W10 Flashcards

(111 cards)

1
Q

magnetic predisposition of a substance -

A

ability of external magnetic fields to affect the nuclei of a particular atom; it is related to the electron configurations of that atom:
- if nucleus is surrounded by paired electrons, it is protected and less affected
- if nucleus is surrounded by unpaired electrons, external magnetic fields can significantly affect it

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

three types of magnetic predisposition

A
  • paramagnetism
  • diamagnetism
  • ferromagnetism
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

PARAMAGNETISM

A

Paramagnetic substances contain unpaired electrons within the atom, they y have a small magnetic field about themselves = magnetic moment. Paramagnetic substances add to (increase) the applied magnetic field.

NO EXTERNAL MAGNETIC FIELD: magnetic moments occur in a random pattern and cancel each other out

PRESENCE OF EXTERNAL MAGNETIC FIELD: paramagnetic substances align with the direction of the field => magnetic moments add together => paramagnetic substances affect external magnetic fields in a positive way: cause a local increase in the magnetic field

Ex: molecular O2

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

DIAMAGNETISM

A

Diamagnetic substances contain paired electrons within the atom. Diamagnetic substances slightly oppose (decrease) the applied magnetic field.

NO EXTERNAL MAGNETIC FIELD: diamagnetic substances show no net magnetic moment

PRESENCE OF EXTERNAL MAGNETIC FIELD: diamagnetic substances show a small magnetic moment that opposes the applied field => substances of this type are repelled by the magnetic field

Ex: water, fat, calcium and most biological tissue

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

FERROMAGNETISM

A

Ferromagnetic substances: remain magnetic, are permanently magnetized and become permanent magnets. Ferromagnetic substances are strongly attracted to, and align with, the applied magnetic field.

PRESENCE OF EXTERNAL MAGNETIC FIELD: strong attraction and alignment, even after the field has been removed => NO EXTERNAL MAGNETIC FIELD: magnetism is present

Ex: iron

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

Magnets’ properties:

A

bipolar as they have two poles (north and south) => magnetic field exerted by them produces magnetic field lines or lines of force, which run from the magnetic north to the south poles of the magnet = magnetic lines of flux

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

magnetic flux density

A

number of lines of force that run from N to S poles of a magnet per unit area

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

strength of the magnetic field, is measured in (3):

A
  • gauss (G)
  • kilogauss (kG)
  • tesla (T)
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

Magnetism summary:

A
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

Magnetic fields are generated by

A

moving charges (electrical current) => changing magnetic fields generate electric currents

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Induced electric current:

A

When a magnet is moved in and out of a closed circuit, a current is produced => This ceases the moment the magnet stops moving

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

basic physical phenomenon of MRI -

A

electromagnetic induction, which is specifically involved in:
* spinning charge of a hydrogen proton which causes a magnetic field to be induced around it
* movement of the net magnetization vector (NMV) across the area of a receiver coil inducing an electrical charge in the coil

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

Three types of magnets are used in clinical MRI machines:

A
  • Permanent
  • Electromagnets
  • Superconducting
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

Permanent magnets:

A

consist of ferromagnetic substances, most commonly used material - alloy of aluminium (Al), nickel (Ni) and cobalt (Co), known as Alnico.

ADVANTAGES:
- have open design
- require no power supply => low operating costs
- have a vertical magnetic field => keep the magnetic field virtually confined within the boundaries of the scan room

DISADVANTAGES:
- excessively heavy
- have low fixed field strengths (0.2 to 0.7 T)
- have low SNR and resolution
- need long scan times.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

Electromagnets

A

utilize the laws of electromagnetic induction: electric current passes through a series of wires to produce a magnetic field;
- its strength is dependent upon the current that passes through its coils of wire
- direction of the main magnetic field follows the righthand thumb rule => electromagnetic field produces lines of flux running horizontally from the head to the foot of the magnet

ADVANTAGES:
- are lighter in weight than permanent magnets
- have a low Capital cost
- easy to install
- easy to turn on and off inexpensively

DISADVANTAGES:
- high Operational cost due to enormous power requirements
- maximum field strength is less than 0.3 T
- scan times are larger than permanent magnets
- have low SNR and resolution

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Superconductive MRI magnets

A

use a solenoidshaped coil made of alloys such as niobium/titanium or niobium/tin surrounded by copper, b/c such alloys have the property of zero resistance to electrical current when cooled down to about 10 kelvin (coil is kept below this T w/ Heliq).
current is passed through loops of wire (Niobium-Titanium alloy) to create the magnetic field or bring the field up to strength => wires are super cooled with cryogens (liquid Helium and Nitrogen) to eliminate resistance

ADVANTAGES:
- give high magnetic field strengths with low power requirements
- have low Operating costs
- can accommodate advanced applications
- can obtain optimum image quality

DISADVANTAGES:
- high Capital cost
- need RF shielding
- a tunnel design unsuitable for large or claustrophobic patients

the most common type of magnet used in clinical MRI

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
17
Q

shimming -

A

correction of inhomogeneities in the main magnetic field (since due to design limitations, it is almost impossible to create an electromagnet with coils of wire that are spaced evenly), performed by placing another loop of current‐carrying wire (shim coil) in the area of the inhomogeneity => compensates for the inhomogeneity in the main magnetic field and creates magnetic field homogeneity or evenness

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
18
Q

three types of motion of particles in the atom and how it is related to MRI:

A
  1. Negatively charged electrons spinning on their own axis.
  2. Negatively charged electrons orbiting the nucleus.
  3. Particles within the nucleus spinning on their own axes.

each of these produces a magnetic field

In MRI, the motion of particles within the nucleus and the nucleus itself is of importance:
- protons and neutrons spin about their own axes within the nucleus;
- if a nucleus has an even mass number the spins cancel each other, and the nucleus has no net spin
- if a nucleus has an odd mass number, the spins do not cancel each other out and the nucleus spins, such nucleus also has a net spin

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
19
Q

MR active nuclei:

A

Nuclei with an odd number of protons are said to be MR active

moving unbalanced charge induces a magnetic field around itself, direction and size of the magnetic field is denoted by a magnetic moment or arrow; total magnetic moment of the nucleus is the vector sum of all the magnetic moments of protons in the nucleus; length of the arrow = magnitude of the magnetic moment, direction of the arrow = direction of alignment of the magnetic moment

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
20
Q

which MR active nucleus used in MRI and why?

A

hydrogen 1, b/c:
* it is abundant in the human body (e.g., in fat and water);
* its solitary proton gives it a large magnetic moment.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
21
Q

alignment:

A

When MR active nuclei are placed in an external magnetic field their magnetic moments line up with the magnetic field flux lines (parallel (more in room T) or anti-parallel).

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
22
Q

NMV -

A

net magnetization vector = net magnetism of the patient, it reflects the balance between parallel and antiparallel magnetic moments and in room T is aligned parallel to the main field

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
23
Q

two energy states / populatons of H nuclei, according to quantum physics:

A
  • 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.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
24
Q

Resonance -

A

energy transition that occurs when an object is subjected to a frequency the same as its own

In MR, resonance is induced by applying a radiofrequency (RF) pulse:
- at the same frequency as the precessing hydrogen nuclei
- at 90° to B0
=> hydrogen nuclei to resonate whereas other MR active nuclei do not => energy absorption, phase coherence (magnetic moments of the nuclei move into phase with each other => net effect is of precession => NMV precesses in the transverse plane at the Larmor frequency) happen

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
25
free induction decay (FID)
**free** because of the absence of the RF pulse and **induction decay** because of the decay of the induced signal in the receiver coil
26
image has contrast if there are
areas of high signal as well as areas of low signal
27
e NMV can be separated into the individual vectors of the tissues present in the patient, such as:
for ex: *fat, cerebro-spinal fluid (CSF), muscle* **high signal** (***white***) = large transverse component of magnetization **intermediate signal** (***grey***) = medium transverse component of magnetization **low signal (*black*)** =small transverse component of magnetization
28
Image contrast is controlled by contrast parameters **controlled by the system operator**: (6)
**Repetition time (TR)** - time from the application of one RF pulse to the application of the next **Echo time (TE)** - time between RF excitation pulse and signal collection **Flip angle** - angle through which the NMV is moved due to RF excitation. **Turbo-factor (TF)** or **echo train length (ETL)** - number of 180° RF pulses and resultant echoes. **Time from inversion (TI)**: used on inversion recovery sequences. **b value**: used in diffusion weighted imaging.
29
parameters **inherent to the tissue which affect contrast and are not operator controlled**: (5)
* T1 recovery (relaxation process, where nuclei emit E absorbed from the RF puse through spin lattice energy transfer). * T2 decay (cumulative dephasing of spin‐spin interactions and inhomogeneities). * Proton density (PD). * Flow. * Apparent diffusion coefficient (ADC)
30
NMV in the transverse plane decreases due to:
* relaxation processes * field inhomogeneities * susceptibility effects.
31
T1 recovery causes
**recovery** of the **longitudinal** magnetization
32
T2 decay causes
**decay** of **transverse** magnetization
33
spins alligned in the anti-parallel direction are said to be in which E state?
High
34
the net magnetic vector NMV is made up of
the magnetic moments of just the excess number of parallel spins
35
resonance occurs when 2 objects do what?
both oscillate at the same frequency
36
Frequency in MRI refers to
how fast the magnetic moments of spins are precessing and is measured in MHz
37
Phase in MRI refers to
the position of a magnetic moment of a spin on its precessional path at any moment in time
38
At rest the magnetic moments of the spins are OUT of/IN phase with each other
At rest the magnetic moments of the spins are **out of phase with each other**.
39
The application of RF energy at the Larmor frequency causes
a net absorption of energy (***excitation***), and also changes the balance between the number of spins in the low‐ and high‐energy populations => orientation of the NMV to B0 depends on this balance
40
T1 RECOVERY | caused by, description of the process
- caused by the exchange of energy from nuclei to their surrounding environment or lattice (= ***spin lattice energy transfer***) => nuclei's magnetic moments relax or return to B0 (= regain their longitudinal magnetization) rate at which this occurs is an exponential process and it occurs at different rates in different tissues => T1 time of a tissue is an intrinsic contrast parameter that is inherent to the tissue being imaged T1 recovery = e time it takes for 63% of the longitudinal magnetization to recover, period during which this occurs is the time between one excitation pulse and the next or the ***TR*** => TR determines how much T1 recovery occurs in a tissue T1 relaxation - result of nuclei exchanging the energy given to them by the RF pulse to their surrounding environment and **efficiency of this process determines the T1 time of the tissue in which they are situated** for ex: - *since fat can absorb energy quickly, the T1 time of fat is very short* => nuclei dispose of their energy to the surrounding fat tissue and return to B0 in a short time. - *Water is very inefficient at receiving energy from nuclei* => T1 time of water is quite long => nuclei take a lot longer to dispose of their energy to the surrounding water tissue and return to B0. repetition time (TR) controls how much of the NMV in fat or water has recovered before the application of the next RF pulse: - short TR does not permit full longitudinal recovery in most tissues => contrast difference between fat and water due to their different T1 recovery times; - long TR allows full recovery of the longitudinal components in most tissues => there is no difference in the longitudinal components magnitude => no contrast difference
41
# T2 DECAY I T2 DECAY
caused by the exchange of energy from one nucleus to another (= spin-spin E transfer), occurs as a result of the magnetic fields of the nuclei interacting with each other => loss of phase coherence (= dephasing) => decay of the NMV in the transverse plane, also an exponential process and occurs at different rates in different tissues => T2 decay time of a tissue is a contrast parameter and is characteristic to the tissue being imaged T2 = time it takes for 63% of the transverse magnetization to be lost due to dephasing => transverse magnetization is reduced to 63% of its original value => 37% remains; it occurs over time between the excitation pulse and the MR signal = the ***echo time, TE*** => TE determines how much T2 decay occurs in a tissue T2 relaxation = result of the spins of adjacent nuclei interacting with each other and exchanging energy, efficiency of this process depends on how closely packed the molecules are to each other, for ex: - *In fat, the molecules are closely packed together* => spin‐spin is efficient => T2 time of fat is therefore very short - *In water, the molecules are spaced apart* => spin‐spin is not efficient => T2 time of water is therefore very long TE controls how much transverse magnetization has been allowed to decay in fat and water when the signal is read => short TE does not permit full dephasing in either fat or water => There is little contrast difference between fat and water due to differences in T2 decay times using a short TE. A long TE allows dephasing of the transverse components in fat and water => There is a contrast difference between fat and water due to differences in T2 decay times when using a long TE.
42
tissues with a low proton density always look how on the MRI img?
tissues with a low proton density are always dark on an MR image
43
Tissues in which nuclei move may be | (what and depending on what?)
dark or bright depending on their velocity and the pulse sequence used
44
T1 weighted images:
differences in the T1 relaxation times of tissues must be demonstrated => TR is selected that is short enough => image with **contrast that is predominantly due to the differences in T1 recovery times of tissues**, differences between the T1 times of tissues is exaggerated **to diminish T2 effects, TE must also be short** => to sum up, T1 weighted img: short T1 (400 ms), short TE (10 ms) => we get an img, where tissues with short T1 relaxation times such as fat, are bright (high signal), tissues with long T1 relaxation times such as water, are dark (low signal) => best demonstration of anatomy, but also pathology if used after contrast enhancement (gadolinium)
45
T2 weighted images:
differences in the T2 relaxation times of tissues must be demonstrated => TE is selected that is long enough => image with contrast that is predominantly due to the differences in the T2 decay times of tissues, differences between the T2 times of tissues is exaggerated **to diminish T1 effects, long TR is selected** => T2 weighted image: long T2 (4000 ms), long TR (100 ms) => Tissues with a long T2 decay time such as water are bright (high signal), tissues with short T2 decay times such as air, are dark (low signal) => T2 weighted images best demonstrate **pathology**
46
PD weighted images
differences in the proton densities must be demonstrated => both T1 and T2 effects are diminished, by selecting selecting a long TR (4000 ms) and short TE (20 ms) respectively => image with contrast that is predominantly due to differences in the proton density of the tissues => tissues with a low proton density are dark (low signal), tissues with a high proton density are bright (high signal) => **anatomy + some pathology**
47
* Cortical bone and air on MR image:
are always dark, regardless of the weighting
48
Answer using the information in figures A and B. What can be said about the contrast of grey matter (GM) and white matter (WM) in a T1w image and in a T2w image? A. GM is as bright as WM on T1 and GM is as bright as WM on T2. B. GM is brighter than WM on T1 and GM is brighter than WM on T2. C. GM is brighter than WM on T1 and GM is darker than WM on T2. D. GM is darker than WM on T1 and GM is brighter than WM on T2. E. GM is darker than WM on T1 and GM is darker than WM on T2.
D. GM is darker than WM on T1 and GM is brighter than WM on T2.
49
What is the weighting of this image?
T2
50
What tissue has the longest T1 & T2 recovery?
water
51
Pulse sequences -
mechanisms that permit refocusing of spins so that images can be acquired with different types of contrast
52
The efficiency of T1 recovery depends on: (2)
1. the inherent energy of the tissue 2. how well the rate of molecular tumbling matches Larmor
53
T1 recovery time is dependent on
magnetic field strength: field strength **increases**, tissues **take longer to relax**
54
T1 contrast is controlled by
TR: for good T1 contrast, the TR must be short
55
T2 recovery time is dependent on
magnetic field strength: field strength **increases**, tissues **take longer to dephase**
56
T2 contrast is controlled by
TE: for good T2 contrast, the TE must be long
57
efficiency of T2 decay depends on
how closely the molecules are packed together
58
Only atoms with an odd number of either protons or neutrons exhibit magnetic resonance.
**True**. Spin angular momentum is an intrinsic property of an atom; those with equal numbers of protons and neutrons have no netspin and so no magnetic moment. With only a single proton, hydrogen has a large magnetic moment.
59
In a 1 T magnetic field a hydrogen atom proton will precess with a frequency of 42.6 MHz.
**True**. This is known as the Larmor frequency and is unique for each element. The frequency varies with magnetic field strength and very slightly depending on what substance the proton is contained within.
60
Placed in a powerful static magnetic field, all the hydrogen atom protons in a patient will align themselves with this field.
**False**. Although all the hydrogen atoms will be affected, nearly as many will run anti-parallel, or in the opposite alignment to the field.
61
The bulk magnetization of one million hydrogen nuclei in a patient will depend on a difference in alignment of only one nucleus in a 1 T magnet.
**False**. It is the population difference between ‘spin up’ and ‘spin down’ states when subject to a strong magnetic field that produces the NMR signal. At room temperature in a 1 T magnet, the population differs by two for every million nuclei involved.
62
It is the combined magnetic vector of the hydrogen nuclei in a static field which provides the signal for MR.
**True**. However, as this vector is in alignment with the magnetic field, it cannot be detected. By applying RF energy to the protons, their net magnetism can be altered into the x,y plane lying perpendicular to the static magnetic field (mxy); this provides the signal for MRI.
63
Most medical magnetic resonance imaging (MRI) detects signals produced by the single protons of hydrogen nuclei.
**True**. The protons comprising hydrogen nuclei are most useful for medical imaging because they are so prevalent in the human body.
64
Other nuclei with uneven numbers of protons or neutrons such as F-19 may also be used in MRI.
**True**. C-13, O-17, F-19 and P-31 can all be used for MRI. At present imaging using anything other than protons is mainly for research purposes.
65
When placed in a 1 T field and before excitation, ‘spin down’ protons predominate.
**False**. Approximately half the protons will align ‘spin up’ and half will be ‘spin down’. At 1 T approximately two extra protons out of every million will align spin up, and this difference accounts for the ‘detectable’ protons that allow the formation of the MR image.
66
Prior to any radiofrequency (RF) pulse the total magnetic vector in the xy plane is equal to 1.
**False**. In the resting state the mxy will be the sum of all the individual out of phase vectors pointing in random directions and thus will be equal to 0.
67
A standard 1 T MRI scanner produces a field strength 100 times that of the earth’s.
**False**. A 1 T field is approximately 20 000 times greater than the earth’s field strength of 50 mT.
68
The net magnetic vector in the z-axis provides a recordable MR signal.
**False**. The z-axis is in line with the field. To enable creation of an MR signal, an RF pulse is applied which tips the net magnetic vector
69
The signal recorded in a 1.5 T magnet will be proportionally higher than in a 3.0 T magnet.
**False**. Signal increases with static field strength.
70
MR signal strength is inversely proportional to proton density.
**False**. Increased PD (number of protons per unit volume) will give an increased signal.
71
RF transmitter/receiver coils need to be able to perform both functions simultaneously.
**False**. A coil can act in both transmit and receive modes, but not simultaneously.
72
Most signals from the body are received from water protons.
**True**. Water protonsform the basis of most MRI, but protons are also very prevalent in fat
73
In the plane running transverse to the static magnetic field, there is no MR signal at rest.
**True**. The signal is only detectable following the application of RF energy
74
Application of RF energy causes the hydrogen protons to precess in phase.
**True**. The application of RF photons at the Larmor frequency will energize the hydrogen protons, causing them to precess in time with one another; this creates a signal which is detectable.
75
A 90-degree pulse requires more energy than a 180-degree pulse.
**False**. A 180-degree pulse has enough energy to reverse the net magnetic vector. A 90-degree pulse is halfas energetic (note this is the total energy of the pulse).
76
Following an RF pulse, the phase coherent protons will remain in this state indefinitely
**False**. Following an RF pulse, those protons in phase and creating a detectable MR signal will immediately begin to dephase due to T2 relaxation, and field inhomogeneities and the signal will rapidly diminish.
77
MR signal depends only on the proton density of the material.
**False**. It also depends on the - field strength - RF pulse flip angle and – to an extent depending on the pulse sequence timings used – - on T1 and T2 relaxation processes - magnetic field inhomogeneities. With a higher field strength, more protons are initially spin up.
78
The Larmor frequency is the frequency of precession of the protons.
**True**. For hydrogen nuclei at 1 T it is approximately 42.6 MHz. It is proportional to field strength, and is also slightly affected by the substance it is in. The Larmor frequency for hydrogen within fat and water is very slightly different, which is the *cause for chemical shift artefact*.
79
Photons with twice the Larmor frequency have the correct energy to tip all the ‘spin up’ protons to ‘spin down’.
**False**. Photons with the same frequency as the Larmor frequency have the correct energy to cause the magnetic vector of a single proton to flip from spin up to spin down. *At 1 T this is approximately 0.2 meV*. ***This frequency lies within the radio-wave end of the electromagnetic spectrum, which is why there is no ionizing radiation in MRI.***
80
Photons in a 180-degree RF pulse have twice the energy of photons for a 90-degree RF pulse.
**False**. A 180-degree pulse has approximately twice the number of photons, but the photons still all must match the Larmor frequency and thus have the same energy.
81
An initial 90-degree RF pulse reduces the net magnetic vector in the z-axis to approximately 0.
**True**. An initial 90-degree RF pulse flips the net magnetic vector such that it lies in the transverse xy plane, reducing the net mz to 0. It also causes the individual protons to precess in phase and thus produces a detectable net mxy rotating at the Larmor frequency.
82
As the magnetic vector returns to its equilibrium position along z, a signal is produced which is received by an RF coil to form the picture.
**True**. The signal used to generate the image is caused by the rotating magnetic vector inducing a current to flow in the RF coils in the same way that a dynamo works. This current is used to form the image.
83
T1: It is the time taken for transverse recovery to reach 37% of the maximum value.
**False**. T1 recovery is in the *longitudinal direction* and is also known as spin–lattice relaxation. T1 is the ***time for 63% maximum recovery***.
84
T1 is increased with greater field strength.
**True**. Stronger magnetic fields hasten the precession, this lengthens T1.
85
Fat and melanin both produce a high signal on a T1-weighted image
**True**. This occurs as they both have a short T1
86
A short time to echo (TE) and short time to repeat (TR) will give a T1-weighted image.
**True**. T1-weighted imagesrequire a short TR and a short TE. Tissues with a short T1 will appear bright with these settings
87
T1 is always longer than T2.
**True**. Protons dephase faster than they realign with the static magnet.
88
T2 decay is longitudinal relaxation.
**False**. It is transverse relaxation
89
A long TR and long TE will give a T2-weighted image.
**True**. Tissues with a long T2 relaxation time give a high MR signal with T2 weighting. TE should ideally be of the order of the T2 relaxation time of the tissues of interest.
90
Cerebrospinal fluid (CSF) and flowing blood will produce high signal on a T2-weighted imaged.
**False**. *CSF, urine, amniotic fluid and water* all have ***long T2*** and are therefore high signal. *Blood* flowing into the imaged slice after the initial 90-degree RF pulses ***does not produce signal***
91
The T2 of grey matter is longer than that of white matter.
**True**. The difference is minimal, approximately 10 ms
92
Spin–spin relaxation occurs because the neighbouring protons exert a tiny magnetic field of their own which can alter the rate of precession.
**True**. This has most effect in solids which have a very short T2.
93
T2 decay occurs due to spin–lattice relaxation.
**False**. Spin–spin relaxation leads to T2 decay through the transfer of energy between adjacent nuclei.
94
T2 relaxation time increases with an increase in magnet strength
**False**. This is true of T1. T2 is unaffected by magnet strength
95
T2 decay is affected by magnetic field inhomogeneities.
**True**. If only a single 90-degree pulse is applied, the MR signal undergoes FID; ***true spin–spin relaxation is enhanced by magnetic field inhomogeneities***. This situation is referred to as T2' and is generally countered using a 180-degree rephasing pulse.
96
When 63% of the transverse signal is lost, this is referred to as time T2.
**True**. T2 is the time when 37% of the transverse magnetization remains. T1 is the time at which 63% of the longitudinal signal has recovered.
97
Free induction decay (FID) is also known as spin–lattice relaxation.
**False**. T1 recovery is also known as spin–lattice relaxation and describes the recovery of the longitudinal magnetization of its equilibrium value along z, with associated loss of energy to the surrounding lattice. T2 decay is spin–spin relaxation and describes the dephasing of the mxy vector due to the small fields caused by surrounding dipoles. An FID signal, however, has amplitude which depends on T2' relaxation. T2' is more rapid than T2 and includes the dephasing effects of magnetic field inhomogeneities.
98
T2 always has a longer decay time than T2'.
**True**. T2' is the decay caused by field inhomogeneities plus tissue relaxation. A further 180-degree RF pulse in SE sequences helpsto reduce the effect of field inhomogeneities by rephasing the mxy and thus tissues show a true T2 signal.
99
T1 time is the time for 63% recovery of mz.
**True**. Conversely, T2 is the time for the mxy to fall to 37% of its value.
100
Fat and large molecules shorten the T1 time of tissues.
**True**. Fat and large molecules such as proteins in fluid are effective at removing energy in spin–lattice relaxation; this shortens T1. However, in solids, where water is more tightly bound, T1 relaxation becomes less efficient and T1 lengthens.
101
Local field variation is fastest in free fluids such as water, giving a short T2.
**False**. In water, where molecules are moving around very rapidly, dipole–dipole interactions are very brief, making T2 relaxation less efficient, leading to a long T2.
102
A very large current is drawn from the electrical mains supply to maintain super conductance.
**False**. It takes several hours for the current in the coil to build up. Once the unit is superconducting, the supply is shorted and the current continues to flow within the magnet without drawing any further external current.
103
Quenching of the system may occur spontaneously if the operating temperature is not maintained.
**True**. If the cooling fails, the system will rapidly heat up due to a loss of superconductivity causing resistive heat losses in the magnet windings. This results in rapid boil-off of liquid helium.
104
A Faraday cage minimizes the effect of the scanner magnetic field beyond the boundary of the scanner room.
**False**. The Faraday cage is a wire mesh that serves to screen the scanner from external RF interference.
105
The field strength at 2 m from the centre of the magnet is 25% of the strength at 1 m from the centre of the magnet
**False**. This is inverse square law which applies to radiation exposure. Modern MRI scanner static fields generally fall-off more rapidly due to active shielding.
106
The use of surface coils gives greater image uniformity than body coils
**False**. Surface coils give better SNR and/or resolution for near-surface tissues but less uniformity. The signal from near to the surface coil is much brighter than on the opposite side of the FOV.
107
A 0.5 T superconducting magnet produces a greater field strength than a 0.5 T resistive magnet.
**False**. The strength of a 0.5 T magnet is 0.5 T. It does not matter what type of magnet is producing it. However, only superconducting magnets are capable of producing fields of *above 0.5 T*. Resistive magnets are limited to approximately 0.5 T by heating effects, and permanent magnets are only made in field strengths up to about 0.3 T.
108
A paramagnetic MR system uses a conductive magnet
**False**. The term paramagnetic is used to describe how some molecules behave within a magnetic field; gadolinium is an example of a paramagnetic substance.
109
A permanent magnet may be rapidly shut down in an emergency
**False**. A permanent magnet cannot be shut down at all. A resistive magnet may be shut down rapidly by switching off the power. A superconducting magnet may be shut down but only very slowly if a quench is to be avoided. In a true emergency, the helium is released raising the temperature of the magnet and thus removing the superconducting properties. This has the effect of rapidly reducing the field strength, but even this method is not as fast as switching off a resistive magnet and can prove very expensive and damaging to the equipment.
110
Shim coils are coilsthat are fine tuned to make the main magnetic field as uniform as possible.
**True**. This reduces field inhomogeneities and thus allows better images to be obtained.
111
Surface coils are placed directly on the patient.
**True**. This is most commonly seen in spinal MRI with surface coils along the back giving very detailed images of the spine.