2). It reflects irreversible dephasing from microscopic field fluctuations.
- T2 star
- Effective transverse decay including reversible dephasing from static field inhomogeneity, with 1/T2* = 1/T2 + 1/T2′. It is always shorter than true T2.
- Spin-echo signal equation
- Signal is proportional to ρ(1 − e^(−TR/T1))e^(−TE/T2). Long TR with short TE gives proton-density weighting; long TR with long TE gives T2 weighting.
- Inversion time null point
- In inversion recovery, Mz(t) = M0(1 − 2e^(−TI/T1)); a tissue is nulled when TI = T1·ln2. STIR nulls fat and FLAIR nulls CSF using this relation.
- Ernst angle
- The gradient-echo flip angle that maximizes signal for a given TR and T1: α = arccos(e^(−TR/T1)). It balances signal against saturation at short TR.
- Slice thickness formula
- Slice thickness equals RF bandwidth divided by the product of γ and slice-select gradient: Δz = Δf/(γGss). Thinner slices require a larger gradient or narrower RF bandwidth.
- Phase encoding
- A brief gradient applied before readout whose area sets the ky location in k-space. The number of phase-encoding steps determines the image matrix size in that direction.
- Frequency encoding
- A readout gradient applied during signal acquisition that maps spatial position linearly to Larmor frequency, allowing position along that axis to be decoded by Fourier transform.
- k-space FOV relation
- Field of view equals 1/Δk, where Δk is the k-space sampling interval. Spatial resolution equals 1/(k_max), the highest sampled spatial frequency.
- Slice profile
- The through-plane excitation profile, equal to the Fourier transform of the RF pulse envelope. A sinc-shaped RF pulse produces a roughly rectangular slice profile.
- Quadrature coil advantage
- A quadrature (circularly polarized) coil detects two orthogonal signal components, improving SNR by a factor of about √2 relative to a linear coil and reducing transmit power needs.
- Surface coil behavior
- A small coil placed near tissue provides high SNR close to the coil but nonuniform sensitivity and limited field of view, because sensitivity falls with distance from the coil plane.
- Receive bandwidth effect
- Wider receive bandwidth admits more noise, lowering SNR, but reduces chemical-shift artifact. Narrower bandwidth improves SNR but increases shift and susceptibility-related artifacts.
- Specific absorption rate
- RF power deposited per unit mass, expressed in W/kg. It scales approximately with B0 squared, flip angle squared, and sequence duty cycle, and is subject to regulatory limits.
- Aliasing artifact
- Wraparound of signal from outside the field of view into the image, occurring when the object exceeds the FOV. Larger FOV, oversampling, or saturation bands prevent it.
- Gibbs artifact
- Truncation ringing near sharp edges caused by finite k-space sampling. It appears as oscillating bands parallel to high-contrast boundaries and is reduced, not resolved, by zero-filling.
- Motion ghosting
- Replicated or smeared signal along the phase-encode direction caused by inconsistent motion between phase-encode lines. Swapping phase and frequency directions moves the artifact.
- Chemical shift artifact
- Spatial displacement of fat relative to water along the frequency-encode direction due to their ~3.5 ppm resonance difference. It increases with field strength and decreases with wider bandwidth.
- Echo-planar imaging
- A fast technique filling k-space after a single excitation using rapid gradient switching. It is prone to geometric distortion and T2* blurring, especially near susceptibility boundaries.
- Parallel imaging SNR
- Coil-sensitivity encoding skips phase-encode lines, reducing scan time. SNR decreases roughly with the square root of the acceleration factor, and unfolding artifacts can occur.
- Balanced SSFP
- A steady-state sequence with fully balanced gradients giving high SNR and T2/T1-weighted contrast. It is sensitive to off-resonance, producing dark banding artifacts.
- Compressed sensing
- A reconstruction approach exploiting image sparsity and incoherent undersampling to recover images from fewer samples than Nyquist requires, enabling faster acquisitions.
- Daily QA phantom checks
- Routine quality assurance measures SNR, geometric accuracy, slice thickness, and image uniformity using a phantom, comparing results against established baseline values.
- Coil element failure sign
- A failed or detuned array element produces regional signal dropout or nonuniformity in the image. Comparing individual element images localizes the faulty coil component.
- Apparent diffusion coefficient
- A quantitative measure of water mobility derived from diffusion-weighted images. Signal follows S = S0·e^(−b·ADC); highly cellular tissue restricts diffusion and lowers ADC.
- Quantitative susceptibility mapping
- A method estimating tissue magnetic susceptibility from gradient-echo phase data after removing background fields and performing dipole inversion, useful for iron and hemorrhage.