US 5,291,171 AGranted

Magnet apparatus suitable for magnetic resonance imaging

AssigneeShin-Etsu Chemical Co., Ltd.

InventorsNobutaka Kobayashi, Ken Ohashi, Koji Miyata

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Abstract

The invention relates to an apparatus for producing a magnetic field in a space between two oppositely arranged permanent magnet discs, which is suitable for use in magnetic resonance imaging (MRI). An object of the invention is to reduce the size and weight of the yoke connecting the two permanent magnet discs without causing magnetic saturation of the yoke in view of the fact that magnetic saturation of the yoke leads to the appearance of leakage flux and consequential lowering of the uniformity of the magnetic field. The object is accomplished by regulating the cross-sectional area of the whole magnetic path in the yoke, A.sub.y, such that the following equation holds: A.sub.y =1/a.times.A.sub.m B.sub.m /B.sub.ys, where A.sub.m is the cross-sectional area of magnetic path in each permanent magnet disc, B.sub.m is the magnetic flux density in each permanent magnet disc at normal temperature, B.sub.ys is the saturation magnetic flux density of the yoke at normal temperature, and a is a coefficient the value of which is not larger than 1 and not smaller than 0.6.

Claims4

Dependent claims

A magnet apparatus suitable for magnetic resonance imaging, the apparatus having a pair of permanent magnet discs each of which is magnetized in the direction of thickness, a yoke which connects said pair of permanent magnet discs and holds the permanent magnet discs parallel and opposite to each other such that a pole face of one of the permanent magnet discs faces the opposite pole face of the other and a pair of disc-like pole pieces which are placed on the opposite pole faces of said pair of permanent magnet discs, respectively, so as to produce a uniform magnetic field in a cylindrical space between the two permanent magnetic discs,

characterized in that in said yoke the cross-sectional area of the whole magnetic path, A.sub.y, is regulated such that the following equation holds:
A.sub.y =1/a.times.A.sub.m B.sub.m /B.sub.ys
where A.sub.m is the cross-sectional area of magnetic path in each of said pair of permanent magnet discs, B.sub.m is the magnetic flux density in each of said permanent magnet discs at normal temperature, B.sub.ys is the saturation magnetic flux density of said yoke at normal temperature, and a is a coefficient the value of which is not larger than 1 and not smaller than 0.6.

Dependencies are inferred from the claim text.