Upload
milo-lindsey
View
214
Download
1
Tags:
Embed Size (px)
Citation preview
A brief introduction to MR physicsA brief introduction to MR physics
Hydrogen/Proton: Hydrogen/Proton: A spinning topA spinning top
= = JJ
With and without the presence of an external With and without the presence of an external magnetic field (magnetic field (BB00)) in the z directionin the z direction
MM00
BB00zz
Randomly oriented hydrogenRandomly oriented hydrogenatoms (spins) in absence of anatoms (spins) in absence of anexternal magnetic fieldexternal magnetic field
The protons aligns with the external The protons aligns with the external field: Low field: 0.47 T, Clinical field: Low field: 0.47 T, Clinical fields: fields: BB00 = 1.5 – 3.0 T = 1.5 – 3.0 T
Together they create a macroscopicTogether they create a macroscopicmagnetic magnetic MM00 vector parallel with vector parallel with BB00
(and z)(and z)
Radio Frequency (RF) coils in the xy-plane (Radio Frequency (RF) coils in the xy-plane (BB11))
A 900 pulse flips M0 into
the xy-plane M0 aligns with the z-axis
BB11
RF on
An oscillating FID signal in the xy-plane (readout plane)An oscillating FID signal in the xy-plane (readout plane)
When the protons aligns with the external field again they When the protons aligns with the external field again they give up their energy to their surroundings. This signal is give up their energy to their surroundings. This signal is registered by a coil (like an antenna):registered by a coil (like an antenna):
RF off:RF off:The spins The spins relax back relax back to their to their equilibrium equilibrium state (along z)state (along z)
TT11 relaxation: relaxation:
The time it takes for The time it takes for MM00 to realign to realign
with with BB0 0 after the influence of after the influence of
an RF pulse. Dependent of the an RF pulse. Dependent of the exchange with the media. exchange with the media. TT1 1 is is
short for fat and long for watershort for fat and long for water
TT22 relaxation: relaxation:
The time it takes before the spinsThe time it takes before the spins(protons) reach equilibrium after (protons) reach equilibrium after spin-spin exchange and thereafter spin-spin exchange and thereafter dephasing in the xy-plane:dephasing in the xy-plane:TT22 TT1 1
The MR signal
• Intrinsic parameters: T1, T2, n(H)
• Instrument parameters: TR, TE
• Pulse sequences: vary TR and TE
• Contrast agents: manipulate T1 and T2
Contrast Agents (CA)
• Even though MR has high specificity, CA are often used to better visualize specific structures and pathology
• Indirect effect on hydrogen spins. The relaxation times (T1 and T2) are reduced, thus signal changes
• Either T1 or T2 CA’s, where T1 CA’s increase the signal and gives “positive” contrast, whereas T2 CA’s reduces the signal and gives “negative” contrast in the image
Different CA’s (exogenous)
Paramagnetic
• Positive contrast: n(H) increases, T1 reduces and T2 increases
• Much stronger T1 than T2 reducing effect, which in total gives an improved T1 contrast by the addition of paramagnetic agents
• T1-weighted images
• Some paramagnetic ions: Gd3+, Mn2+
Electron spin:• Non-paired electrons
MnMn2+2+11HH
ParamagneticParamagneticionion
• A magnetic moment analogous to the A magnetic moment analogous to the magnetic moment of protonsmagnetic moment of protons
• The magnetic moment of an electron ~600 times The magnetic moment of an electron ~600 times stronger than the magnetic moment of protons, and stronger than the magnetic moment of protons, and will therefore have an influence on themwill therefore have an influence on them
• Change the magnetic environment of the Change the magnetic environment of the protons, where Tprotons, where T11 and T and T22 will be reduced will be reduced
Efficacy in a homogenous solution
Relaxivity r1 and r2:
• The measured effectiveness of an CA to reduce T1 and T2
• Given in (s mM)-1
A simple linear formula:
T1 -1with CA = T1
-1without CA + r1 • [CA]
TT11 relaxation relaxation – – shorter and shorter Tshorter and shorter T1 1 (CA) (CA)
stronger and stronger signal in a Tstronger and stronger signal in a T1 1 weighted image where weighted image where
the CA is presentthe CA is present
Different types• Free metal ions are toxic in large quantities, that is why
they are bound to a chelate. This “shielding” influence the effectiveness of the CA, and safety is competing with efficacy
• Few side effects; does not result in severe allergic reactions as with X-ray CA’s
Extracellular (infarction, pathology)• Gd-DTPA (Magnevist*)Liver CA (pathology)• MnDPDP (Teslascan**)Intravascular/E.C. (few protons < 5% of all the tissue
protons). Large complexes which are trapped in the blood pool
• Gd-DTPA-BMA (Omniscan**)
Small moleculesSmall molecules
*Schering,**Amersham Health/GE Healthcare
Water Exchange Theory
H2OicH2Oic
t ec-1
t ic-1
ec: Extracellular
ic: Intracellular
Pic T1ic
Pec T1ec
Intrinsic values
A relaxivity in each ”homogenous” water compartment
Intracellular relaxivity: rIntracellular relaxivity: r1ic1ic
Monoexponential decayMonoexponential decayInversion Recovery pulse sequence:Inversion Recovery pulse sequence:
MMzz(t) = (t) = MM00 ( 1 - 2e ( 1 - 2e-t/-t/T1T1 ) )
T1-1
FAST EXCHANGE
1T’1ic
=1
T1ic
+1ic
1T’1ec
=1
T’1ec
+1ec
The apparent biexponential The apparent biexponential TT11’s are sums ’s are sums
of the intrinsic relaxation rates and of the intrinsic relaxation rates and the water exchange in each compartment:the water exchange in each compartment:
T’1ec
T’1ic
p’ic
p’ec
SLOW EXCHANGE: Apparent values
MMzz = = pp’’icic ( 1 - 2e ( 1 - 2e-t/-t/T1’icT1’ic ) + ) + pp’’ecec ( 1 - 2e ( 1 - 2e-t/-t/T1’ecT1’ec )) ))
Biexponential signal:Biexponential signal:
1/1/ = (PA)/V = (PA)/V
Intermediate exchange
2 SX equation for R1ic
2 SX equation for R1ec
2 SX equation for pic and pec
Calculating relaxivities, lifetimes of water and population fractions
EKSTRASTOFFEKSTRASTOFF
c (s)
temp
nonviscousliquids
viscousliquids Solids
R2
R1
1/T1M ,
1/T2M
SOLOMON-BLOEMBERGEN dipole-dipole term
20 MHz
60 MHz
100 MHz
10-11 10-7
CAec + 1H20ec
1H20ic
1H20*CAec
m-1
ic-1
ec-1
1H20*CAp CAp
1H20p
+
1H20ic
m-1
ic-1
p-1
Vessel wall
Interstitium
Intracellular
Ext
race
llula
r
Plasma
IntravascularE.C. Contrast Agent
Conclusions• Multi-component analyses of T1 and T2
revealed two compartments with different chemical environments in the heart cells detectable with 0.47 T MR
• Two compartment model more suitable for T1 analysis
• Close correlation between tissue Mn content and T1relaxation
• Slow water exchange in excised cardiac tissue
• Remarkably high relaxivity of intracellular Mn2+ ions
Main findings
MnCl2 Mn/Ca-100
-50
0
50
100
L
VD
P (
%)
-53
59
MnCl2 Mn/Ca0
1000
2000
3000
4000 3720
1620
Tis
sue
Mn
co
nte
nt
(nm
ol/
g d
ry w
t.)
Physiology and Mn contentPhysiology and Mn content
-100
-50
0
50
100
0
250
500
-70
-18 -9
468
269189
0.30 1.25 3.00 Ca2+ (mM):
LV
DP
(%
)
Mn
co
nte
nt
( n
mo
l/g
dry
wt.
)
25 µM MnCl2
-100
-50
0
50
100
0
500
1000
Ca2+ (mM): 0.30 1.25 3.00
-87-52 -52
574 556 692
LV
DP
(%
)
Mn
co
nte
nt
( n
mo
l/g
dry
wt.
)
100 µM MnCl2