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Magnetic Resonance Imaging

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Title: Magnetic Resonance Imaging


1
Magnetic Resonance Imaging
  • Basic Principles
  • V.G.Wimalasena Principal
  • School of Radiography

2
Introduction
Modern 3 Tesla MRI unit
Bore of the magnet
RF Coil (for head)
Main magnet body
Patient Couch
3
What is MRI?
  • Magnetic resonance imaging (MRI), or nuclear
    magnetic resonance imaging (NMRI), is primarily a
    Medical Imaging technique most commonly used in
    radiology to visualize the structure and function
    of the body.
  • It provides detailed images of the body in any
    plane.

4
MRI Vs CT
  • MRI provides much greater contrast between the
    different soft tissues of the body than CT does,
    making it especially useful in neurological
    (brain), musculoskeletal, cardiovascular, and
    oncological (cancer) imaging.
  • Unlike CT, it uses no ionizing radiation, but
    uses a powerful magnetic field to align the
    nuclear magnetization of (usually) hydrogen atoms
    in water in the body.

5
Uses RF fields
  • Radiofrequency fields are used to systematically
    alter the alignment of the nuclear magnetization
    of Hydrogen atoms, causing the hydrogen nuclei to
    produce a rotating magnetic field detectable by
    the scanner.
  • This signal can be manipulated by additional
    magnetic fields to build up enough information to
    construct an image of the body.

6
History
  • MRI is a relatively new technology, which has
    been in use for little more than 30 years
    (compared with over 110 years for X-ray
    radiography).
  • The first MR Image was published in 1973 and the
    first study performed on a human took place on
    July 3, 1977.
  • Magnetic resonance imaging was developed from
    knowledge gained in the study of nuclear magnetic
    resonance

7
Brief lay explanation of MRI physics
  • The body is mainly composed of water molecules
    which each contain two hydrogen nuclei or
    protons.
  • When a person goes inside the powerful magnetic
    field of the scanner these protons align with the
    direction of the field.

8
  • A second radiofrequency electromagnetic field is
    then briefly turned on causing the protons to
    absorb some of its energy.
  • When this field is turned off the protons release
    this energy at a radiofrequency which can be
    detected by the scanner.

9
  • The position of protons in the body can be
    determined by applying additional magnetic fields
    during the scan which allows an image of the body
    to be built up.
  • These are created by turning gradients coils on
    and off which creates the knocking sounds heard
    during an MR scan.

10
  • Diseased tissue, such as tumors, can be detected
    because the protons in different tissues return
    to their equilibrium state at different rates.
  • By changing the parameters on the scanner this
    effect is used to create contrast between
    different types of body tissue.

11
Use of contrast agents
  • Contrast agents may be injected intravenously to
    enhance the appearance of blood vessels, tumours
    or inflammation.
  • Contrast agents may also be directly injected
    into a joint, in the case of arthrograms, MR
    images of joints.

12
Safety precaution
  • Unlike CT scanning MRI uses no ionizing radiation
    and is generally a very safe procedure.
  • But Patients with some metal implants, cochlear
    implants, and cardiac pacemakers are prevented
    from having an MRI scan due to effects of the
    strong magnetic field and powerful radiofrequency
    pulses.

13
Uses of MRI
  • MRI is used to image every part of the body,
  • But is particularly useful in
  • neurological conditions,
  • disorders of the muscles and joints,
  • for evaluating tumors and
  • showing abnormalities in the heart and blood
    vessels.

14
System components
Magnet power supply
Gradient amplifiers
Shim power supply
RF transmitter
Operator consol
Magnet coils
Shim coils
Host computer
Gradient coils
RF coils
Magnet bore
Image processor
Image disk
RF receiver
Digitizer
15
Explaining Basic principles
  • This is an Integration of Two ways of explaining.
    i. e
  • Classically
  • Via quantum physics
  • It describes
  • Properties of atoms
  • Their interaction with magnetic fields

16
Atomic structure
  • Central nucleus orbiting electrons
  • Nucleus
  • Nucleons
  • (Protons neutrons)
  • Atomic number
  • Mass number
  • Electrically stable

17
Motion within the atom
  • There are three types of motion within an atom
  • Electrons spinning on their own axis
  • Electrons orbiting the nucleus
  • The nucleus spinning about its own axis

18
  • The principles of MRI rely on the spinning motion
    of specific nuclei present in biological tissues
  • These are called (MR active nuclei)

19
MR active nuclei ?
  • MR active nuclei are Characterized by their
    tendency to align their axis of rotation to an
    applied magnetic field
  • Due to the laws of electromagnetic induction,
    nuclei that have a net charge and are spinning
    acquire a magnetic moment and are able to align
    with an external magnetic field

20
MR active nuclei continued..
  • Important Examples
  • Hydrogen 1
  • Carbon 13
  • Nitrogen 15
  • Oxygen 17
  • Fluorine 19
  • Sodium 23
  • Phosphorus 31
  • The nuclei with odd mass numbers undergoes this
    interaction
  • The result of this interaction is angular
    momentum or spin

21
The magnetic moment alignment
  • The alignment of the magnetic moment is measured
    as the total of the nuclear magnetic moments and
    is expressed as a vector sum
  • The strength of the total magnetic moment is
    specific to every nucleus and determines the
    sensitivity to magnetic resonance

22
The hydrogen nucleus
  • The hydrogen nucleus is the MR active nucleus
    used in clinical MRI
  • Very abundant in the body
  • Solitary proton gives a relatively large magnetic
    moment

23
The hydrogen nucleus as a magnet
  • The nucleus contains one positively charged
    proton that spins
  • The spin of the proton induces a magnetic field
    around it and acts as a small magnet

N
N
S
S
24
The magnetic vector
  • The magnetic moment of each nucleus has vector
    properties.
  • i.e. it has size and direction and is denoted by
    an arrow

size
direction
25
Alignment of the magnetic moments
  • In the absence of an applied magnetic field the
    magnetic moments are randomly oriented
  • When placed in a strong external magnetic field
    the magnetic moments of the hydrogen nuclei align
    with this magnetic field , parallel or
    anti-parallel (as shown in next slide)

26
Alignment of the magnetic moments
Parallel
Anti-parallel
Random alignment in the absence of external
magnetic field
Alignment
External magnetic field
27
The state of alignment
  • Quantum physics describes that the hydrogen
    nuclei only possesses two energy states or
    populations low high
  • Low energy nuclei align their magnetic moments
    parallel to the external magnetic field
  • High energy nuclei align their magnetic moments
    anti-parallel to the external magnetic field

28
Energy levels field strength
Low energy population
Energy difference depends on field strength
high energy population
29
Energy levels alignments
  • The energy level and the number of nuclei aligned
    in each direction is determined by the strength
    of the external magnetic field and the thermal
    energy level of the nuclei
  • Low thermal energy nuclei do not have enough
    energy to oppose the field and align parallel
  • High thermal energy nuclei have sufficient energy
    to oppose and may align anti-parallel

30
Alignment field strength
  • Thermal energy depends on the body temperature
  • The main deciding factor to increase the number
    of parallel alignments is the high field strength
    of the external magnetic field
  • At thermal equilibrium the parallel population is
    higher than the anti-parallel population
  • Therefore there is a net magnetic moment parallel
    to the external magnetic field

31
The net magnetization vector
B0
Net Magnetization Vector (NMV)
32
Summary
  • The magnetic moment (of hydrogen in this case) is
    called the Net Magnetization Vector (NMV)
  • The static external magnetic field is called B0
  • The interaction of the NMV with B0 is the basis
    of MRI
  • The unit of B0 is Tesla or Gauss.
  • 1 Tesla (T) 10000 Gauss (G)

33
Summary continued
  • When a patient is placed in the bore of the
    magnet the hydrogen nuclei within the patient
    align parallel and anti-parallel to B0.
  • A small excess of hydrogen nuclei line up
    parallel to B0 and constitute the NMV of the
    patient.
  • The energy difference between the two populations
    increases as B0 increases.
  • The magnitude of NMV is larger at high field
    strengths(B0 )

34
Precession
  • Each hydrogen nucleus that makes up the NMV is
    spinning on its own axis
  • The influence of B0 produce an additional spin or
    wobble
  • This path is called the precessional path and the
    speed at which the NMV wobbles around B0 is
    called the precessional frequency

Precessional path
B0
Magnetic moment of the nucleus
Precession
Hydrogen nucleus
35
Precession continued.
  • Two populations
  • High energy nuclei spin down
  • Low energy nuclei spin up
  • Their magnetic moments precess on a circular path
    around B0 as shown

Spin up nuclei
B0
Precession
Spin down nuclei
36
The Larmor equation
  • The value of the precessional frequency is
    governed by the Larmor equation i.e
  • The precessional frequency (?0) Magnetic field
    strength(B0) x Gyro-magnetic ratio(?)
  • ? 0 B0 x ?
  • Gyro-magnetic ratio is a constant for a specific
    MR active nucleus and is expressed as the
    precssional frequency at 1.0 tesla. The unit is
    MHz / T

37
Precessional frequencies of Hydrogen
? B0 ?
1.5 T 63.86 MHz
42.57 Mhz/T 1.0 T 42.57 MHz
0.5 T 21.28 MHz
38
Resonance
  • Resonance is a phenomenon that occurs when an
    object is exposed to an oscillating perturbation
    that has a frequency close to its own natural
    frequency of oscillation.
  • At resonance the object can absorb energy from
    the external source
  • Therefore Exchange of energy between two systems
    at a specific frequency is called resonance.

39
Nuclear Resonance
  • When a nucleus is exposed to an external
    perturbation that has an oscillation similar to
    its own natural frequency, the nucleus gains
    energy from the external force.
  • The nucleus gains energy and resonates if the
    energy is delivered at exactly its precessional
    frequency.

40
RF signal Nuclear magnetic Resonance
  • Energy at the precessional frequency of hydrogen
    at all field strengths in clinical MRI
    corresponds to the radio frequency (RF) band of
    the electromagnetic spectrum
  • For resonance of hydrogen to occur, an RF pulse
    of energy at exactly the Larmor frequency of the
    hydrogen NMV must be applied
  • Other MR active nuclei that have aligned with B0
    do not resonate because their precessional
    frequencies are different to that of hydrogen

41
Excitation RF frequency
  • The application of an RF pulse that causes
    resonance to occur is termed excitation.
  • The absorption of energy causes an increase in
    the number of spin down hydrogen nuclei
    populations as some of the spin up nuclei gain
    energy via resonance and become high energy
    nuclei (next slide)
  • The energy difference corresponds to the energy
    required to produce resonance via excitation

42
Energy transfer during excitation
Low energy population
Some nuclei gain energy to join the high energy
population
High energy population
43
The results of resonance
  • The first result is the NMV moves out of
    alignment away from B0
  • The angle to which the NMV moves out of alignment
    is called the flip angle
  • The magnitude of the flip angle depends upon the
    amplitude and duration of RF pulse
  • Usually the flip angle is 900 (see next slide).
    The transverse NMV rotates at the Larmor frequency

44
The flip angle Transverse plane
  • B0 is now termed the longitudinal plane
  • The plane at 900 to B0 is termed the transverse
    plane

Longitudinal plane
Longitudinal plane
B0
NMV
Flip angle
Flip angle 900
NMV
Transverse plane
Transverse plane
45
In phase / out of phase
  • The second result of resonance is that the
    magnetic moments within the transverse NMV move
    into phase with each other
  • Phase is the position of each magnetic moment on
    the precessional path around B0
  • Magnetic moments that are in phase are in the
    same place on the precessional path around B0 at
    any given time
  • MM that are out of phase are not in the same
    place on the precessional path

46
Phase of magnetic moments around the precessional
path
Out of phase
In phase
47
Summary
  • For resonance of hydrogen to occur, RF at exactly
    the Larmor frequency of hydrogen must be applied
  • The result of resonance is an NMV in the
    transverse plane that is in phase
  • This NMV precesses in the transverse plane at the
    Larmor frequency

48
The MR signal
  • Formation of MR signal after removal of RF pulse

49
The MR signal
  • As a result of resonance the NMV is precessing in
    phase in the transverse plane.
  • According to Faradays laws of induction,
  • When a receiver coil (a conductive loop) is
    placed in the area of moving magnetic field a
    voltage is induced in it.
  • This Signal is produced when coherent (in phase)
    magnetization cut across the coil.

50
MR signal continued.
  • Therefore the moving NMV produces magnetic field
    fluctuations inside the coil
  • As the NMV precesses at the Larmor frequency in
    the transverse plane a voltage is induced in the
    coil.
  • This voltage constitutes the MR signal

51
  • The frequency of the MR signal is the same as the
    Larmor frequency
  • The magnitude of the MR signal depends on the
    amount of magnetization present in the transverse
    plane

52
Generation of the MR signal in the receiver coil
B0
Precession of NMV
Receiver coil
NMV
53
Relaxation The free induction decay signal
  • Switching off RF pulse
  • Relaxation
  • Recovery decay
  • FID

54
Relaxation
  • When the RF pulse is turned off the NMV is again
    influenced by B0 , and, it tries to realign with
    it.
  • To do that it must lose the energy given to it by
    the RF pulse.
  • The process by which the NMV loses energy is
    called relaxation

55
Recovery Decay
  • As relaxation occurs the NMV returns to align
    with B0
  • When this happens,
  • The amount of magnetization in the longitudinal
    plane gradually increases this is called
    recovery
  • The amount of magnetization in the transverse
    plane gradually decreases this is called decay

56
The free induction decay signal
  • As the magnitude of transverse magnetization
    decreases so does the voltage induced in the
    receiver coil.
  • The induction of this reduced signal is called
    the free induction decay (FID) signal

57
Result of relaxation
  • During relaxation
  • The NMV gives up absorbed energy and returns to
    B0
  • The magnetic moments of the NMV lose the
    transverse magnetization due to dephasing

Looking down on to transverse plane
In phase
Dephasing
Out of phase
58
T1 Recovery T2 Decay
  • Relaxation results in
  • recovery of magnetization in the longitudinal
    plane
  • and
  • decay of magnetization in the transverse
    plane.
  • The recovery of longitudinal magnetization is
    caused by a process called T1 recovery
  • The decay of transverse magnetization is caused
    by a process called T2 decay

59
T1 Recovery
  • T1 recovery is caused by the nuclei giving up
    their energy to the surrounding environment or
    lattice and it is often termed spin - lattice
    relaxation
  • The rate of recovery is an exponential process
    with a recovery time constant called T1

60
Recovery time constant -T1
  • T1 is the time it takes 63 of the longitudinal
    magnetization to recover in the tissue

100
63
Signal intensity
T1
Time
61
T2 decay
  • This is caused by nuclei exchanging energy with
    neighbouring nuclei.
  • The energy exchange is caused by the magnetic
    fields of each nucleus interacting with its
    neighbour.
  • It is often termed spin-spin relaxation results
    in a decay or loss of transverse magnetization
  • The rate of decay is also an exponential process
    so that the T2 relaxation time is its time
    constant of decay

62
Time constant of decay T2
100
  • T2 is the time it takes 63 of the transverse
    magnetization to be lost

Signal intensity
37
T2
Time
63
Dephasing of the FID
  • A signal or voltage is only induced in the
    receiver coil if there is magnetization in the
    transverse plane that is in phase

Dephasing (T2)
Signal (FID)
64
Pulse timing parameters
  • The magnitude and timing of the RF pulses form
    the basis of MRI and are discussed in Next lesson
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