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1 Magnetic Field Gradients • Spatial information is obtained by the application of magnetic field gradients (i.e. a magnetic field that changes from point-to- point). • Gradients are denoted as Gx, Gy, Gz, corresponding to the x, y, or z directions. Any combination of Gx, Gy, Gz can be applied to get a gradient along an arbitrary direction (gradients are vector quantities). • Depending on the gradient’s function, these gradients are called – Slice-select gradient – The read or frequency-encoding gradient

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Magnetic Field Gradients. • Spatial information is obtained by the application of magnetic field gradients (i.e. a magnetic field that changes from point-to-point). - PowerPoint PPT Presentation

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Page 1: Magnetic Field Gradients

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Magnetic Field Gradients • Spatial information is obtained by the application of magnetic field gradients (i.e. a magnetic field that changes from point-to-point).

• Gradients are denoted as Gx, Gy, Gz, corresponding to the x, y, or z directions. Any combination of Gx, Gy, Gz can be applied to get a gradient along an arbitrary direction (gradients are vector quantities).

• Depending on the gradient’s function, these gradients arecalled – Slice-select gradient – The read or frequency-encoding gradient – The phase-encoding gradient

Page 2: Magnetic Field Gradients

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Slice Selection Gradient

• Gradient coils provide a linear variation in Bz with position.

• Result is a resonant frequency variation with position.

Bz

Position

= (B0 + Bz)

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Selective Excitation

Frequency

Mag

nitu

de

Time

RF

Am

plitu

de

Pos

ition Slope =

1 G

Frequency

RF Pulse (Resonance Freq and Bandwidth)

Slice

(position &

thickness)

Thickness = BW/Bz

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RF Pulse for Excitation

• The bandwidth of an RF pulse depends on its length and shape.

• Fourier Transform of a RF pulse displays bandwidth.

• A RF pulse with a sinc profile is commonly used in MRIfor slice selection.

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Frequency Encoding

• After having defined a slice through the subject, we need to resolve features along the other two directions (x and y) using frequency-encoding (along x) and phase encoding (along y)

• A smallest volume element in this slice is called a “voxel”.

• The frequency encoding gradient is applied when we “read-out” signals

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Image Acquisition

• Gradient causes resonant frequency to vary with position.

• Receive sum of signals from each spin.

Frequency

Position

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Image Reconstruction

• Received signal is a sum of “tones.”

• The “tones” of the signal are intensities of objects.

• This also applies to 2D and 3D images.

FourierTransform

Received SignalFrequency(position)

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Readout Example

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Phase Encoding

• Phase encoding resolves spatial features in the vertical direction (y) by using the phase information of precessing spins.

• To get enough data to make an image, we need to repeat the phase encoding process many times, each time with a different strength of phase encoding to impart a different phase angle to the voxel.

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Number of Phase Encoding Step

• The # of phase encoding steps = # of rows in image (i.e. the resolution in the y-direction).

• The phase shift between adjacent rows is = 360° / # rows

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Pulse Sequences

• Excitation and imaging are separate.

• Pulse sequence controls:

• RF excitation

• Gradient waveforms

• Acquisition

• Reconstruction information as well.

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1D-Pulse Sequence

RF

Gz

Gx

Acq.

Excitation Readout

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1D-Pulse Sequence – Detailed!

RF

Gz

Gx

Acq.

Phase, Modulation Frequency

Finite amplitude, slew rate

• Demodulation frequency, phase• Sampling rate and duration

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2-D Image Sequence

RF

Gz

Gx

Acq.

Excitation Readout

Gy

Phase-encoding

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2D Image Reconstruction

ky

kx

Frequency-space(k-space)

Image space

FT

(phase-encoding)

readout

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Resolution

• Image resolution increases as higher spatial frequencies are acquired.

1 mm 2 mm 4 mm

ky

kx

ky

kx

ky

kx

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k-Space Trajectories

kx

ky

kx

ky

kx

ky

2D FourierTransform

Echo-Planar Spiral