MRI: FOUNDATIONS
9.1 Historical Introduction of MRI
What is MRI? (Essence)
Magnetic Resonance Imaging (MRI) is a medical imaging technique that produces high-quality images of the inside of the human body, especially soft tissues.
MRI is based on Nuclear Magnetic Resonance (NMR)—a spectroscopic method originally used by chemists and physicists to study molecules, not patients.
The word “nuclear” frightened people in the 1970s, so the term was wisely dropped.
MRI sounds safer than NMRI—and medicine is also psychology.
From Chemistry to Medicine (Timeline Logic)
1946 – Felix Bloch & Edward Purcell independently discovered magnetic resonance
→ Nobel Prize in 19521950–1970 – NMR used for chemical and molecular analysis, not imaging
1971 – Raymond Damadian
→ Discovered different relaxation times between normal tissue and tumors
→ This was the medical turning point1973
CT introduced by Hounsfield
→ Proved hospitals would invest in expensive imagingPaul Lauterbur produced the first MR image using gradients
1975 – Richard Ernst
→ Introduced Fourier Transform, phase and frequency encoding
→ This is the foundation of modern MRI1977
Damadian demonstrated early MRI scanning
Peter Mansfield developed Echo-Planar Imaging (EPI)
1980–1986
Body MRI achieved
Scan time reduced from 5 minutes → 5 seconds
1987
Real-time cardiac MRI
Magnetic Resonance Angiography (MRA) without contrast
1992
Functional MRI (fMRI) developed
→ Brain function mapping
2003
Lauterbur & Mansfield awarded Nobel Prize in Medicine
Conclusion: MRI is a young science, but it evolved rapidly and intelligently.
Why MRI? (Compared to X-ray and CT)
X-ray
Excellent spatial resolution
Poor contrast resolution
Best for bone
CT
Better contrast than X-ray
Still limited for soft tissue
MRI (Key Advantage)
Superior soft tissue contrast
Multiplanar imaging (any plane without moving the patient)
No ionizing radiation
Adjustable parameters for specific pathology
Rule to remember:
Bone → X-ray / CT
Soft tissue → MRI
9.2 MRI Hardware (Big Picture)
An MRI scanner is built around one central requirement:
A very strong, extremely uniform magnetic field
Hardware choice depends on:
Purpose
Image quality needed
Cost
Patient comfort
9.3 Magnet Types
Two Ways to Create Bo (Main Magnetic Field)
Permanent Magnets
Electromagnets
Resistive
Superconducting
9.3.1 Permanent Magnets
Made of ferromagnetic material
Field strength: up to 0.4 Tesla
Open design
Advantages:
Comfortable
Less claustrophobia
Disadvantages:
Heavy
Lower field strength → lower image quality
9.3.2 Electromagnets
A. Resistive Magnets
Wire coils with large electric current
Field strength: up to 0.6 Tesla
Advantages:
Cheaper
Open design
Disadvantages:
High power consumption
Heat generation
Cooling required
B. Superconducting Magnets (Most Important)
Made of niobium-titanium / niobium-tin
Cooled with liquid helium
At 4 K (−269°C) → zero resistance
Field strength: up to 12 Tesla
Clinical standard: 1.5 Tesla
Advantages:
High field homogeneity
High image quality
Stable magnetic field
Disadvantages:
Expensive
Bore (tunnel-like) design
Modern trend:
Open design vs High field strength
Engineering is still trying to marry the two.
9.4 Shimming (Field Perfection)
MRI demands a perfectly uniform magnetic field
→ Variations must be within parts per million (ppm)
What is Shimming?
Shimming = fine adjustment of the magnetic field to improve homogeneity.
Two Types
Passive Shimming
Steel pieces added
Mechanical correction
Active Shimming
Electric currents through shim coils
Electrical correction
Both methods add corrective fields to improve Bo uniformity.
9.5 RF Coils (Signal Makers)
RF coils:
Transmit RF pulses
Receive MR signals
They directly affect image quality.
9.5.1 Volume Coils
Large field of view
Homogeneous RF field
Used for:
Whole body
Head
Lower SNR for small regions
9.5.2 Surface Coils
Placed directly over anatomy
High SNR
High resolution
Limited depth penetration
Depth ≈ ½ coil diameter
9.5.3 Quadrature Coils
Two coils at 90°
√2 signal improvement
Circular polarization
Most modern volume coils use this design
9.5.4 Phased Array Coils
Multiple surface coils combined
Large coverage + high SNR
Used in modern MRI
Best for spine, body imaging
9.6 Other Hardware
Faraday Cage
Shields MRI from radiofrequency interference
Prevents artifacts
Protects outside equipment
Without shielding, MRI would be drowned in noise.
9.7 Atomic Structure (Why Hydrogen?)
Atoms
Made of:
Nucleus (protons + neutrons)
Orbiting electrons
Hydrogen
Most abundant in the body
Present in water and fat
Has one proton
Ideal for MRI because:
High abundance
High gyromagnetic ratio
9.8 Magnetization
A spinning charged particle creates a magnetic field
→ Like Earth itself
Hydrogen protons act as tiny bar magnets
When placed in Bo:
Protons align:
Parallel (low energy)
Anti-parallel (high energy)
More choose low energy
→ Net magnetization forms
9.9 Larmor Frequency (Very Important)
Equation
ω0=γB0\omega_0 = \gamma B_0ω0=γB0
ω₀ = Larmor frequency
γ = Gyromagnetic ratio (Hydrogen = 42.57 MHz/T)
B₀ = Magnetic field strength
Example:
1.5T → 63.86 MHz
MRI systems operate exactly at this frequency.
Net Magnetization Vector
Aligned along Z-axis
Called longitudinal magnetization (M₀)
Without excitation, no image is formed.
9.10 In-Phase and De-Phase (Foundation of Signal)
In-phase → spins aligned → strong signal
Out-of-phase → spins misaligned → signal loss
MRI signal lives and dies by phase coherence.
Final Old-Tutor Advice
Don’t memorize MRI.
Understand the logic:
Magnet → Protons → RF → Signal → Image
9.11 RF PULSE — THE MOMENT EVERYTHING CHANGES
Before RF:
Protons precess around B₀
Net magnetization points along Z-axis
No signal. No image.
Now listen carefully.
What is an RF pulse, really?
An RF pulse is:
A small magnetic field
Applied perpendicular to B₀ (X or Y direction)
Oscillating at the Larmor frequency
Only when the RF frequency matches the Larmor frequency do protons respond.
This is resonance.
No match = no effect.
Why oscillating, not static?
A static field would cause chaotic motion
An oscillating field at the exact frequency causes a clean rotation
This clean rotation tips the net magnetization away from Z.
90° RF Pulse
Rotates net magnetization from Z-axis into XY-plane
Produces maximum transverse magnetization
Starts:
T2 decay immediately
T1 recovery immediately
The instant you excite, relaxation begins.
Nature never waits.
9.12 EXCITATION — ENERGY IN
Before acquisition
A short pre-scan determines:
Exact Larmor frequency
System calibration
This is necessary because:
Field strength slightly varies
Precision matters in MRI
What excitation really means
Protons absorb RF energy
They move to a higher energy state
Net magnetization is flipped
Flip Angle (FA):
Controlled by:
RF pulse strength
RF pulse duration
Can be 1° to 180°
Standard teaching example: 90°
Excitation = controlled disturbance
MRI is polite physics, not violence.
Resonance analogy (important)
Like:
Opera singer shattering glass
Only the correct frequency works
Wrong frequency → nothing happens
9.13 RELAXATION — ENERGY OUT
Now we reach the heart of MRI contrast.
Relaxation =
Return to equilibrium
Protons:
Do not like high energy
Always seek lowest energy state
Two independent processes happen simultaneously:
Process | Direction | What it describes |
|---|---|---|
T1 | Z-axis | Energy loss to surroundings |
T2 | XY-plane | Loss of phase coherence |
9.13.1 T1 RELAXATION (SPIN–LATTICE)
What T1 describes
Recovery of longitudinal magnetization (MZ)
Energy transferred to surrounding tissue (lattice)
Immediately after 90° pulse:
MZ = 0
All magnetization in XY-plane
With time:
MZ recovers
System returns to equilibrium
T1 definition
T1 = time for MZ to recover to 63% of its original value
Mathematically:
Mz=M0(1−e−t/T1)M_z = M_0 (1 - e^{-t/T1})Mz=M0(1−e−t/T1)
At:
t = T1 → 63%
t = 5T1 → ~99%
Why tissues differ
Fat: tightly bound → short T1
Water / CSF: loosely bound → long T1
This difference = contrast
MRI sees how protons live, not just where they are.
9.13.2 T2 RELAXATION (SPIN–SPIN)
This is where students panic.
Don’t.
Key rule (memorize this sentence):
T2 has NOTHING to do with T1, except that they occur at the same time.
What happens right after 90° pulse
Spins are:
In XY-plane
In-phase
Strong signal is produced
Immediately:
Spins begin to lose phase coherence
Transverse magnetization decays
This loss of coherence = T2 relaxation
Why spins de-phase
Protons interact with neighboring protons
Local magnetic fields differ slightly
Some spins:
Speed up
Slow down
End result:
Vectors point in all directions
Net transverse signal → zero
T2 definition
T2 = time for transverse magnetization to decay to 37%
Equation:
Mxy=M0e−t/T2M_{xy} = M_0 e^{-t/T2}Mxy=M0e−t/T2
Important truths
T2 is:
Much faster than T1
Tens of milliseconds
Fat:
Dephases quickly → short T2
Water:
Dephases slowly → long T2
9.13.2.2 T2 RELAXATION (IMPERFECTION EFFECT)*
Now reality interferes.
T2* includes:
True T2 effects
PLUS:
Magnetic field inhomogeneity
Susceptibility differences
Chemical shift
Gradients
Relationship:
T1>T2>T2∗T1 > T2 > T2*T1>T2>T2∗
Or:
1T2∗=1T2+γΔB\frac{1}{T2*} = \frac{1}{T2} + \gamma \Delta BT2∗1=T21+γΔB
Spin-Echo vs Gradient-Echo
Spin Echo (180° pulse):
Removes inhomogeneity effects
Shows true T2
Gradient Echo:
No refocusing pulse
Shows T2*
9.14 ACQUISITION — LISTENING TO THE BODY
During relaxation:
Protons emit RF signals
Receive coils detect them
Critical rule
Receive coil must be perpendicular to B₀
Why?
If B₀ passes through coil → huge induced current
RF signal is drowned in noise
This is Faraday’s Law, not superstition.
FID (Free Induction Decay)
Signal immediately after excitation
Strong at first
Rapidly decays due to T2*
9.16 FOURIER TRANSFORM — TRANSLATION
MRI data is first:
In time domain
Image needs:
Frequency domain
Fourier Transform:
Converts time → frequency
Separates signals by:
Frequency
Phase
Amplitude
Without Fourier, MRI is just noise.
9.17–9.19 GRADIENTS — LOCATION, LOCATION, LOCATION
If B₀ were perfectly uniform:
All protons spin the same
No spatial information
No image
Gradients solve this.
Three gradients
Gradient | Purpose |
|---|---|
Slice Select (Gz) | Chooses slice |
Phase Encode (Gy) | Rows |
Frequency Encode (Gx) | Columns |
Slice Selection
Gradient ON + RF pulse
Only spins with matching frequency respond
Slice thickness depends on:
Gradient strength
RF bandwidth
Thin slice:
Better detail
Lower SNR
Phase Encoding
Applied briefly
Creates phase differences
Repeated many times
Determines image resolution
Frequency Encoding
Applied during signal readout
Creates frequency differences
Allows localization using Fourier Transform
9.20 K-SPACE — THE TRUTH BEHIND THE IMAGE
K-space:
Raw data matrix
NOT an image
Center:
Contrast information
Edges:
Detail (resolution)
When K-space is full:
Fourier Transform → image appears
The “miracle” is math, not magic.
FINAL MASTER SUMMARY (THIS IS GOLD)
RF pulse → excitation
T1 → energy loss (Z)
T2 → phase loss (XY)
Gradients → location
Fourier → image
K-space → raw truth
9.21 GRADIENT ECHO (GRE) PULSE SEQUENCE
(Understand this once, and half of MRI sequences stop being scary)
What is a Pulse Sequence?
A pulse sequence is simply:
The timetable of what the MRI machine does, and when it does it.
It shows:
RF pulses
Gradient pulses
Signal acquisition
all plotted against time
Think of it as a musical score for the scanner.
Why Gradient Echo?
Gradient Echo (GRE):
Uses gradients, not a 180° RF pulse, to form the echo
Faster than Spin Echo
More sensitive to T2* effects
GRE trades speed for susceptibility sensitivity.
Key Features of GRE (Memorize This Table)
Feature | GRE |
|---|---|
Flip angle | Small (< 90°) |
Refocusing | Gradient reversal |
Echo type | Gradient echo |
Sensitivity | T2* |
Scan time | Short |
Why Small Flip Angle?
Two consequences (very important):
Smaller signal
Shorter TR possible
Short TR → short scan time
MRI is always a compromise between signal and time.
Step-by-Step GRE Sequence Logic
RF pulse + Slice Select Gradient (GS)
Excites a slice
Introduces phase dispersion
Slice Rephasing Gradient
Corrects slice-selection dephasing
Phase Encoding Gradient (GPh)
Changes from TR to TR
Each step fills one k-space line
Readout Dephasing Gradient
Prepares spins for echo
Readout Gradient (GRO) + Acquisition
Signal sampled
Echo peak occurs at TE
This entire cycle fills one line of k-space.
Very Important Exam Line
RF, slice and readout gradients remain constant; phase encoding gradient changes each TR.
Repeat this 256 times → k-space full → Fourier Transform → image.
9.22 GRADIENT SPECIFICATIONS (WHY HARDWARE MATTERS)
If MRI were a car:
Gradients are the engine
Three Key Gradient Specs
Parameter | Meaning | Desired |
|---|---|---|
Max strength | How strong the gradient can be | High |
Rise time | Time to reach max | Short |
Slew rate | Strength / rise time | High |
Why They Matter
Faster gradients → shorter TE, TR
Enables:
Fast imaging
EPI
DWI
fMRI
Many “advanced” MRI techniques fail not because of software—but because of weak gradients.
9.23 MRI IMAGE QUALITY
(This is where marks are gained or lost)
Image quality depends on three pillars:
Signal-to-Noise Ratio (SNR)
Contrast Resolution
Spatial Resolution
Signal-to-Noise Ratio (SNR)
SNR = useful signal ÷ background noise
Noise comes from:
Patient (thermal motion)
Electronics
Coils
Field inhomogeneity
Fixed vs Controllable Factors
You cannot change:
Magnet imperfections
Patient size
Electronics noise
You can change:
RF coil
Voxel size
NEX
Bandwidth
TR / TE / Flip angle
Golden Rule
Improve SNR → improve contrast resolution
9.23.2 PIXEL, VOXEL, MATRIX (ABSOLUTE EXAM FAVORITE)
Pixel → 2D picture element
Voxel → 3D tissue volume
Matrix → grid of pixels
Voxel size =
FOVMatrix×Slice Thickness\frac{FOV}{Matrix} \times Slice\ ThicknessMatrixFOV×Slice Thickness
Smaller voxel
Higher spatial resolution
Lower SNR
Larger voxel
Lower resolution
Higher SNR
Resolution and SNR are enemies.
9.23.3 INTER-SLICE GAP (WHY GAPS EXIST)
Slices are not perfectly rectangular.
Problem:
RF excites adjacent slices
Causes cross-talk
Reduces SNR
Solution:
Inter-slice gap (25–50%)
Spin-echo needs gaps.
3D imaging avoids this problem.
9.23.4 MATRIX & FOV EFFECTS
Matrix Size
128×128 → coarse
512×512 → fine
Fine matrix:
Better detail
Worse SNR
Longer scan time
Field of View (FOV)
Doubling FOV:
Voxel volume ↑ ×4
SNR ↑ ×4
Halving FOV:
SNR ↓ ×4
Increasing FOV is the most efficient way to increase SNR.
9.23.5 TR, TE, FLIP ANGLE (CONTRAST CONTROLS)
TR (Repetition Time)
Controls T1 contrast
Long TR → high SNR
Short TR → T1 weighting
TE (Echo Time)
Controls T2 contrast
Long TE → T2 weighting
Short TE → high SNR
Flip Angle
Large flip → higher sig
nal
Small flip → faster scan
GRE lives on small flip angles.
Classic Rule
Long TR + Short TE → best SNR
Short TR + Long TE → worst SNR
9.23.6 NEX (AVERAGES)
SNR ∝ √NEX
Double NEX → SNR ×1.41
Scan time doubles
NEX improves SNR slowly but increases time fast.
9.23.7 RECEIVER BANDWIDTH
Lower bandwidth → higher SNR
But:
Longer readout
Longer minimum TE
More chemical shift
Always a compromise.
9.24 MRI CONTRAST AGENTS
Why We Need Them
Sometimes tissues look too similar.
MRI contrast agents:
Alter relaxation times
Do NOT “block X-rays” like CT contrast
Two Main Types
Type | Effect | Image |
|---|---|---|
T1 agents (Gd) | Shorten T1 | Bright |
T2 agents (Iron) | Shorten T2 | Dark |
Mechanism
Contrast agents:
Interact with water protons
Increase relaxation rate
1/T=1/T0+rC1/T = 1/T_0 + rC1/T=1/T0+rC
9.25 SPECIAL APPLICATIONS (HIGH-YIELD)
MRA / MRV
Visualize blood flow
Flowing blood = bright
Uses GRE
Can be:
Non-contrast
Gadolinium-enhanced
MR Myelography
Heavy T2 weighting
CSF = bright
Cord = dark
Replaced X-ray myelography
MRCP
Heavily T2-weighted
Bile & pancreatic ducts = bright
No contrast needed
Chemical Shift Imaging (CSI)
Spectrum per pixel
Combines MRI + spectroscopy
Very long scan
Small matrix
Diffusion-Weighted Imaging (DWI)
Measures Brownian motion
Restricted diffusion:
High DWI
Low ADC
⚠ Always confirm on ADC
(T2 shine-through is real)
FINAL OLD-TUTOR SUMMARY
If you remember only this, you will pass:
GRE → fast, T2*
SNR ↔ voxel size
TR → T1
TE → T2
FOV ↑ → SNR ↑↑
Matrix ↑ → detail ↑, SNR ↓
DWI needs ADC confirmation
MRI is not memorization.
It is cause and effect.