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MRI Physics for Technologists: A Beginner's Guide

Unlike X-ray, CT, or nuclear medicine, MRI uses no ionizing radiation. Instead, it leverages the magnetic properties of hydrogen protons in the body to create incredibly detailed images of soft tissues. This beginner's guide covers the MRI physics that every MR technologist must understand — from basic principles through practical sequence selection.

Before You Read: What Makes MRI Different

MRI doesn't produce images by measuring how much radiation passes through or is emitted from the body. Instead, it excites hydrogen protons with radio waves, then listens to the signal they emit as they relax back to equilibrium. The spatial location is encoded by precisely varying the magnetic field across the patient. No radiation, no moving X-ray tube — just magnets, radio waves, and sophisticated mathematics.

The Three Pillars of MRI Physics

All of MRI rests on three physical phenomena. Understanding these is the foundation for everything else:

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Magnetic Field (B0)

The main static magnetic field, measured in tesla (T). Clinical strengths: 1.5 T and 3.0 T. Higher field = more signal, better resolution, but more artifacts.

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RF Pulses

Radiofrequency energy at the Larmor frequency excites protons, knocking them out of alignment with B0. The same coil that transmits RF also receives the return signal.

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Gradients

Three sets of gradient coils create linear variations in the magnetic field along X, Y, and Z axes. They encode spatial position into the signal.

The Larmor Frequency: Why Protons Resonate

The equation at the heart of MRI is the Larmor equation:

ω₀ = γ × B₀

At 1.5 T: Larmor frequency = 42.58 × 1.5 = ~63.9 MHz
At 3.0 T: Larmor frequency = 42.58 × 3.0 = ~127.8 MHz

The RF pulse must be at the Larmor frequency to transfer energy to the protons. This is why different field strengths need different RF frequencies — and why RF shielding must be appropriate for the operating frequency.

T1 and T2 Relaxation: The Basis of Contrast

After an RF pulse knocks protons out of alignment, two independent relaxation processes occur simultaneously:

T1 Relaxation (Spin-Lattice)

T1 is the time constant for the longitudinal magnetization to recover to 63% of its original value. It represents protons giving energy back to the surrounding molecular lattice.

T2 Relaxation (Spin-Spin)

T2 is the time constant for the transverse magnetization to decay to 37% of its initial value. It represents protons losing phase coherence due to spin-spin interactions.

Clinical Appearance by Sequence

TissueT1-WeightedT2-WeightedFLAIR
CSF / WaterDark ↓Bright ↑↑Dark ↓ (suppressed)
FatBright ↑↑IntermediateIntermediate
Gray matterGrayGrayGray
White matterLight grayDark grayDark gray
Edema / TumorDark ↓Bright ↑↑Bright ↑↑
Bone (cortex)Dark ↓Dark ↓Dark ↓
Blood (acute)IntermediateDark ↓Variable
Gadolinium contrastBright ↑↑ (on T1)VariableVariable

Memory Aid

"T1 — Fat is bright." Think of T1 as the "anatomy" sequence — structures are well-defined, fat is white, water is black.

"T2 — Water is bright." Think of T2 as the "pathology" sequence — anything with excess fluid (edema, tumor, inflammation) is white.

TR and TE: The Knobs You Control

TR (Repetition Time) — The time between successive RF pulses applied to the same slice. Controls how much T1 relaxation is allowed.

TE (Echo Time) — The time between the RF pulse and the peak of the signal echo. Controls how much T2 decay is allowed.

SequenceTRTE
T1-weightedShort (400–800 ms)Short (10–30 ms)
T2-weightedLong (2000–5000 ms)Long (80–120 ms)
PD-weightedLong (2000–5000 ms)Short (10–30 ms)
FLAIRLong (6000–10000 ms)Long (80–140 ms) + inversion pulse

Gradient Coils: Spatial Encoding

Without gradients, every proton would experience the same magnetic field and resonate at the same frequency — producing a signal but with no spatial information. Gradient coils create linear variations in the magnetic field along each axis:

Gradients are also responsible for the loud knocking sounds during MRI — the rapid switching of currents through gradient coils causes mechanical vibration (the Lorentz force on the coils).

RF Coils: The Antennas

RF coils function as both transmitters (sending RF pulses) and receivers (detecting the MRI signal). Different coils are optimized for different body parts:

Coil TypeLocationBest For
Body coil (built-in)Inside the boreWhole-body imaging, large FOV
Head coilEncloses the headBrain, orbits, sinuses (highest SNR)
Spine coilEmbedded in tableCervical, thoracic, lumbar spine
Surface / Phased-arrayPlaced on body surfaceKnee, shoulder, breast, wrist — high resolution near the coil
Cardiac coilAnterior + posterior arrayCardiac MRI, MR angiography

Phased-array coils with multiple receiver elements allow parallel imaging (GRAPPA, SENSE) which reduces scan time by using multiple coil elements to partially replace gradient-encoded spatial information.

Key MRI Safety Concepts

MRI has unique safety concerns that every technologist must know:

Putting It Together: A Basic MRI Sequence

  1. Patient is placed in the bore. B₀ aligns hydrogen protons with the main field
  2. A slice-select gradient (Z) is turned on. An RF pulse at the Larmor frequency excites protons in the selected slice
  3. The phase-encoding gradient (Y) is applied briefly to encode Y position
  4. The frequency-encoding gradient (X) is turned on. The MR signal is read (this is the "echo")
  5. Steps 2-4 are repeated with different phase-encoding amplitudes for each line of k-space
  6. The 2D k-space data is Fourier-transformed to produce the image
  7. For 3D imaging, the slice-select gradient is also phase-encoded instead of selecting a single slice

For more on how MRI compares to other modalities, see CT vs MRI: When to Use Which and explore our MRI modality overview.

About the author: This guide was prepared by the Radiography 101 Clinical Team, referencing MRI in Practice (Westbrook & Talbot, 5th ed.), Handbook of MRI Technique, and current ARRT MR exam standards. Content is reviewed for clinical accuracy.