MRI Notes
Magnetism in MRI
Magneton
The apparatus used in MRI.
Magnets and Magnetic Fields
- A magnet attracts metallic objects.
- A magnetic field influences its environment by orienting it.
Magnetic Materials
- Magnets attract iron; this is called ferromagnetism.
- Ferromagnetism exists in iron, cobalt, manganese, gadolinium, and dysprosium, as well as certain alloys.
Magnetic Poles
- Magnets have a North (N) and South (S) pole.
- Like poles repel, opposite poles attract.
Magnetic Fields Defined
- A magnet influences its surroundings, represented by a vector field called the magnetic field.
Magnetic Spectra Visualization
- Iron filings are used to visualize magnetic spectra.
- The filings align with the magnetic field, forming lines of force.
Magnetic Field and Electric Current
- Electric current in a wire creates a magnetic field (Oersted's experiment, 1820).
- A moving magnetic field generates electric current (Faraday's experiment, 1831).
Magnetic Field of a Straight Conductor
- No N or S poles.
- The magnetic field direction depends on the current direction.
- Field intensity increases with current and decreases with distance from the conductor.
- Magnetic field lines are concentric circles around the conductor.
Earth's Magnetic Field
- The Earth has a magnetic field used for navigation.
- The magnetic south pole is near the geographic north pole, and vice versa.
Magnetic Field of a U-shaped Magnet
- The magnetic field (B) is uniform between the branches of the magnet.
Magnetic Field of a Straight Magnet
- Field lines exit the N pole and enter the S pole.
Magnetic Field Lines
- Magnetic field lines indicate the direction and magnitude of the magnetic vector B.
- Denser lines indicate a stronger field.
Broken Magnet Experiment
- Breaking a magnet results in two magnets, each with N and S poles.
- Magnetic poles cannot be isolated.
- Ferromagnetic materials are made of microscopic magnets that are randomly organized when not magnetized.
- In a magnetic field, these elementary magnets align.
Nuclear Magnetic Resonance
Spin
- Atoms consist of a nucleus and electrons; the nucleus contains nucleons (protons and neutrons).
- Protons are positively charged, and nuclei spin, possessing a spin or angular momentum S.
Gyromagnetic ratio
- µ = γS where γ is the gyromagnetic ratio.
Nucleons
- Protons and neutrons pair up, canceling magnetic moments.
- Atoms with an odd number of nucleons have a net magnetic moment.
- Key nuclei for MRI: hydrogen ^{1}H, carbon ^{13}C, fluorine ^{19}F, phosphorus ^{31}P, sodium ^{23}Na.
Hydrogen in MRI
- Hydrogen is abundant in soft tissues (70-90% water).
- Its nucleus (a single proton) has a magnetic spin moment.
- Most MRI uses hydrogen nuclei.
- Gyromagnetic ratios (MHz/tesla): H=42.58, F=40, Na=11.2, C13=10.7, N=3
Magnetic Moments
- Normally, hydrogen nuclei's magnetic moments are randomly oriented, so net magnetization is zero (\Sigmaµ = 0).
Absence of External Magnetic Field
- Protons orient randomly; the microscopic magnetization vectors sum to zero (\Sigma m = 0).
- No macroscopic magnetization vector M exists.
Presence of External Field
- Protons align with the external field (Oz), resulting in a macroscopic magnetization vector Mzo.
Larmor Frequency
- In an external magnetic field, protons precess at an angular frequency \omega0 = γ B0 (rad/s).
- B_0 = magnetic field (tesla).
- γ = gyromagnetic ratio.
- Larmor frequency: ν0 = γ B0 / 2π (Hertz).
Energy Levels
- Protons align either parallel or anti-parallel to B_0.
- Parallel alignment is slightly more common and has lower energy (E1); anti-parallel is higher energy (E2).
Macroscopic Magnetization
- The few extra parallel protons create a net macroscopic magnetic moment along B_0, called Mz0.
- This overall magnetic moment Mz0 is weak and requires dynamic physical methods (RF transfer) to detect.
RF Pulses
- RF pulses cause Mz0 to tilt towards the xOy plane, decreasing longitudinal magnetization (Mz) and creating transverse magnetization (Mxy).
Resonance
- Applying a radiofrequency wave perpendicular to B0 modifies the precession angle: \omega = γB0.
- Equilibrium State: M aligns with Oz, M = Mzo, Mxy = 0
- 90° RF Pulse: Mz decreases, Mxy increases, achieving Mz = 0 and Mxy = maximum.
Magnet Components
- The MRI machine includes shim coils, cryostat, superconducting coil, head antenna, magnet, gradient coils, and body antenna.
Magnet Characteristics
- Magnetic field intensity:
- Low fields (<0.25 T)
- Medium fields (<1 T)
- High fields (>1 T, 1.5, 3T)
- Earth's magnetic field = 0.5 x 10^{-4} Tesla
- Homogeneity
Magnet Types
- Permanent magnets: no electricity or cooling; heavy, inhomogeneous fields.
- Resistive magnets: electromagnets with high heat dissipation and electricity consumption, require cooling.
- Superconducting magnets
Superconducting Magnets
- Electromagnets using superconducting metal
- Generate intense, uniform B_0 fields.
- Lower electricity consumption.
- Cooled by Helium (cryostat).
Constant Magnetic Field
- The magnetic field B_0 is constant and always present.
- MRI rooms include a Faraday cage.
Gradient Coils
- Electromagnetic coils introduce gradients in B_0.
- Characterized by amplitude (mT/m), rise time (µsec), and slew rate.
RF Antennas
- Transmit and receive RF signals.
- Types: cylindrical (deep exploration), surface (superficial exploration).
- Can be used alone or in phased arrays.
- Phased arrays offer small fields with good signal-to-noise ratio (S/B) and larger coverage.
Antenna Use
- The magnet can serve as a "body antenna."
- Dedicated antennas improve the signal-to-noise ratio and spatial resolution.
- Choice depends on the region to be explored.
Antenna Positioning
- Center the region of interest in the antenna and at the magnet's center.
MRI Other Components
- Examination table, computer system, acquisition and image processing consoles, archiving, and Faraday cage.
Faraday Cage
- Surrounds the room.
- Reduces magnetic fields and isolates from external RF interference.
RF Pulses and Magnetization
- 180° RF Pulse: Mz decreases and inverts, resulting in M = -Mzo.
RF Pulse Values
- 90° Pulse: tips M into the OXY plane, maximizing Mxy while Mz is zero (saturated system).
- 180° Pulse: inverts M to the opposite of B_0, inverting Mz while Mxy is zero (inverted system).
Summary of MRI Principles
- Larmor frequency: \omega0 = γ B0.
- Electromagnetic wave: rotating magnetic field B_1.
- Equilibrium: excess protons create a magnetization vector M, aligned with B_0.
- B_1 perturbs equilibrium, tilting M into the xOy plane (90° pulse) => M = Mxy.
- Two mechanisms: equalization of protons across two energy levels and phase alignment of protons.
- 180° RF pulse inverts protons across energy levels > M.
Relaxation
- Upon stopping the RF wave, a signal is collected as an RF wave.
- This free induction decay (FID) signal is characterized by its initial intensity (RHO) and decay, depending mainly on T2* and T2.
Relaxation - Return to Equilibrium
- After excitation, the system returns to equilibrium.
- Longitudinal magnetization recovers; transverse magnetization disappears.
- Transverse and longitudinal relaxations have different mechanisms.
Tissue Magnetization
- Two types of tissue magnetization: longitudinal (Mz, parallel to B0, related to T1) and transverse (Mxy, perpendicular to B0, related to T2).
Longitudinal Relaxation (T1)
- Spins return to the parallel state.
- Longitudinal magnetization regrows.
- T1 is the time to recover approximately 63% of longitudinal magnetization.
Transverse Relaxation (T2)
- Spins dephase.
- Transverse component disappears.
- T2 is the time for approximately 63% of transverse magnetization to disappear.
Relaxation Times
- Depend on the tissue structure and are the primary factor for contrast.
- T1 = longitudinal relaxation time.
- T2 = transverse relaxation time.
T1 and T2 Contrasts
- Tissues have different T1 values, even with the same proton density, resulting in varying signal intensities.
- T1 short = fast regrowth (e.g., fat).
- T1 long = slow regrowth (e.g., liquids).
- T1 relaxation time increases with increasing B_0.
T2 Characteristics
- T2 = time for MT to lose 63% of its value.
- Depends on proton dephasing.
- T2 short = rapid decay (liquids).
- T2 long = slow decay (fat).
- T2 relaxation time is linked to molecular heterogeneities.
Relaxation Summary
- Longitudinal relaxation (T1) = regrowth of Mz.
- Transverse relaxation (T2) = loss of phase coherence of protons.
- T1 and T2 are distinct with different durations.
- T2 is much faster than T1.
Signal Measurement
- Antennas convert tissue magnetization into an electrical signal.
- Free induction decay (FID) reflects tissue properties.
Free Induction Decay (FID)
- Depends on the nucleus's resonance frequency.
- Amplitude is determined by the RF wave intensity, B_0 intensity, number of protons, and the physicochemical environment.
Tissue contrast dependence
- Proton density.
- T1 relaxation time.
- T2 relaxation time.
- Flow.
Proton Density Contrast
- Tissues without protons (calcification, air) produce no signal.
Programming
- MRI machines are programmed to emphasize contrast elements.
- Sequences are programmed to favor a particular contrast (T1, T2, proton density, or flow).
Image Acquisition
- Images are derived from multiple sequences.
- The time between sequence repetitions is the repetition time (TR), a key parameter to set.
Spin Echo Sequence
- Employs a 90° pulse followed by a 180° pulse to create an echo.
- TR = time between two 90° pulses.
- TE = echo time = time between the 90° pulse and signal reception.
TR Influence
- TR influences T1 contrast.
- If TR is long compared to tissue T1, longitudinal magnetization fully recovers.
- If TR is short, longitudinal magnetization is less than maximal.
TE Influence
- TE influences T2 contrast.
- If TE is short, T2 decay differences are minimized.
- If TE is long, differences in T2 are highlighted.
Long Sequences
- Long TE (40-100ms) and TR (1000-3000 ms)
- Ponderation in T2
- TR long (>2000msec)
- TE long
Short Sequences
- Short TE (<30 ms) and TR (<600msec)
- Ponderation in T1
- TR short.
- TE short.
Mixed Sequences
- Less common.
- TE long, TR short.
- TE short, TR long: Ponderation in proton density.
Inversion Recovery Sequence
- Improves T1 contrast.
Spatial Encoding
Spatial Localization of Signal
- Without spatial discrimination, signals from the sample are irresolvable.
Magnetic Gradient Creation
- By = B0 + g_y * y
Selective Excitation
- Selective excitation of a plane can be done if the radiofrequency is the resonance frequency of protons in that plan.
Gradient Determinations
- Gradients determine the orientation of the slice.
- The central frequency of the RF pulse sets the slice level.
- The RF pulse bandwidth controls slice thickness.
Slice Selection
- A gradient (Gz) defines the slice.
Fourier Transform
- Mathematical calculation to classify frequencies and transform them into RMN signals.
- Allows transformation into a gray scale image.
Image Acquisition Time
- One cycle provides information for one line.
- The phase gradient is shifted to acquire subsequent lines.
- TA = TR x N x n; N = number of lines, n = number of accumulations.
Reducing Acquisition Time
- Use asymmetric matrices.
- Reduce TR.
- Reduce flip angle.
Asymmetric Matrix
- Only the number of lines affects acquisition time.
Gradient Echo Sequence
- Signal echo achieved by applying a reading gradient Gx.
- Reduces acquisition time.
Contrast with Gradient Echo
- If angle > 60°, equivalent to SE; TR and TE determine T1 or T2 contrast.
- If angle < 30°:
- TE > 30 ms: T2* images.
- TE short and TR > 100 ms: DP.
Image Quality Trade-offs
- Signal-to-noise ratio (S/B), acquisition time, spatial resolution, number of slices, and weighting.
Contrast Modification
- Fat suppression sequences (IR, STIR) and fat saturation.
- Contrast agents.
Gadolinium Chelates
- Decrease T1 in tissues.
- Used with T1-weighted sequences after IV administration.
Artifacts
- Motion, susceptibility, aliasing, chemical shift, truncation, partial volume, system defects.
Motion Artifacts - non-periodic
- Caused by patient movements, propageted along the phase and/or the frequency
- Correction: Information, Contention, Sedation
Motion Artifacts - periodic
- Caused by respiratory or cardiovascular movements
- Propageted along the phase, generating ghost images
- Correction: fast imagery, saturation bands, synchronisation
Susceptibility Artifacts
- Metallic objects distort the image due to local B changes.
Aliasing Artifact
- Occurs when the object is larger than the field of view (FOV).
- Correction: increase the FOV.
Chemical Shift Artifact
- Linked to localization errors along the encoding gradient, specifically at fat-water interfaces.
- correction: fat supression.
Truncation Artifact
- Occurs at abrupt signal changes.
- Correction: increase matrix and higher spatial resolution.
Partial Volume Artifact
- Similar to CT artifact = reduce slice thickness.
Magnet Safety
- All materials must be non-magnetic.
- Patients must be screened for contraindications.
Absolute Contraindications
- Certain devices (pacemakers, implanted pumps, neurostimulators) and ferromagnetic foreign bodies.
Relative Contraindications
- Orthopedic prostheses, claustrophobia, involuntary movements, pregnancy (first trimester).
Patient Preparation
- Confirm identity, check for contraindications, explain the exam.
Room Preparation
- Verify emergency equipment.
- Ensuring hygiene
Antenna Preparation
- Select the appropriate antenna and proper connection.
Patient Installation
- Ensure patient comfort and safety.
Console Settings
- Select the appropriate sequence, plane, weighting, matrix, FOV, echo time, slice thickness, and fat suppression.
Image Interpretation
- T1, proton density, and T2 contrasts each provide different information about tissue properties.
- For T1-weighted images, fat appears hyperintense.
- Calcium and air typically appear hypointense on all sequences.
- Water/CSF will appear hypointense on T1, hyperintense on T2, and very hyperintense on FLAIR.