Title: Gradient echo pulse sequences
1Gradient echo pulse sequences
- Conventional gradient echo
- Steady state Coherent gradient echo
- Steady state Incoherent gradient echo
- Steady state free precession
- Ultra fast sequences
- Echo planer imaging (EPI)
2Gradient echo pulse sequences
- Conventional gradient echo
- Uses variable flip angles so that, TR and
therefore the scan time, can be reduced without
producing saturation. - A gradient instead of 180 rephasing RF pulse is
used to rephase the FID. - The frequency encoding gradient is used for this
purpose. - A gradient is quicker to apply than a 180 pulse
- Therefore the minimum TE can be reduced.
3- Frequency encoding gradient is initially applied
negatively to speed up the dephasing of the FID. - Then its polarity is reversed producing rephasing
of the gradient echo. - Gradient does not compensate for magnetic field
inhomogenities - So the resultant echo displays great deal of T2
information - Used to acquire T2, T1, and proton density
weighting - Allow for reduction in scan time as the TR is
greatly reduced
4Conventional gradient echo
TR
RF
RF
Echo
FID
FID
Frequency encode
rephase
dephase
TE
5Uses of gradient echo
- Used for single slice breath-hold acquisitions in
the abdomen - Used for dynamic contrast enhancement
- Used to produce angiographic type images, because
the flowing nuclei which have been previously
excited, always give a signal as gradient
rephasing is not slice selective.
6Manipulating Parameters
- Flip angle and TR determines the degree of
saturation and, therefore the T1 weighting. - For saturation flip angle should be large and TR
short so that full recovery cannot occur. - To prevent saturation, flip angle should be small
and the TR long enough to permit full recovery. - TE controls the amount of T2 dephasing
- To minimize T2 Te should be short
- To maximize T2 TE should be long.
7Typical values
- T1 weighting
- Large flip angle 70 -110 degrees
- Short TE 5-10 ms
- Short TR less than 50 ms
- Average scan time several seconds to minutes
- T2 weighting
- Small flip angle 5 -20 degrees
- Long TE 15 -25 ms
- Short TR enough for full recovery as flip angle
is small - Scan time several seconds to minutes
- Proton density weighting
- Small flip angle 5 -20 degrees
- Short TE 5 -10 ms
- Short TR for full recovery as flip angle is small
- Scan time several seconds to minutes
8The steady state
- This is a stage where the TR is shorter than the
T1 and T2 times of the tissues. - There is no time for the transverse magnetization
to decay, before the pulse sequence is repeated - There is coexistence of both longitudinal and
transverse magnetization - The flip angle and TR maintain the steady state
which holds the longitudinal and transverse
components and the NMV steady during the data
acquisition - Flip angles of 300 to 450 and TR of 20 to 50 ms
achieves a steady state.
9B0
Longitudinal component held steady
NMV held steady
Transverse component held steady
- If steady state is maintained, the transverse
component does not have time to decay during
pulse sequence. - This transverse magnetization, produced as a
result of previous excitations , is called the
residual transverse magnetization(RTM)
10- The residual transverse magnetization (RTM)
affects the contrast as it results in tissues
with long T2 times , appearing bright on the
image - Most gradient echo sequences use the steady
state, as the shortest TR and scan times are
achieved. - Gradient echo sequences are classified according
to whether the residual transverse magnetization
is in phase (coherent) or out of phase
(incoherent).
11Learning point
- The steady state involves repeatedly applying RF
pulses at TR less than the T1 and T2 of all
tissues - This train of RF pulses generates two signals
- A FID signal which occurs as a result of the
withdrawal of the RF pulse and contains T2
information - A spin echo whose peak occurs at the same time as
an RF pulse
12- This happens because every RF pulse contains
individual radio waves that have sufficient
energy to rephase a previous FID - These radiowaves rephase the RTM left over from
previous RF excitation pulses to form a spin
echo. - This ocurs at exactly the same time as the next
RF pulse as the RTM takes the same time to
rephase as it took to dephase. Therfore when
utilizing steady state , the TR TAU of the spin
echo.
13A FID and a spin echo occur at each RF pulse
RF pulse 2
Produces own FID and rephases FID of pulse 1
RF pulse 3
RF pulse 1
Spin echo
FID
FID
FID
dephasing
rephasing
TR
14Summary
- Any two RF pulses produce a spin echo.
- The first RF pulse excites the nuclei regardless
of its net amplitude - The second RF pulse rephases the FID resulting
from the first. - The spin echoes produced are sometimes called
Hahn or stimulated echoes. - This concept applies to all pulse sequences that
use steady state.
15GE-Coherent residual transverse magnetization
- This pulse sequence uses a variable flip angle
excitation pulse followed by gradient rephasing,
to produce a gradient echo. - Steady state is maintained by selecting TR
shorter than T1 and T2 - There is therefore RTM left over when the next
excitation pulse is applied. - The RTM is kept coherent by a process known as
rewinding.
16- Rewinding is achieved by reversing the slope of
the phase encoding gradient after readout. - This results in RTM rephasing, so that it is in
phase at the beginning of the next repetition - This alows the RTM to build up so that tissues
with a long T2 time produce a high signal.
17Coherent gradient echo pulse sequence
TR
Rewinder gradient
Phase encode
readout
FID
echo
18Sample image
- T2 weighted image using a coherent gradient
echo. TE 15 ms, TR 40 ms, flip 350, breath
holding single slice obtained in 11s
19Uses of coherent gradient echo
- This pulse sequences produce T2 weighted images.
- As fluid is bright they give an angiographic,
myelographic or arthrographic effect. - Can be used to determine whether a vessel is
patent, or whether an area contains fluid. - Can be acquired slice by slice, or in a 3D volume
acquisition - As the TR is short, a sliice can be acquired in a
single breath hold.
20Parameters
- To maintain the steady state
- Flip angles 30 45
- TR 20-50 ms
- To maximize T2 long TE 15- 25 ms
- Use gradient moment rephasing to accentuate T2
- Average scan time
- Seconds for single slice
- 4-15 min for volumes
- (to minimize T2 to produce T1 or proton density
weighting TE should be the shortest possible)
21Advantages Disadvantages
- Very fast scans, breath holding possible
- Very sensitive to flow so good for angiography
- Can be acquired in a volume acquisition
- Poor SNR in 2D acquisitions
- Magnetic susceptibility increases
- Loud gradient noise
22Incoherent(spoiled) RTM
- Pulse sequence that use incoherent RTM begin with
a variable flip angle excitation pulse, and use
gradient rephasing to produce agrdient echo. - The steady state is maintained so that RTM is
left over from the previuos RF. - The RTM is spoiled so that its effect on image
contrast is minimal. - There are two ways to achieve spoiling
- Digitized RF spoiling
- Gradient spoiling
23RF spoiling
- RF spoiling is achived by controling the phase of
the digitised RF pulses that are transmitted. - The digitized RF is transmitted at a specific
frequency phase - The resultant NMV and transverse component are
fillped to a certain position in the transvere
plane. - The receiver coil can lock onto the phase of the
RF that has just being transmitted and receives
only signal at that phase. - Transverse magnetization at other phases or
positions in the transverse plane are not recived
by the coil
24- Each RF is delivered at a different phase and the
receiver coil is locked to recieve signal only at
that phase - This process continues and the TRM which is at a
different phase is ignored by the receiver coil. - So the effect of RTM on the image is eleminated.
- T2 is therefore cannot predominate and T1 and
proton density weighting prevails.
25Uses
- RF spoild GE pulse sequencs produce T1 or proton
density weited images, although fluid may have a
rather high signal due to gradient rephasing - Can be used for 2D and volume acquisition and as
the TR is short the 2D acquisition can be used to
acquire T1 weighted breath-hold images. - Demonstrate good T1 anatomy
26Example for RF spoiled GE 5.21
- T1/proton density weighted image using RF
spoiling. TE 6 ms, TR 35 ms, flip 35, part of
volume acqusition which took 7 minutes
27Parameters
- To maintain steady state
- Flip angle 30-45
- TR 20-50 ms
- To maximise T1 short TE 5-10ms
- Average scan time several seconds for single
slice, 4-15 min for volumes - Advantages
- Can be acquired in a volume or 2D
- Breath holding possible
- Good SNR and anatomical detail in volumes
28Gradient spoiling
- Gradient spoiling is the opposite of rewinding.
- The slice select, phase encoding, and frequency
encoding gradients can be used to dephase the
RTM, so that it is incoherent at the beginning of
the next repetition. - T2 effects are reduced
- Uses and parameters are similar to those in RF
spoiling. - Can be used to achieve T2 when the parameteres
are similar to those in conventional GE.(because
GS is less efficient than RF spoiling and moreT2
information is present in the signal)
29Steady state free prcession (SSFP)
- Can be used to get shortest possible TR and scan
time with steady state GE - Used to produce more T2 weighted images than
conventional gradient echo sequences. - The pulse sequences used here help to obtain
images that have a sufficiently long TE and less
T2 when using steady state than other gradient
echo pulse sequences. - This is achieved in the manner described below.
30Composition of RF pulse
- RF pulse contains radio waves of differing
amplitudes. The magnetude of RF pulse is an
average of these amlitudes. E.g. - 10 waves of amplitude of 100
- 2 waves of amplitude of 300
- 15 waves of amplitude of 600
- 5 waves of amplitude of 1800
- The average amplitude 19600/32 61.250
31- Therfore every RF pulse contains waves that on
their own have sufficient magnitude to move
magnetic moments within the NMV through 1800. - These radio waves are therefore able to rephase a
FID. - In SSFP, the steady state can be maintained by
using a flip angle between 300 and 450 with a TR
of 20-50ms. - Every TR an excitation pulse is applied.
- When the RF is switched off a FID is produced.
32- After the TR another excitation pulse is applied
which also produces its own FID. - The radiowaves within it that have an amplitude
of 180 rephase the FID from the previous pulse,
and a spin echo is produced. - Each RF pulse therefore not only produces its own
FID, but also rephases the FID produced from the
previous excitation. - As nuclei take as long to rephase as they took to
dephase, the echo from the first excitation pulse
occurs at the same time as the third excitation
pulse. - However this cannot be sampled, as RF cannot be
transmitted and received at the same time.
33- To receive the spin echo, a rewinder gradient is
used to speed up the rephasing process after the
RF rephasing has begun. - The rewinding moves the echo so that it occurs
before the next excitation pulse, rather than
during it. - This way the resultant ehco can be received.
- It demonstrate more true T2 weighting than
conventional gradient echo sequences. - Because
- The effective TE is now longer than the TR.
- The rephasing is initiated by an RF pulse rather
than a gradient so that more T2 and less T2
information is present.
341
3
2
FID 1
Echo of FID 1
FID 3
FID 2
TE
TR
1
3
2
Rewinder gradient
FID 1
Echo of FID 1
Effective TE
35Effective TE actual TE
- Actual TE is the time between the echo and the
next excitation pulse - Effective TE is the time from the echo to the
excitation pulse that created its FID - Effective TE (2xTR) actual TE
- If TR 50 ms, actual TE 10 ms
- Then effective TE 90 ms
36Uses of SSFP
- Used to acquire images that demonstrate true T2
weighting. - Especially useful in the brain and joints and on
most systems can be used with both 2D and 3D
volume acquisitions.
Effective TE 71 ms, TE 9ms, TR 40 ms, flip angle
350, volume scan time 9 minutes.
37Parameters
- To maintain steady state flip angle 30-45, TR
20-50 ms - Actual TE affects the effective TE unless the
system uses a fixed TE. - Average scan time 4-15 min volume acquisition
- Some manufacturers suggest decreasing the
effective TE to reduce magnetic susceptibility,
and increasing the flip angle to create more
transverse magnetisation which results in higher
SNR
38Comparison between Coherent, incoherent SSFP
RF pulse
RF pulse
RF pulse
FID spin echo
FID
FID
Spin echo
Gradient echo
Gradient echo
TE
TE
FID
TE
Spin echo moved away from RF pulse by rewinding
gradient
Coherent
Incoherent
SSFP
39Ultra-fast sequences
- Advances have been made in developing very fast
pulse sequences. - Usually employ the coherent or incoherent
gradient echo sequences. - The TE is significantly reduced by
- Aplying only a portion of the RF exciation pulse.
- Reading only a portion of the echo
- TE kept to a minimum (2.5 3.0 ms)
- TR and therefore the scan time is reduced.
- TR as low as 10 ms is achieved and about 16
slices can be achieved in a single breath hold.
40- Many ultra-fast sequences use extra pulses
applied before the pulse sequences begins, to
pre-magnetise the tissue. - This way certain contrast can be obtained.
- Pre-magnetisation is achieved in the following
manner. - Applying a 1800 pulse before the pulse sequence
and a specified delay time similar to inversion
recovery. - Applying a combination of 900/1800/900 pulses
before the pulse sequence begins.
41- (first 90 pulse produces transverse
magnetisation. 180 pulse rephases this, and at a
specific time later second 90 pulse is applied.
This drives the coherent transverse
magnetisation into the longitudinal plane. It is
available to be fliped when the pulse sequence
begins. This is used to produce T2 contrast and
is sometimes known as driven equilibrium)
42Echo planer imaging(EPI)
- Fills all the lines of k-space during one TR
- Uses a single echo train
- Multiple Echos are generated and each is phase
encoded by a different slope of gradient to fill
all the required lines of k space. - Echoes are generated either by 180 rephasing
pulses or by gradients. - Gradients are much faster