Discovered Nuclear Magnetic Resonance (NMR) in 1946
Won the Nobel Prize of 1952 with Felix Bloch
Proposed that atomic nuclei behave like magnets
EDWARD PURCELL
Charged particles have magnetic fields
Led to the development of Nuclear Magnetic Resonance (NMR) spectrometers
Spectrometry – analysis of molecular configuration based on NMR spectrum
FELIX BLOCH
Nobel Prize winner of 1952, along with Edward Purcell
Proposed the Bloch Equations
Relationship between nuclear magnetization and relaxation times
RAYMOND DAMADIAN
Malignant tissue have different NMR parameters compared with normal tissue
First NMR image of a rat tumor in 1974
Built The Indomitable with his team in 1977
First scan took five hours to complete
PAUL LAUTERBUR
Expanded Herman Carr's idea of using magnetic gradients
Managed to obtain pictures that demonstrate the difference between regular water and heavy water (deuterium oxide)
PETER MANSFIELD
Improved upon Paul Lauterbur's technique by using Larmor Frequency and Fourier Transformation
Larmor Frequency - rate of spin wobble when placed in a magnetic field, directly proportional to magnetic field strength
Fourier Transformation - Mathematical technique to decompose an MRI signal, Interpolation that speeds up image formation
Credited with "slice selection" in MRI
The original name for MRI was Nuclear Magnetic Resonance Imaging, but the "nuclear" was removed because of the various negative connotations of the word.
BASICS OF MAGNETISM
Any charged particle in motion generates a magnetic field, hence "Electromagnetism"
The magnetic field exists in a 90-degree angle to the motion of the particle, hence "Fleming's Hand Rule"
DEFINING A MAGNET
Device that attracts iron and produces a magnetic field
SI unit of measurement – Tesla (T) or Gauss (G), 10,000 G = 1 T
Nikola Tesla – proponent of alternating current (AC)
Carl Friedrich Gauss – first to measure the magnetism of Earth using a magnetometer, Magnetometer – instrument that measures changes in the Earth's magnetic field
Magnetic dipole
Some elements form magnetic dipoles based on the spin of their nucleus and electrons, Dipole – means a magnet that has a north and south pole, The alignment of many magnetic dipoles result in a magnetic domain
Types of magnetism
Ferromagnetism
Paramagnetism
Diamagnetism
Ferromagnetism
Strong attraction, Can be permanently magnetized, "Alnico" alloy
Paramagnetism
Slight attraction to a magnet, Loosely influenced by magnetic fields, Contrast agents for MRI
Diamagnetism
Weakly repelled by magnetic fields, Pure water, plastic, Used in MRI shielding
Non-magnetic
Unaffected by magnetic fields, Wood, glass
Aspects of magnetism
Magnetic Intensity
Magnetic Permeability
Magnetic Susceptibility
Magnetic Intensity
Amount of magnetic flux in an area perpendicular to the direction of magnetic flow, Measurement of field "Strength"
Magnetic Permeability
Ability of a material to attract lines of magnetic field intensity, Characteristic of a material to "strengthen" or "weaken" a magnetic field
Magnetic Susceptibility
A measure of magnetic properties of a material, Determines whether a material can be affected by an external magnetic field
Types of magnets
Permanent
Resistive Magnet / Electromagnet
Superconducting Magnet
Permanent Magnet
Magnetized material that do not lose magnetism, Low field strength (0.064T – 0.3T), Usually has an open design (less claustrophobia), Low magnetic strength means longer scan time and less image quality
Resistive Magnet / Electromagnet
Magnetic field is generated by a current that passes through coiled wire, Either Air-Core or Iron-Core, Up to 0.3T, Generates a lot of heat, requires water-cooling, Open design, Can be switched off and on
Superconducting Magnets
Most common among MRI machines, Similar to a resistive magnet inside, except the metal is cooled to near absolute zero, making it a superconductor, Superconductivity – a property that some materials gain when reaching extremely low temperatures wherein their electric resistance becomes zero, Requires multiple vacuum shields to prevent heat from reaching the magnet
Cryogen
Cooling agent used to achieve superconductivity, Liquid helium can cool to 47 K, Liquid nitrogen can cool to 97 K, 0 K = -273 degrees Celsius or -459 degrees Fahrenheit
Dewer / Cryostat
Double-walled flask of metal with vacuum between walls, The inner chamber contains the cryogen, Similar to an Aquaflask / Hydroflask vacuum-insulated tumbler
Fringe Magnetic Field
Magnetic field outside of the patient aperture
Quenching
Rapid expulsion of liquid cryogen as gas
Humans contain a large amount of water, hence a lot of hydrogen.
Hydrogen has the highest gyromagnetic ratio (42.6 MHz / T)
The hydrogen nucleus functions as a magnetic dipole since it spins on its own axis
What happens when a person is put inside an MRI machine
1. The hydrogen atom precess at the Larmor Frequency
2. More hydrogen atoms are in the parallel configuration (low-energy) than in anti-parallel configurations (high energy)
3. There is a net magnetization (sum of all magnetic fields of each proton) pointing in the same direction as the MRI machine's magnetic field
4. All of these are part of the MRI Machine's initial phase – Magnetization
Excitation
1. The MRI machine performs a pre-scan to detect the frequency of the spinning protons (the Larmor Frequency)
2. The MRI machine then sends a radio frequency pulse that matches the frequency of the spinning protons
3. The protons that resonate with the frequency then change vectors and starts pointing away from Bo
4. This change in vector is called "flipping," hence there is a parameter in sequences called "flip angle," which can be anywhere from 0o to 180o
Relaxation Phase
1. The protons will keep the RF pulse they received for a time, putting them in a "high energy state"
2. Eventually the protons will revert back to a lower energy state, They do this by releasing the stored RF pulse along with some of it converted into heat
3. Eventually the net magnetization of the once-resonant protons return to point at Bo
4. This is what happens in T1 Relaxation, also called Spin-Lattice Relaxation or Longitudinal Relaxation
T2 Relaxation
After an excitation pulse, the protons begin to all spin towards the same direction, This is called being "in-phase"
As time passes and they lose energy, some protons start to spin in other directions, This is called "de-phasing"
Eventually with enough time, none of the protons spin in the same direction, Hence why T2 is called "spin-spin relaxation" or "transverse relaxation"
Acquisition
1. The RF signal released by the protons are picked up by the Receive Coil
2. It can only be done at 90o angles from Bo; otherwise, the current induced by Bo overwhelms the current produced by the RF signals from tissue
3. Signals are strong in the beginning, and quickly becomes weaker, This is called Free Induction Decay
Computing and Display
The received signal is fed into the computer and converted into images
Coils
Gradient Coils
Radiofrequency Coils
Gradient Coils
Uses resistive electromagnets, Creates additional magnetic fields and allows slice selection