Current magnetic resonance (MR) imaging systems use four basic types o
f magnets: permanent, resistive (electromagnets), hybrid (combines pri
nciples of permanent and resistive magnets), and superconducting (resi
stive-like magnets cooled to near absolute zero to achieve superconduc
tivity). The first three have relatively low field strength (0.2-0.6 T
) compared with superconducting magnets (2.0 T), but they cost less, h
ave limited fringe fields, and have minimal siting restrictions. Altho
ugh current low-field-strength units have signal-to-noise ratios compe
titive with those of high-field-strength superconducting units, the la
tter still allow faster data acquisition. Use of shim coils improves t
he uniformity of the primary magnetic field and thus image quality. Ho
wever. distortions may be incurred depending on the magnetic susceptib
ility of materials being imaged or chemical shift effect. Image nonuni
formities can result from the interactions between the shim coils and
gradient coils, which are used to create the high-performance linear g
radients needed in many MR techniques (eg, gradient-echo and echo-plan
ar imaging). The gradient coils must be shielded to prevent these eddy
current effects. The imager must also be shielded from external radio
-frequency signals, which can cause interference. Image degradation ca
used by respiratory motion, cardiac motion, and blood flow can be redu
ced by use of gating and special imaging techniques.