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Encoding and image formation
1.
2. Content
o Encoding
o Gradients
o Slice selection
o Frequency encoding
o Phase encoding
o Sampling
o Nyquist Theorem
o Data collection and image formation
o K space description
o K space filling
o Fast Fourier transform (FFT)
3. Encoding
• Locating the signal in 3 dimensions so that
it can positioned each signals at correct
points on the image.
• First locate a slice.
• Once a slice is selected, the signal is
located or encoded along both axis of the
image.
• These are performed by gradients.
4. Select a slice
Locate/encode signal along both axis of the image
Locating slice & encoding signal is performed by gradients
5. Gradients
• Gradients are alteration to the main magnetic field and
generated by cell of wire located with in the bore of magnet
through which current is passed.
• The passage of current through a gradient coil induces a
gradient coil induces a gradient magnetic field around it.
• which either subtracts from, or adds to the main static
magnetic field Bo.
• Bo is altered in a linear fashion by the gradient coils.
• so, the magnetic strength and therefore precessional
frequency experienced by nuclei situated along the axis of the
gradient can be predicted called spatial encoding.
• 3 gradients coils situated within the bore of the magnet.
6. • These are named A/c to the axis along which they act when they
are switched on.
• These directions in a super conducting magnet.
o Z- gradient alters the magnetic field strength along the z- (long)
axis of the magnet.
o Y – gradient alters the magnetic field strength along the Y-
(vertical) axis of the magnet.
o X- gradient alters the magnetic field strength along the X-
(horizontal) axis of the magnet.
• Gradients can be used to either dephase or rephase the magnetic
moments of nuclei.
• Gradients also perform the 3 main tasks in encoding-
1. Slice selection
2. Phase encoding
3. Frequency encoding
7.
8. Slice selection
• Locating a slice within the scan plane selected.
• When a gradient coil is switched on. The magnetic field
strength and therefore precessional frequency of nuclei
located along its axis.
• Nuclei situated within a slice have particular
precessional frequency.
• A slice can be selectively excited, by transmitting RF
with a band of frequencies coinciding with the larmour
frequencies of spins in a particular slice as defined by
the slice select gradient.
9.
10. Slice thickness
• A band of nuclei must be excited b y the excited by the
excitation pulse.
• The slope of the slice select gradient determined the
differences in precessional frequency between the two point
on the gradients.
• Steep gradient slopes result in a large difference in
precessional frequency between two points on the gradient.
• While shallow gradient slopes result in a small difference in
precessional frequency between the same two points.
• The RF pulse transmitted to excite the slice must contain a
range of frequencies to match the difference in precessional
frequency b/w two points.
11. • This frequency range is called the bandwidth and the RF is being
transmitted at this point it is specifically called transmit
bandwidth.
o To achieve thin slices, a step slices select slope or narrow
transmit bandwidth is applied.
o To achieve thick slices, a shallow slices select slope or broad
transmit bandwidth is applied.
Note:-
To achieve the axial slices then cut the z-gradient.
To achieve the coronal slices then cut the Y-gradient.
To achieve the sagittal slices then cut the X-gradient.
12. A B
Thick slice- shallow gradient
Thin slice- steep gradient
To achieve thin slices, a steep slice select slope & narrow bandwidth is applied.
To achieve thick slice, a shallow slice select slope & broad bandwidth is
applied.
Bandwidth Bandwidth
13. Phase encoding
• The signal must now be located along the
remaining short axis of the image and this
localization of signal is called phase encoding.
• When the phase encoding gradient is
switched on, the magnetic field strength and
therefore precessional frequency of nuclei
along the axis of the gradient is altered.
• The phase encoding gradient is usually
switched on just before the application of the
180* rephasing pulse.
14. Fig showing phase change of nuclei when phase
encoding gradient is switched on
15.
16. Frequency encoding
In this process signal is located along the long axis (z- axis) of
the anatomy.
When frequency encoding gradient is switched on-
Now signal can be located along the axis according to its frequency.
Magnetic field strength & precessional frequency of signal
along the axis of the gradient is altered in a linear fashion.
Thus, this gradient produces a frequency
difference or shift of signal along the axis.
17.
18. When gradients are switched on
Spin echo
sequence
Gradient echo spin
sequence
Slice select 90 & 180 RF pulse Excitation pulse
Phase encoding Before 180 RF pulse B/t excitation & signal
collection
Frequency
encoding
Collection of the signal Collection of the signal
21. The frequency encoding gradient is switched on while
the system reads frequencies present in the signal, &
samples or digitizes them.
This gradient is sometimes called Readout gradient.
Duration of readout gradient is called sampling time/
acquisition window.
Sampling rate- rate at which frequencies are sampled
or digitized during readout. system samples
frequencies up to 1024 different times.
Each sample is stored as a data point.
Sampling
22. Collected data or information from each signal is
stored as data points
K-space is rectangular in shape & has two axis
perpendicular to each other.
Unit of k-space is radians per cm.
K-space is a special frequency domain where information about
the frequency of a signal & where it comes from in the patient is
stored.
23. Frequency axes- horizontal
Phase axes- vertical.
Each slice has its own k-space.
Data space– matrix of processed image
data.(analog signal)
24. An MR image consists of a matrix of pixels, the number of which is
determined by the no. of lines filled in K- space and no. of data points in each
line.
Each data point contains phase and frequency information from the whole
slice at a particular moment in time during read out.
The FFT process mathematically converts this to frequency amplitudes in the
frequency domain. It is necessary because gradients spatially locate signal
according to their frequency, not their time