1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio...

34
1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan Magnetic Resonance Radio frequency absorption Relaxation: Radio frequency emission Gradients Increases signal/noise: antenna selection, field strength. Excellent references: www.cis.rit.edu/htbooks/mri/ www.easymeasure.co.uk/principlesmri.aspx

Transcript of 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio...

Page 1: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

1

MRI Physics 1: Image Acquisition

Chris Rorden & Paul Morgan– Magnetic Resonance– Radio frequency absorption – Relaxation: Radio frequency emission– Gradients– Increases signal/noise: antenna selection, field strength.

Excellent references:– www.cis.rit.edu/htbooks/mri/– www.easymeasure.co.uk/principlesmri.aspx

Page 2: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

2

Units of magnetic strength

Tesla and Gauss are measures of magnetic field strength– Earth’s magnetic field ~0.5 Gauss.– 1Tesla = 10,000 Gauss.– Our fMRI system is 3T.

~x60,000 earth’s field strength

Page 3: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

3

Anatomy of an atom

Atoms are the building blocks of our world. Composed of 3 components

– Electrons: tiny negatively charged particles.– Protons: heavy positively charged particles.– Neutrons: heavy particles without charge.

Electrons are often thought of like planets: tiny objects distantly orbiting a massive core.

Neutrons and protons form the dense nucleus of an atom.

Page 4: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

4

Atomic Nuclei Atomic nuclei are composed of protons and neutrons. Protons determine the element, e.g. hydrogen has one proton, helium has two. Neutrons determines the isotope.

– Helium: Usually, two neutrons: 4He. Rarely, only have one neutron: 3He.

– Hydrogen Usually, no neutrons: 1H. Rarely, Deuterium (2H) is found in ‘heavy’ water Tritium (3H) is radioactive (spontaneous decay).

4He 3He 1H 2H

Page 5: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

5

Nuclear Magnetic Resonance

Felix Block and Edward Purcell– 1946: the nuclei of some elements absorb and re-emit radio frequency energy

when in magnetic field– 1952: Nobel prize in physics

Atoms with odd number of protons/neutrons spin in a magnetic field– Nuclear: properties of nuclei of atoms– Magnetic: magnetic field required– Resonance: interaction between magnetic field and radio frequency

Bloch Purcell

Page 6: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

6

How fast do hydrogen atoms spin?

Field Strength (Tesla)

180

401.0 4.0

The rate of rotation is determined by the strength of the magnetic field.

Larmor equationf = B0

For Hydrogen, = 42.58 MHz/T

At 1.5T, f = 63.76 MHzAt 3T, f = 127.7 MHz

Res

on

ance

Fre

qu

ency

(M

Hz)

Page 7: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

7

Radiofrequency Pulses

A radiofrequency (RF) pulse at the Larmor frequency will be absorbed.

This higher energy state tips the spin, so it is no longer aligned to the field.

An RF pulse at any other frequency will not influence the nuclei.

This is resonance.

Page 8: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

8

Source of MR signal

At rest, atoms align parallel to magnetic field.– Lowest energy state.

After RF absorption, net magnetization is orthogonal to magnetic field– RF emission at larmor frequency– RF emission decays with time

Page 9: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

9

Absorption and Relaxation

Our RF transmission is absorbed by atoms at Larmor frequency.

After the RF pulse, atoms will begin to realign with the magnetic field: relaxation

During this period, an RF signal is emitted.This signal will be at the Larmor frequency.An antenna can measure this signal.

Page 10: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

10

Hydrogen is the mainstay for MRI

We will focus on Hydrogen– Hydrogen abundant in body (63% of atoms).– Elements with even numbers of neutrons and protons have no

spin, so we can not image them (4He, 12C).– 23Na and 31P are relatively abundant, so can be imaged.

Larmor frequency varies for elements:– 1H = 42.58 Mhz/T– 13C = 10.7 Mhz/T– 19F = 40.1 Mhz/T– 31P = 17.7 Mhz/T

Therefore, by sending in a RF pulse at a specific frequency we can selectively energize hydrogen.

Page 11: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

11

Electromagnetic Spectrum

MRI signals are in the same range as FM radio and TV (30-300MHz). MRI frequency is non-ionizing radiation, unlike X-rays. Absorbed RF will cause heating. Specific absorption rate (SAR): measure of the energy absorbed by tissue.

– Increases ~ with square of field strength.– Higher SAR = more energy = more signal = more heating– FDA limits SAR, and is a limiting factor for some protocols (3 W/kg averaged over 10

minutes).

Ioni

zing

Rad

iatio

nB

reak

s B

onds

Non

-Ion

izin

g R

adia

tion

Hea

ting

Excites Electrons

Excites Nuclei

Page 12: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

12

Making a spatial image

To create spatial images, we need a way to cause different locations in the scanner to generate different signals.

To do this, we apply gradients. Gradients make the magnetic field slightly stronger

at one location compared to another. Lauterbur: first MRI: 2003 Nobel Prize.

Lauterbur

Page 13: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

13

Slice Selection Gradient

Gradients make field stronger at one location compared to another.

Larmor frequency different along this dimension.

RF pulse only energizes slice where field strength matches Larmor frequency.

Fie

ld S

tren

gth

Z Position

128

Mh

z

127

Mh

z

126

Mh

z127 MhzRF pulse

LarmorFreq

Page 14: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

14

Slice Selection Gradient

Gradual slice selection gradients will select thick slices, while steep gradients select thinner slices.

– The strength of your scanner’s gradients can limit minimum slice thickness.– FDA limits speed of gradient shift (dB/dt) and some of our protocols can

elicit slight tingling sensation or brief muscle twitches. Position of gradient determines which 2D slice is selected.

Fie

ld S

tren

gth

Z Position

Fie

ld S

tren

gth

Z Position

Fie

ld S

tren

gth

Z Position

Fie

ld S

tren

gth

Z Position

Page 15: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

15

Phase encoding gradient

Orthogonal gradient applied between RF pulse and readout This adjusts the phase along this dimension. Analogy: Phase encoding is like timezones. Clocks in

different zones will have different phases.Y

Pos

ition

Field Strength

Page 16: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

16

Frequency encoding gradient

Apply final orthogonal gradient when we wish to acquire image.

Slice will emit signal at Lamour frequency, e.g. lines at higher fields will have higher frequency signals.

Aka ‘Readout gradient’.

X P

ositi

on

Field Strength

Page 17: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

17Source: Traveler’s Guide to K-space (C.A. Mistretta)

Raw MRI image: K-Space

Raw MRI is 2D Frequency Map.Apply Fourier Transform to reconstruct image.

Page 18: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

18

Reconstruction

Medical scanners automatically reconstruct your data. You can manually reconstruct data using Tokarczuk’s

free Intel Reconstruction Tool: www.mricro.com/import.html

Fourier Transforms are slow: 1021-sample data requires >2 million multiplications (2*N2)

Fast Fourier Transform: 1024-sample data requires 20,000 multiplications. (2(N log N))– Optimal when data is power of two (64,128,256, 512), reverts

to traditional Fourier for prime numbers– This is why most image matrices are a power of 2.

Page 19: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

19

MRI scanner anatomy

A helium-cooled superconducting magnet generates the static field.– Always on: only quench field in

emergency.– niobium titanium wire.

Coils allow us to – Make static field homogenous

(shims: solenoid coils)– Briefly adjust magnetic field

(gradients: solenoid coils)– Transmit, record RF signal (RF

coils: antennas)

Page 20: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

20

MRI scanner anatomy

Magnet Gradient RF Transmit RF Receive

Antennas

Page 21: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

21

EPI

In conventional MRI, we collect one line of our matrix with each RF pulse.

So a 64x64 matrix with a TR of 2sec will be generated in 128 seconds.

Problem: this is unacceptable if the object changes rapidly:

– Images of the heart: shape changes quickly, conventional image would be blurred.

– Imaging brain activity: could not see changes that occur within a few seconds.

Echo Planar Imaging: By rapidly applying the frequency gradient, we can collect a 2D slab with a single RF pulse.

Page 22: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

22

Echo Planar Imaging

EPI was devised in 1977 by Sir Mansfield.– 2003 Nobel Prize.

EPI remains the principle technique for fMRI acquisition.– Alternative is ‘spiral’ imaging.

EPI does have a cost:– Image warping due to slow

encoding.

Mansfield

Multi-shotEPI

www.fmrib.ox.ac.uk/~karla/

Page 23: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

23

MRI terminology

Orientation: typically coronal, sagittal or axial, can be in-between these (oblique)

Matrix Size:– Voxels in each dimension

Field of view:– Spatial extent of each

dimension. Resolution:

– FOV/Matrix size.

Axial Orientation64x64 Matrix192x192mm FOV3x3mm Resolution

Sagittal Orientation256x256 Matrix256x256mm FOV1x1mm Resolution

Page 24: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

24

1mm Gap

2mm Thick

Volumes

3D volumes are composed of stacks of 2D slices, like a loaf of bread.

Each slice has a thickness.– Thicker slices have more hydrogen, so

more signal Volume of 1x1x1mm voxel is 1mm3

Volume of 1x1x2mm voxel is 2mm3

– Thinner slices provide higher resolution. Optional: gap between slices.

– Reduces RF interference– Allows fewer slices to cover whole brain.

3mm

Page 25: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

25

Creating 3D volumes from 2D EPI

Slices can be either collected sequentially (e.g. ascending axial slices) or in interleaved order (e.g. collect all odd slices, then all even slices).

……

Sequential Interleaved

Time Time

Page 26: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

26

Sequential vs Interleaved Volumes

Interleaving reduces interference between slices. Useful if thin gap between slices.

Unfortunately, any head movements will cause worse ‘spin history’ effects for interleaved slices than sequential. (TR will be shorter for regions that were previously in another slice).

You must know slice order if you want to ‘slice time correct’ data (temporal processing lecture).

Slice 4

Slice 3

Slice 2

Slice 1

Slice 4

Slice 3

Slice 2

Slice 1

Slice 4

Slice 3

Slice 2

Slice 1

Page 27: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

27

Signal to Noise

Signal To noise is given by the formulaSignal = VN

Where V is the volume and N is the number of samples averaged (referred to as ‘Nex’, as in ‘number of excitations’).

For example, to get the same SNR as a single 3x3x3mm scan (27mm3) we would need to collect 12 2x2x2mm (8mm3) scans or 768 1x1x1mm (1mm3) scans.

Page 28: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

28

Signal to Noise: Antennas

Volume coil Surface coilHead coil

www.fmrib.ox.ac.uk/~karla/

Surface coil

The MRI antenna is called a coil.We use different coils for different body parts.For brains, the most common antenna is the head

coil, which is a volume coil: it shows the whole brain.We can also use a surface coil: it gives great signal

for a small field of view.

Page 29: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

29

Parallel Imaging (SENSE, iPat)

Parallel imaging uses multiple surface coils to generate a volume image.

Dramatically reduces spatial distortion and increases signal.

Optionally, you can acquire images more rapidly by only collecting a portion of k-space.– SENSE R=2 collects half of the lines.– SENSE R=3 collects one third– Reduces spatial distortion and increases speed

of acquisition. Some loss in signal.

8-channel array

Page 30: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

30

Parallel Imaging (SENSE, iPat)

Increasing SENSE reduction factor decreases acquisition time and spatial distortion, but high values lead to reduced signal.

Eff

ect

s of

SEN

SE f

act

or

(R)

on E

PI

R=1 R=2 R=3

Page 31: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

31

Outside magnetic field •Spins randomly oriented

In magnetic field:•Spins tend to align parallel or anti-parallel to magnetic field.•At room temperature, ~4 parts per million more protons per Tesla align with versus against field.•As field strength increases, there is a bigger energy difference between parallel and anti-parallel alignment (faster rotation = more energy).

•A larger proportion will align parallel to field.•More energy will be released as nuclei align.•Therefore, MR signal increases with square of field strength.

Signal and Field Strength

Page 32: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

32

Signal and Field Strength

Most clinical MRI: 1.5T Our fMRI systems: 3.0T Maximum for NbTi MRI ~11.7T World record for superconductive MRI ~22T (Nb3Sn) Field strength influences:

– Faster Larmor frequency : Bigger energy difference between parallel and anti-parallel alignment

• Larger ratio of nuclei aligned = more signal• More signal as nuclei realign.

Reduced TR and TE: less time to take images (next week).

Page 33: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

33

Signal and Field Strength In theory:

– Signal increases with square of field strength– Noise increases linearly with field strength– A 3T scanner should have twice SNR of 1.5T scanner; 7T should have ~4.7

times SNR of 1.5T. Unfortunately, physiological artifacts also increase, so advantage is less in

practice. Benefits: speed, resolution Costs: Artifacts, Money, SAR, wavelength effects, auditory noise

Page 34: 1 MRI Physics 1: Image Acquisition Chris Rorden & Paul Morgan –Magnetic Resonance –Radio frequency absorption –Relaxation: Radio frequency emission –Gradients.

34

Magnetic attraction

Force in magnetic field (1.8T, unit dynes)– Water: -22– Copper: -2.6– Copper Chloride: +280– Iron: +400,000

Diamagnetic material repelled (e.g. H2O). Paramagnetic material attracted (e.g. CuCl, Gd). Ferromagnetic material strongly attracted (Fe).

– Even without magnetic field, magnetic moments aligned– Dangerous near MRI scanner