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8/6/2019 MRI Principles
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Yves De Deene
MRI PRINCIPLES
NMR imaging is non-invasive
Strong static magnetic field
Radiofrequent electromagnetic waves
Space and time dependent magnetic fields
MRIMRS MRRMM agnetic
RR esonantceSS pectroscopy
MM agneticRR esonance
ImagingImaging
MM agneticRR esonance
RR elaxometry
Spectra Relaxation timesDiffusion coefficients
Images
tt
R1,2
M M
g(R 1,2)
NN .. MM .. RRNN .. MM .. RR
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NN .. MM .. RRNN .. MM .. RR
Water
H2O
m p = 1,67.10 -24 g
mp = 0,00000000000000000000000167 g
+ ++++
++++
+q p = 1,6.10 -19 C
q p = 0,00000000000000000016 C
Properties of the atomic nucleus
.( 1) L I I = +. z I L m=
.( / 2 ) p L p pg q m L =
, .( / 2 ) p z L p p zg q m L =
N
Z
Otto Stern
Walther Gerlach Nobel price for physics in 1943
Discovery: Nuclear spin momentum of the proton19221922Frankfurt
Discovery of Nuclear Magnetic Resonance19381938
Nobel price physics in 1944
Isidor Isaac Rabi
From left to right: N. Bohr,J. Franck, A. Einstein, I. Rabi
Z
N
Z
Z
N
N
New York
( ) z
H F z
=
H z
H z
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( )dM
M Bdt
=
B
M
The Bloch equation
dM dt
Nuclear Magnetic Resonance:Nuclear spin precession
Cross-section of an NMR scanner
Water molecule
Cryogenic magnet
Radiofrequency coil
Gradient coil
Hydrogenproton transmitsaradiofrequent electromagneticwave(yellow) afterexcitationbyan RFpulse(red)
B0
B0 B0 B0
2 RF f B
=
EXCITATION PULSE
COIL
ImageProcessing(2D-FFT)
Nuclear Magnetic Resonance Imaging:Basic principle
Topview of precession(transverse plane)
= . B
EXCITATION
COIL OBJECT:spin-system
SIGNAL RECEPTION
COIL OBJECT:spin-system
Nuclear Magnetic Resonance Imaging:Excitation and signal reception
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= . BNuclear Magnetic Resonance Imaging:Dephasing
IN PHASE OUT OF PHASE
Illinois
First discovery of a spin-echo
- E. Hahn (1950) -
19491949
Erwin Hahn
Pulsed field NMRThe spin-echo experiment
Excitationpulse
Refocusingpulse
TE
Excitationpulse
Refocusingpulse
TR
Erwin Hahn1949
TE/2 TE/2
REFOCUSSINGPULSE
EXCITATIONPULSE
N
ZZ
N
Pulsed field NMRThe spin-echo experiment
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Excitationpulse
Refocusing-pulse
TE/2 TE/2
MAGNETIC DIPOLE MOMENT PHASORS
Pulsed field NMRThe spin-echo experiment
Erwin Hahn1949
NicolaasBloembergen
RobertPound
EdwardPurcell
EXCITATIONPULSE
REFOCUSINGPULSE
EXCITATIONPULSE
REFOCUSINGPULSE
Nuclear Magnetic Resonance Imaging:Relaxation mechanisms
B 0
BL
tOnewater molecule
BL
tManywater molecules
c
T1, T2
T1(64 MHz)
T2(64 & 128 MHz)
01
liquids solids
1210
410
110
110
910 610
T1(128 MHz)
c
T
Nuclear Magnetic Resonance Imaging:Relaxation mechanisms
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INTERMEDIATELAYER
FREEWATER
Hydrogen bridges
C
C
OO
C N BOUNDLAYER
+
+ +
+
-
-- +
+
- - +
-
- +
+++
Relaxation theory in tissue(Daskiewicz, Zimmerman, Brittin, Edzes en Samulski)
J
0
BL
t
F
Bound layer
Intermediatelayer
Free water
R2mosteffective
R1mosteffective
0 = 1/ c
0 > 1/ c
0 < 1/ c
Pound PurcellBloembergen
INTERMEDIATELAYER
FREEWATER
Hydrogen bridges
C
C
OO
C N BOUNDLAYER
+
+ +
+
-
-- +
+
- - +
-
- +
+++
Protein, polymer, cell membrane
M
M
M
t
t
tLow mobility
High mobility
Contrast in MR images is determinedby the interaction of spin systems
Nuclear Magnetic Resonance Imaging:Two important relaxation mechanisms
Spin-lattice relaxation Spin-spin relaxationT1 T2
Energy transfered to lattice (phonons)
Entropy increases
Repopulation of spins between spin energy levels
Restoration of longitudinal magnetization
Energy transferred between spins
No entropy change of total spin system
No repopulation of spins between spin energy levels
Dephasing of transverse magnetization
time
B0
time
B0
Interactions with magnetic field fluctuations at Larmor frequency Interactions with magnetic field fluctuations at low frequency
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From nuclear magnetic resonance signal to Magnetic Resonance ImagingAn analogon in acoustics
1 2
1
2
3
From nuclear magnetic resonance signal to Magnetic Resonance ImagingAn analogon in acoustics:
Localisation of glasses close together
Frequency encoding
Spatial encoding of the NMR signal is based onfrequency changes in the precession
B
M
B
M
B
M
RF COIL
Fouriertransform
/ f =
4.7 m =
64 f MHz=
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Nature 242, (1973), 190-191
Illinois / Nottingham
19731973
Nobel price for physiology and medicine (Lauterbur & Mansfield) in 2003
Paul Lauterbur Peter Mansfield
NMR scanner with backprojection
Zurich
19741974
Richard Ernst
NMR scanner with 2D Fourier transformation
Nobel price for chemistry in 1991
Slice selection
1.52 T
B
z
64.8 MHz
f = 64.8 MHz
= . B
Spatial encoding of the NMR signal
GRADIENT COILS
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Spatial encoding of the NMR signal
Frequency encoding
MHz64 6860
T1.5 1.61.4 = . B
BG
x
SLICE SELECTION
B
z
EXCITATIONPULSE
R = 64.8 MHz B = 1.52 T
f = 64.8 MHz
1.52 T
= . B
1.52 T
EXCITATIONPULSE
PHASE ENCODING
B
y
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EXCITATIONPULSE
REFOCUSINGPULSE
1.4
FREQUENCY ENCODING
B
y
T1.5 1.6
SLICE SELECTION
2D-FOURIERTRANSFORM
FREQUENCY AND PHASE ENCODING
FREQUENCY
PHASE
AMPLITUDEIMAGE
(f , )
The first MRI scanners ...
and recent ones
Mobile MRI unitOpen MRI unitInterventional MRI unit
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Anatomical imagingBone and soft tissue
T2 weighted(torn ligaments)
rheumatoid arthritiswhrist
rheumatoid arthritisknee
T2 weighted(hernia)
Osteoporosis (femur)
But there is more to MRIthan anatomical imaging ...
First NMR images
19721972State of the art
3D images dynamic images
sharp image resolution
20082008
In research phase quantitative imaging
celspecific contrastagents hyperpolarized MRI in vivo spectroscopy functional imaging
multimodality imaging
I visited Copenhagen frequently after the war. At one point, I gave a talk in Copenhagen, and then afterwards we met with Bjerrum. Bjerrum was a chemist and a great friend of Niels Bohr Bohr said to him: You know, what these people do is really very clever. They put little spies into the molecules and send radio signals to them, and they have to radio back what they are seeing. I thought that was a very nice way of formulating it. That was exactly how they were used. It was not anymore the protons as such. But from the way they reacted,you wanted to know in what kind of environment they are, just
like spiesthat you send out. That was a nice formulation.- Felix Bloch -