Open-circuit magnet structure for cross-field tubes and the like

Claim 2

In an open permanent circuit defining a relatively small working gap a permanent magnet assembly comprising: a first body comprising magnetic material including Alnico and having north and south pole faces, said body defining one boundary of said working gap with one of said pole faces; a second body comprising magnetic material including Cobalt in chemical union with a rare earth element and having north and south pole faces; and a transition member comprising iron, said member being interposed between said first and second bodies in contact with opposite pole faces of said bodies such that said first body contacts said transition member with the other of said pole faces, and said second body contacts said transition member with a pole face thereof which is polarized oppositely to said other pole face of said first body, whereby the flux density within said working gap is enhanced.

Claim 3

A magnetic assembly as in claim 1, in which said first body face has an area A 1 and said second body face has an area A 2 and area A 2 is greater than A 1 , whereby the flux of said second body is concentrated and tends to match that of said first body.

Claim 4

An assembly as in claim 2 in which area A 1 is to area A 2 as the intrinsic force of said Cobalt magnetic body is to the intrinsic force of said Alnico magnetic body.

Claim 5

An assembly as in claim 2 in which said first body has a length L 1 and said second body has a length L 2 , and the length L 1 is greater than L 2 .

Claim 6

An assembly as in claim 1 in which the volume of said first body is greater than the volume of said second body.

Claim 7

An assembly as in claim 1 in which said first and second magnetic body and said transition member are aligned along a central axis, and in which said faces are parallel to and concentriclly aligned along said axis with one another, and in which said transition member includes two oppositely facing outer surfaces, each surface being generally congruent with the body face which it contacts.

Claim 8

An assembly as in claim 6, in which said first and second magnetic bodies are cylindrical, and said transition member is in the form of a truncated cone.

Claim 9

An assembly as in claim 6, in which said transition member includes a radially extending first portion adjacent to said first body, a second portion axially extending away from said first body, said second body interfacing with said transition member along said axially extending second portion.

Claim 10

An assembly as in claim 8, in which said second body is spaced from said first portion of said transition member, and the areas that interface of said second body and said transition member exceeds the area of the interface between said transition portion and said first body.

Claim 11

An assembly as in claim 1, in which said rare earth is samarium.

Claim 12

An assembly as in claim 1, in which said Alnico is Alnico 5-7.

Claim 13

An assembly as in claim 1, in which said Alnico is Alnico 9.

Claim 14

An open permanent magnetic circuit for developing an optimal degree of flux density within a gap in said circuit, comprising: a first permanent magnet assembly; a second permanent magnet assembly spaced from said first magnet assembly and in alignment therewith so as to form a first gap therebetween, with the north pole of one assembly facing the south pole of the other across the gap; each of said magnet assemblies comprising a sandwich construction including a first body of magnetic material including Alnico, a second body of magnetic material including Cobalt in chemical union with a rare earth element and a transition member comprising iron between said first and second bodies, the first body portion of both said magnetic assemblies facing said gap, said first and second bodies having respective interface surfaces facing upon said transition member, said second body interface being larger in area than said first body interface area, whereby magnetic flux density within said gap is optimized.

Claim 15

An open permanent magnetic circuit for developing an optimal degree of flux density within a gap in said circuit, comprising: a first permanent magnet assembly; a second permanent magnet assembly spaced from said first magnet assembly and in alignment therewith so as to form a first gap therebetween, with the north pole of one assembly facing the south pole of the other across the gap; each of said magnet assemblies comprising a sandwich construction including a first body of magnetic material including Alnico, a second body of magnetic material including Cobalt in chemical union with a rare earth element and a transition member comprising iron between said first and second bodies, the first body portion of both said magnetic assemblies facing said gap, said first and second bodies having respective interface surfaces facing upon said transition member, said second body interface being larger in area than said first body interface area, whereby magnetic flux density within said gap is optimized.

Claim 16

A circuit as in claim 13, in which the volume of said first bodies is larger than the volume of said second bodies.

Claim 17

A circuit as in claim 13, in which the area of said second body interface is related to the area of said first body interface as in the flux density of said first body is related to the flux density of said second body.

Claim 18

A circuit as in claim 13, in which a non-magnetic return path is provided for the magnetic flux flowing between the outer most ends of said first and second magnetic assemblies.

Claim 19

A circuit as in claim 13, in which said rare earth is samarium.

Claim 20

In a crossed-field interaction device including cathode means for generating a stream of electrons, microwave circuit means for supporting electromagnetic fields in interaction relationship with said stream of electrons, means for applying electric field between said cathode means and said circuit means, and means for applying a magnetic field perpendicular to said electron field in the region of said stream, the improvement wherein said means for applying a magnetic field comprises: a first and a second permanent magnet assembly on opposing sides of said stream of electrons, the facing ends of said assemblies being of opposite magnetic polarity; each of said magnet assemblies comprising a sandwich construction including a first body of magnetic material including Alnico; a second body of magnetic material including cobalt in chemical union with a rare earth element, and a transition member comprising iron between said first and second bodies, the first body portion of both said magnet assemblies facing said electron stream, said first and second bodies having respective interface surfaces facing upon said transition member, said second-body interface surface being larger in area than said first-body interface area.

Claim 21

In a crossed-field interaction device including cathode means for generating a stream of electrons, microwave circuit means for supporting electromagnetic fields in interaction relationship with said stream of electrons, means for applying electric field between said cathode means and said circuit means, and means for applying a magnetic field perpendicular to said electron field in the region of said stream, the improvement wherein said means for applying a magnetic field comprises: a first and a second permanent magnet assembly on opposing sides of said stream of electrons, the facing ends of said assemblies being of opposite magnetic polarity; each of said magnet assemblies comprising a sandwich construction including a first body of magnetic material including Alnico; a second body of magnetic material including cobalt in chemical union with a rare earth element, and a transition member comprising iron between said first and second bodies, the first body portion of both said magnet assemblies facing said electron stream, said first and second bodies having respective interface surfaces facing upon said transition member, said second-body interface surface being larger in area than said first-body interface area.

Claim 22

The device as in claim 18 in which the return flux path between the outer ends of said first and second magnet assemblies is substantially through non-magnetic media.

Claim 23

A device as in claim 19 in which said permanent magnet assemblies are elongated, and said first bodies are of substantially greater length and volume than said second bodies.

Claim 24

A device as in claim 19 in which said transition member is of substantially less length and volume than said first bodies.

Claim 25

A device as in claim 18 in which said first and second bodies are of cylindrical configuration, and said transition member is in the form of a truncated cone.

Claim 26

In an open magnetic circuit a permanent magnet assembly comprising: a first magnet of high flux density material, said magnet having two ends of opposite magnetic polarity; a second magnet of high coercive force material, said coercive force being greater than that of said first magnet, said high coercive force material having lower flux density than said first magnet, said second magnet having two ends of opposite magnetic polarity, at least one of said second magnet ends being of greater area than, and of opposite polarity to, at least one of said first magnet ends; and an iron transitional member interposed between and contacting both said one second magnet end, and said one first magnet end, the surface area of said member in contact with said second magnet being greater than the surface area of said member in contact with said first magnet end, whereby the flux density immediately adjacent said other, free end of said first magnet is enhanced as compared to comparably-sized magnet assemblies of either of said materials alone.

Claim 27

In an open magnetic circuit a permanent magnet assembly comprising: a first magnet of high flux density material, said magnet having two ends of opposite magnetic polarity; a second magnet of high coercive force material, said coercive force being greater than that of said first magnet, said high coercive force material having lower flux density than said first magnet, said second magnet having two ends of opposite magnetic polarity, at least one of said second magnet ends being of greater area than, and of opposite polarity to, at least one of said first magnet ends; and an iron transitional member interposed between and contacting both said one second magnet end, and said one first magnet end, the surface area of said member in contact with said second magnet being greater than the surface area of said member in contact with said first magnet end, whereby the flux density immediately adjacent said other, free end of said first magnet is enhanced as compared to comparably-sized magnet assemblies of either of said materials alone.

Claim 28

An assembly as in claim 23 in which the surface portions of said iron transitional member facing said one magnet ends are coextensive therewith.

Claim 29

An assembly as in claim 23 in which said first magnet is of substantially greater volume than said second magnet.

Claim 30

An assembly as in claim 25 in which said second magnet of high coercive force is of cobalt in chemical union with a rare earth element.

Claim 31

An assembly as in claim 25 in which said first magnet of high flux density is one of Alnico 5-7 material.

Claim 32

An assembly as in claim 25 in which said first magnet of high flux density is of Alnico 9 material.

Claim 33

A permanent magnet assembly as in claim 23, in which said assembly is aligned along a straight central axis, whereby said enhanced flux density is developed at said other free end in the axial direction.

Claim 34

An open permanent magnetic circuit defining a relatively small working gap and a relatively large non-working gap, and developing an optimal degree of flux density within said working gap, comprising: a first permanent magnet assembly; a second permanent magnet assembly spaced from said first magnet to define said working gap therebetween, with the north pole of one assembly oriented toward the south pole of the other assembly; each of said assemblies comprising a first magnet of high flux density, a second magnet of high coercive force greater than that of said first magnet and of lower flux density than said first magnet, and a transition member comprising iron between and contacting both said magnets; the high flux density first magnet portions of both said assemblies being in opposed relationship across said working gap; said first and second magnets having respective interface surfaces facing upon said transition member, said second magnet-transition member interface being larger in area than said first magnet-transition member interface, whereby magnetic flux density in said working gap is optimized.

Claim 35

An open permanent magnetic circuit defining a relatively small working gap and a relatively large non-working gap, and developing an optimal degree of flux density within said working gap, comprising: a first permanent magnet assembly; a second permanent magnet assembly spaced from said first magnet to define said working gap therebetween, with the north pole of one assembly oriented toward the south pole of the other assembly; each of said assemblies comprising a first magnet of high flux density, a second magnet of high coercive force greater than that of said first magnet and of lower flux density than said first magnet, and a transition member comprising iron between and contacting both said magnets; the high flux density first magnet portions of both said assemblies being in opposed relationship across said working gap; said first and second magnets having respective interface surfaces facing upon said transition member, said second magnet-transition member interface being larger in area than said first magnet-transition member interface, whereby magnetic flux density in said working gap is optimized.

Claim 36

A circuit as in claim 30, in which the area of said second magnet-transition member interface is related to the area of said first body interface as the flux density of said first body is related to the flux density of said second body.

Claim 37

A permanent magnet assembly as in claim 1, in which said first body comprises a magnet element of said magnetic material, and an iron pole piece element having two faces, with one face in contact with said magnet element, and the other face thereof defining said one boundary of said working gap.