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Goo Goo : MRI: Magnetic Resonance Imaging: is a way of seeing inside people and animals. How is this relevant to us?


Erasmus Profile Erasmus : Magnetic resonance imaging (MRI) uses the body's natural magnetic properties to produce detailed images from any part of the body.

For imaging purposes the hydrogen nucleus (a single proton) is used. It is abundant in water and fat in the human body. Also, Single protons are easier to flip magnetically than electrons.

Though electrons are a lot lighter they orbit much further from the nucleus (e.g. the proton of a hydrogen atom in water). So when we calculate momentum: Mass x Velocity (movement at a distance), protons have a much smaller Magnetic Dipole Moment than electrons. This means they are easier to flip: requiring less energy and less powerful magnetic fields to create alignment with the magnetic fields.

The hydrogen proton spins on its axis, with a north-south pole, perhaps akin to a bar magnet. Under normal circumstances, these hydrogen proton “bar magnets” spin in the body with their axes randomly aligned.
When the body is placed in a strong magnetic field, such as an MRI scanner, the protons' axes all line up. This uniform alignment creates a magnetic vector oriented along the axis of the MRI scanner.

MRI Scanner MRI Scanner

 

Kinkajou Profile Kinkajou : MRI scanners come in different field strengths, usually between 0.5 and 1.5 tesla. When additional energy (in the form of a radio wave) is added to the magnetic field, the magnetic vector is deflected. The radio wave frequency (RF) that causes the hydrogen nuclei to resonate is dependent on the element sought (hydrogen in this case) and the strength of the magnetic field.

 


Erasmus Profile Erasmus : The RF frequency required is called the Lamor Frequency and can be calculated using:

W = YB. Where W is the Larmor frequency in MHz, Y is the gyromagnetic ratio in MHz/tesla and B is the strength of the static magnetic field in tesla.
Note that the gyromagnetic ratio is defined in different ways by different authors. In this case a useful, simplified version is shown representing the Armor frequency when B0=1.

Erasmus Profile Erasmus : Follow the Link to see how the variables affect the RF Frequency required to spin Protons. Link

* The gyromagnetic ratio (MHz/T) for a few commonly measured or imaged isotopes are :
o H-1                   42.58
o F-19                 40.05
o Na-23               11.26

Larmour Frequency Calculator for
Various Nuclei in Nuclear Magnetic Resonance
 
Nucleus:
1H
2H
3He
7Li
13C 14N 15N 17O
23Na 31P 129Xe  
Magnet Field Strength:  (T)
Theoretical Gyromagnetic Ratio:                  0 [MHz/T]
Actual Gyromagnetic Ratio:                  0 [MHz/T]
Theoretical Larmour Frequency:                  0 [MHz]
Actual Larmour Frequency:                  0 [MHz]

Link

Calculations are for a uniform magnetic field at the given strength.
Data for actual numbers obtained from:
-M A Bernstein, K F King and X J Zhou (2004). Handbook of MRI Pulse Sequences. San Diego: Elsevier Academic Press. p. 960. ISBN 0-1209-2861-2.
-R C Weast, M J Astle, ed (1982). Handbook of Chemistry and Physics. Boca Raton: CRC Press. p. E66. ISBN 0-8493-0463-6.

 

Erasmus Profile Erasmus : Specific Quantised energy levels for RF must be attained to align the protons in the magnetic field.

The strength of the magnetic field can be altered electronically from head to toe using a series of gradient electric coils, and, by altering the local magnetic field by these small increments, different slices of the body will resonate as different frequencies are applied.

When the radiofrequency source is switched off the magnetic vector returns to its resting state, and this causes a signal (also a radio wave) to be emitted. It is this signal which is used to create the MR images. Receiver coils are used around the body part in question to act as aerials to improve the detection of the emitted signal. The intensity of the received signal is then plotted on a grey scale and cross sectional images are built up.

Multiple transmitted radiofrequency pulses can be used in sequence to emphasise particular tissues or abnormalities. A different emphasis occurs because different tissues relax at different rates when the transmitted radiofrequency pulse is switched off.

The time taken for the protons to fully relax is measured in two ways. The first is the time taken for the magnetic vector to return to its resting state and the second is the time needed for the axial spin to return to its resting state. The first is called T1 relaxation; the second is called T2 relaxation.

Kinkajou Profile Kinkajou : Pacemakers, metal clips, and metal valves can be dangerous in MRI scanners because of potential movement within a magnetic field. Metal joint prostheses are less of a problem, although there may be some distortion of the image close to the metal. MRI departments always check for implanted metal and can advise on their safety.

Proton Resonance


Kinkajou Profile Kinkajou : The hydrogen proton can be likened to the planet earth, spinning on its axis, with a north-south pole. In this respect it behaves like a small bar magnet. Under normal circumstances, these hydrogen proton “bar magnets” spin in the body with their axes randomly aligned.


When the body is placed in a strong magnetic field, such as an MRI scanner, the protons' axes all line up. This uniform alignment creates a magnetic vector oriented along the axis of the MRI scanner.

 

Kinkajou Profile Kinkajou :
Why are electrons not influenced when the magnetic field is applied (in NMR)?


Erasmus Profile Erasmus : The electron is not affected by NMR because the magnetic dipole moment of the electron is by far greater than a proton (x658 stronger), due to the greater mass of the proton (x1836)  but especially the much smaller effective size of the proton.

In electron spin resonance experiments the electron is affected by the magnetic field, a phenomenon called Zeeman splitting.


Kinkajou Profile Kinkajou : Tell about the Zeeman Effect in Hydrogen
Erasmus Profile Erasmus : When an external magnetic field is applied, sharp spectral lines like the n=3 > 2 transition of hydrogen split into multiple closely spaced lines. This splitting is attributed to the interaction between the magnetic field and the magnetic dipole moment associated with the orbital angular momentum. In the absence of the magnetic field, the hydrogen energies depend only upon the principal quantum number n, and the emissions occur at a single wavelength.

 

 

 

 

 

 

 

 

Erasmus