Selecting the slice plane and spatial encoding of each voxel involves the use of magnetic field gradients. The intensity of the magnetic field varies regularly along the gradient application axis. These magnetic field gradients are characterized by amplitude(greater or lesser field variation for the same unit of distance), direction, duration and moment of application.
The slice selection gradient modifies the precession frequency of the protons such that an RF wave of the same frequency will cause them to shift (resonance). The selective pulse bandwith and gradient amplitude will determine the slice thickness.
The slice selection gradient is simultaneously applied to all the RF pulses.
The phase encoding gradient (GPE) differentiates the « rows ». GPE is regularly incremented, as many times as there are rows to receive, leading to different phase shifts for each voxe line. The frequency encoding gradient (GFE) differentiates the « columns ». Its application gives distinct frequencies to each voxel column.
In 3D imaging, more phase encoding steps, applied in the third spatial direction, are added to each of these phase encoding steps, thus lengthening acquisition time. 3D imaging improves spatial resolution and the signal to noise ratio.
Phase and frequency encoding can be compared to a sieve that is sensitive to spatial distribution, in the horizontal and vertical directions, and whose fineness varies according to gradient value.
The entire set of data is combined in the RF signal simultaneously received on applying the GFE (still called the readout gradient). All the signals of the same slice are recorded in a matrix then processed to form an image of the slice plane.