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Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 otes: Walter Block and Frank R Korosec, PhD Departments of Biomedical Engineering 1, Radiology 2 and Medical Physics 3 University of Wisconsin - Madison

Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

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Page 1: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Medical Imaging Systems:MRI Image Formation

Instructor: Walter F. Block, PhD 1-3

Notes: Walter Block and Frank R Korosec, PhD 2-3

Departments of Biomedical Engineering 1,Radiology 2 and Medical Physics 3

University of Wisconsin - Madison

Page 2: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

MRI Physics: So far...

What we can do so far:

1) Excite spins using RF field at o2) Record time signal (Known as FID)3) Mxy decays, Mz grows4) Repeat.

But so far RF coils only integrate signal from entire body. We have no way of forming an image. That brings us to the last of the three magnetic fields in MRI.

Page 3: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Image Formation Overview

• Gradient fundamentals• Slice Selection

• Limit excitation to a slice or slab• Can be in any orientation

• Gradient echo in-plane spatial encoding• Radial imaging ( like CT)• Frequency encoding• Phase encoding

Page 4: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

3nd Magnetic Field • Static High Field

• Termed B0

• Creates or polarizes signal• 1000 Gauss to 100,000 Gauss

• Earth’s field is 0.5 G

• Radiofrequency Field (RF)• Termed B1

• Excites or perturbs signal into a measurable form• O.1 G but in resonant with signal

• Gradient Fields • 1 -4 G/cm• Used to determine spatial position of signal• MR signal not based directly on geometry

Page 5: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Gradient Coils

Fig. Nishimura, MRI Principles

Page 6: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

X Gradient Example: Gx

Magnetic field all along z, but magnetic strength can varies spatially with x. Stronger at right, no change in middle, weaker at left.

Page 7: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Gradient Coil Fundamentals

• Gradient strength directly proportional to current in coil• On the order of 100 amps peak

• Performance• Power needed proportional to radius5

• Tight bore for patient• Strength – G/cm or mT/m

• 4 G/cm is near peak now for clinical scanners• Higher strength with localized gradients (research only)

• Slew rate• Need high voltages to change current quickly• 100- 200 T/m/s is high performance

• Rise to 1 G in .1 ms at 100 T/m/s• Limited by peripheral nerve stimulation

Page 8: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Magnetic Field Gradient Timing Diagrams

Page 9: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

B0

Larmor Equation

PrecessionalFrequency

Static Magnetic Field

tB0 + Gx(t)x)

Before, only B0

Now with Gx

Page 10: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Gx, Gy, Gz: One for each spatial dimension

Magnetic field all along z, but magnetic strength can vary spatially with x, y, and/or z.

Page 11: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Two Object Example of Spatial Encoding

x

m(x)

t

sr(t)

Receiver Signal: No gradient

Gx On: Beat Frequency Demodulated Signal

Water

Page 12: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Gz Gradient Example

The effects of the main magnetic field and the applied slice gradient. In this example, the local magnetic field changes in one-Gauss increments accompanied by a change in the precessional frequency from chin to the top of the head.

Image, caption: copyright Proruk & Sawyer, GE Medical Systems Applications Guide, Fig. 11

Page 13: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Selective RF Excitation

Build RF pulse from sum of narrow frequency range

Recall frequency of RF excitation has to be equal

or in resonance with spins

Page 14: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Slice Selection- Consider a pulse B1(t) that is multiplied by cos(ot). This is called

modulation .

B1(t) is called the RF excitation.

o is the carrier frequency = B0. Mixer

cos(ot)

B1(t) cos(ot)

A(t)

o f

Frequency profile of modulated RF pulse

o = 2fo

Page 15: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical
Page 16: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Frequency Encoding

Spin Frequency (x)

Image each voxel along x as a piano key that has a different pitch. MR coil sums the “keys” like your ear.

Page 17: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Frequency Encoding

Page 18: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

GRE Pulse Sequence Timing Diagram

SliceSelect

Freq.Encode

rf

Signal

°

TE

Page 19: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Frequency Encoding & Data Sampling

FrequencyEncoding

GeneratedSignal

DAQ

SampledSignal

Page 20: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

In-plane Encoding

• MR signal in frequency encoding (x) is Fourier transform of projection of object

• Line integrals along y

• Encoding in other direction • Vary angle of frequency encoding direction

• 1D FT along each angle and Reconstruct similar to CT

• Apply sinusoidal weightings along y direction• Spin-warp imaging or phase-encoding

• By far the most popular

Page 21: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

2D Projection Reconstruction MRI

kx

Gx

Gy

DAQ

Reconstruction: convolution back projection or filtered back projection

ky

Page 22: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Central Section Theorem in MRI

In MR, echo gives a radial line in spatial frequency space (k-space).

x’

x’

y’

x

y

Interesting - Time signal gives spatial frequency information of m(x,y)

ky

kx

F.T.

θ

θ

Object

CT Projection

MR Signal (t)

Page 23: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

k-Space Acquisition (Radial Sampling)

ky

kx

Y readout

X readout

kx

ky

Page 24: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

In-plane Encoding

• MR signal in frequency encoding (x) is Fourier transform of projection of object

• Line integrals along y

• Encoding in other direction • Vary angle of frequency encoding direction

• 1D FT along each angle and Reconstruct similar to CT

• Apply sinusoidal weightings along y direction• Apply prior to frequency encoding• Repeat several times with different sinusoidal weightings• Spin-warp imaging or phase-encoding• By far the most popular

Page 25: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Phase Encoding: Apply Gy before Freq. encoding

Page 26: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

GRE Pulse Sequence Timing Diagram

SliceSelect

PhaseEncode

Freq.Encode

rf

Signal

°

TE

Page 27: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

PhaseDirection

Frequency DirectionOne line of k-space

acquired per TR

k-Space Acquisition

PhaseEncode

DAQ

SampledSignal

kx

ky

Page 28: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

kx

ky

k-Space Signal

Page 29: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

8 x 8512 x 512

Page 30: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

16 x 16512 x 512

Page 31: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

32 x 32512 x 512

Page 32: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

64 x 64512 x 512

Page 33: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

128 x 128

512 x 512

Page 34: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

256 x 256

512 x 512

Page 35: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

512 x 32512 x 512

Page 36: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Scan Duration

Scan Time = TR PE NEX

TR = Repetition TimePE = Number of phase encoding valuesNEX = Number of excitations (averages)

Page 37: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

GRE Pulse Sequence Timing Diagram

SliceSelect

PhaseEncode

Freq.Encode

rf

Signal

°

TE

Page 38: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Images of the Knee

-weighted T2-weightedNeeds longer TE

Page 39: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

T2 & T2* Relaxation: Sources of Image Contrast

Mxy

Time

T2*

T2

T2*

1 =T2

1 + B0

Page 40: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

t

Gx(t)

6GRADECH.AVI

Effects of Local Magnetic Inhomogeneity

Page 41: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Perils of Gradient Echo Imaging and T2*

TE = 8 ms TE = 24 ms

0.17 T GE Orthopedic Scanner

Page 42: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Image Formation Overview

• Gradient fundamentals• Slice Selection

• Limit excitation to a slice or slab• Can be in any orientation

• Gradient echo in-plane spatial encoding• Radial imaging• Frequency encoding• Phase encoding

Page 43: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

T1-, T2-, and Density-Weighted Images

T1-weighted T2-weighted -weighted

Page 44: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

T2-Weighted Image of the Spine

Page 45: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Images of the Knee

-weighted T2-weighted

Page 46: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

T1-, T2-, and Density-Weighted Images

T1-weighted T2-weighted -weighted

Page 47: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Spin Echo Parameters

TR TE

T1-weighting short (400 msec) short (20 msec)

T2-weighting long (3000 msec) long (100 msec)

-weighting long (3000 msec) short (20 msec)

Page 48: Medical Imaging Systems: MRI Image Formation Instructor: Walter F. Block, PhD 1-3 Notes: Walter Block and Frank R Korosec, PhD 2-3 Departments of Biomedical

Signal vs Weighting

T1-weighting long T1, small signal short T1, large signalT2-weighting long T2, large signal short T2, small signal-weighting high , large signal low , small signal

T1-weighted T2-weighted -weighted