US3681691A

US3681691A - High frequency galvanometer

Info

Publication number: US3681691A
Application number: US71576A
Authority: US
Inventors: Alfred C Mercier
Original assignee: Honeywell Inc
Current assignee: Honeywell Inc
Priority date: 1970-09-11
Filing date: 1970-09-11
Publication date: 1972-08-01
Anticipated expiration: 1989-08-01

Abstract

There is disclosed a high frequency galvanometer with minimal interia about the vibratory axis resulting from a circular suspension bobbinless and distributed coil construction.

Description

United States Patent Mercier Aug. 1, 1972 [54] HIGH FREQUENCY GALVANOMETER [56] References Cited! UNITED STATES PATENTS 3,281,68 3 10/1966 Stefansson et al.

Sept 11, 1970 Primary Examiner-Alfred E. Smith Attorney-Arthur H. Swanson and Lockwood D. Burton 211 App]. No.2 71,576

ABSTRACT 52] us.cl...................@..............324/1s4R,324/96 [571 Int. 1/00, GOlr 3 H00 There is disclosed a high frequency galvanometer with [58] Field of '324/154, 96 minimal interia about the vibratory axis resulting from a circular suspension bobbinless and distributed coil construction.

' 8 Claims, 6 Drawing Figures PATENTEDAuc H912 3,681,691

SHEET 1 [IF 2 INVENTOR. ALFRED C. MERCIER ATTOR N E Y PATENTEDMIE H972 SHEETZUFZ FIG.2 F|G.6

FIG.4 FIG. 5

INVIENTOR. ALFRED C. MERCIER ATTORNEY.

HIGH FREQUENCY GALVANOMETER This invention relates to improvements in high frequency galvanometers. More particularly, the invention relates to a galvanometer with a frequency response operable to at least 25,000 Hz.

A principle failure of prior art galvanometers is their inability to operate at high frequencies in the order of 25,000 Hz. The draw-backs of the prior art invention is due to the relatively large moment of inertia of the movement assembly. The polar moment of inertia taken about the longitudinal axis of the galvanometer has been great due to, among other reasons, the use of unitary coils, bulky bobbins and long, flat ribbons as suspension means.

A flat ribbon does not have an optimum or minimal polar moment of inertia about its central longitudinal symmetrical axis. Therefore, a flat ribbons inertial re sistance to angular acceleration is high relative to a circular ribbon. Since the moment of inertia of a flat ribbon is not optimal from the standpoint of the moment of inertia for a constant cross-sectional area, flat ribbons do not lend themselves to high frequency applications. Another limitation on performance of galvanometers in the prior art is the bobbin itself on which the coil is wound. The entire coil assembly, with the bobbin, a part thereof, is mounted within the galvanometer. The miniaturization with respect to the mass, size and shape of the bobbin is restricted because of the great difficulty in assembling very small com ponents. The mass, size and shape of the bobbin which holds the coil contributes substantially to the total moment of inertia about the longitudinal axis of the galvanometer. In the prior art in order to hold the moment of inertia to a reasonable value, only one bobbin has been used. A single bobbin necessitates the use of a closely wound unitary coil. A unitary coil because of its low ratio of surface area to volume has poor heat transfer characteristics. Hot spots develop readily in such a closely wound coil. Suchhot spots tend to make galvanometers burn out.

Another disadvantage of the flat ribbon type suspension, of the prior art, results in a high spring constant due to the high stresses building up at the edges of the ribbon. A high spring constant reduces the current sensitivity of the galvanometer. The current sensitivity is defined as the ratio of the coil deflection to the input current. For a predetermined deflection, obviously, the greater the spring constant of the suspension the greater will be the required current flow through the coil. A long flat ribbon type suspension reduces the resonant frequency of the galvanometer. Obviously, the longer the suspension member happens to be, the lower the resonant frequency of this member and, therefore, the lower the resonant frequency of the galvanometer.

It is accordingly an object of the present invention to provide an improved galvanometer which obviates the foregoing deficiences of the prior art apparatus.

It is another object of the present invention to provide an improved galvanometer which has a very high frequency response.

It is a further object of the present invention to provide an improved galvanometer which has a minimal moment of inertia about its longitudinal axis.

It is yet another object of the present invention to provide an improved galvanometer which has high current sensitivity as well as very high frequency response.

It is still another object of the present invention to provide an improved galvanometer, as set forth, which is resistant to hot spots and subsequent bumouts.

In accomplishing these and other objects, there has been provided, in accordance with the present inven tion, an improved galvanometer structure which features circular suspension ribbons, a coil wound in two sections attached to the flattened! portions of the circular suspension ribbon. The circular suspension ribbons receive the coil, which has a bobbinless structure, against the flattened portions thereby resulting in a gal vanometer with a very low moment of inertia about its vibratory axis.

A better understanding of the invention may be had from the following detailed description when read in connection with the accompanying drawings, in which;

FIG. 1 is an exploded perspective view of the coil assembly of the galvanometer.

FIG. 2 is a perspective diagram of the vibratory assembly.

FIG. 3 is a perspective diagram of the galvanometer assembly and suspension.

FIG. 4 is an exploded view of the magnetic structure of the galvanometer assembly.

FIG. 5 is a perspective diagram of the complete assembly.

FIG. 6 is an exploded perspective view of the galvanometer and showing a different embodiment of the present invention. I

Referring now to the drawings in more detail, there is shown in FIG. 1, an exploded view of a coil assembly according to the present invention. A moving coil 10 of fine wire is wound in two distributed sections 10A and 10B although together they comprise one continuous coil. An upper suspension wire 20 is formed of circular wire. The lower end of the wire suspension member 20 is flattened; a small hold 16 is formed therein and a pin or peg 12 is inserted in the hole 16 with a portion of the pin extending beyond the flattened end of the wire on opposite sides thereof. A similar lower suspension wire 22, also formed of circular wire, is provided. The upper end of the wire 22 is flattened; and the pin or peg 14 is inserted through the hole 18, with a portion thereof extending from opposite sides of the flattened end of the wire 22.

Referring now to FIG. 2, an end 24 of the coil 10 is wrapped around and soldered to the upper circular suspension wire or ribbon 20. The other end 26 of the coil 10 is similarly wrapped around and soldered to the lower circular suspension wire 22. Thereby, a mechanical and electrical bond is formed between the

ends

24 and 26 of the coil 10 and the

circular suspension wires

20 and 22, respectively. The upper portion of the circular suspension 20 has a mirror 30 affixed thereto. The circular suspension wire 20 to which the mirror 30 is attached is permanently affixed to a rod 32, of FIG. 3, by a suitable method, such as soldering or welding. This upper suspension rod 32 is provided with an enlarged flattened end 33' and is connected to an adjustable yoke 40 by a pin 42 made of an insulating material. The adjustable yoke 40 is provided with a threaded shaft 44 which engages an adjusting nut 46. A guide pin 48 prevents rotation of the assembly with respect to the housing to be described later. The lower circular suspension wire 22 is provided with a similar means for permanently being affixed to a lower suspension rod 34 by a suitable method such as soldering or welding. To the lower suspension wire 22 a paddle 28 is affixed which provided damping for the vibratory assembly of the galvanometer. The lower rod 34 is centered in a bushing 50. On the upper rod 32 a locating disc 36 is provided which surrounds part of the shank of said rod 34. Symmetrically, a locating disc 38 is similarly provided for centering the lower rod 34. In addition, the lower rod 38 is centered in a bushing 50.

A wire, not shown, connects the lower rod 34 to a slip ring 54 which, as shown, is suitably mounted on an insulating member 55.

Referring now to FIG. 4, the oscillitory assembly is encased within an inner tubular body 56 in coaxial arrangement therewith. The inner tubular body 56 is constructed from nonmetallic material such as glass tubing, having an inner bore of capillary dimensions. In a preferred embodiment of the present invention, the inner tubular body 56 is utilized for allowing the outer tubular body 62, FIG. 5, to be fabricated with openings therethrough for reasons which will become obvious hereinbelow. The inner tubular body 56 is filled with a damping fluid 57 to a level position to totally immerse the coil while avoiding contact with the mirror 30. The damping fluid 57 is retained within the inner tubular body 56 by capillary action. The fluid 57, which totally immerses the coil should have a high thermal capacity for removing sufficient thermal energy from the coil, thereby preventing coil hot spots. The damping fluid 57 may be one of many desirable types, such as silicon oil, which may be inserted into the inner body by a conventional hypodermic syringe, not shown. Permanent

magnet pole pieces

58 and 60 are inserted into respective openings in the tubular body 56 and are shaped to provide a magnetic field having lines of flux transverse to the longitudinal axis of the coil assembly 10 located within the tubular housing 56. The outer surfaces of the

permanent magnets

58 and 60 are also characterized to provide a smooth extension of the outer surface of the tubular housing 56 while providing a fluid type seal with the tubular housing 56 to retain the damping fluid 57 therein.

The galvanometer assembly is completed by sliding the protective outer casing 62 over the inner tubular body 56 and aligning a rectangular opening 64 within the protective outer casing 12 for communicating with the mirror 30. An upper cap 66 is then pressed into the top position of the projected outer casing 62 for closing the casing. An aperature 68 within the cap 66 allows the adjustment of the end adjusting nut 46. A kerf 70 is provided in the upper end of the cap 66 for providing a holding point from which rotational adjustment of the entire galvanometer assembly, about its longitudinal axis, may be obtained.

In accordance with the present invention, a wire suspension and 22 of circular cross section is utilized to reduce the polar moment of inertia about the longitudinal axis of the galvanometer to an absolute theoretical minimum. The minimum value of inertia thereby increases the frequency response as a function of this factor to its absolute maximum value. The bobbins of the prior art have been eliminated completely in accordance with the present invention by winding the coil 10 on very small diameter pins 12 and 14 which protrude through the flatten ends of the

circular suspension ribbons

20 and 22. The

pins

12 and 14 add only very insignificantly to the moment of inertia of the assembly. The flattened ends of the

suspension ribbons

20 and 22 allow the coil 10 to be mounted as close to the longitudinal symmetrical axis as is possible. Mounting the coil 10 in this fashion reduces its contribution to the total moment of inertia to a very minimum value. On the small diameter pins 12 and 14, the coil 10 is wound in two sections symmetrically spaced on opposite sides of the

circular suspension wires

20 and 22, thereby dispensing with the use of a bobbin. By distributing the coil 10 on both sides of the

suspension ribbons

20 and 22, the symmetry of the structure is preserved and the moment of inertia which the coil 10 contributes to the total moment of inertia is kept to a minimum. Another advantage of a distributed coil as opposed to a unitary coil, of the same wire size, wire length and number of turns, is that the ratio of the surface area to the volume is greater in a distributed-coil thereby improving the cooling properties of the distributed coil and reducing the occurrence of hotspots.

' formed of a single piece. Whereas the suspension wire means in FIG. 1 includes an upper and a

lower suspension wire

20 and 22, respectively, with flattened ends; in FIG. 6, the suspension is shown as a single continuous wire 70. The wire 70, as before, is essentially a round wire. However, the middle portion 72 thereof is flattened to provide a pair of planar surfaces. Whereas in FIG. 1 the

coils

10a and 10b were attached to the suspension wire means 20 and 22 by small pins which extend through the flattened ends of the suspension wires, in the construction illustrated in FIG. 6, the

coils

10a and 10b may be cemented, respectively, to opposite sides of the flattened portion 72 of the suspension wire 70.

The present invention has a low spring constant since the

suspension wires

20 and 22 are circular in crosssection. For a spring line member with a constant crosssectional area and made of a specific material the spring constant will be a minimum for a circular cross section area. The moments taken about the longitudinal central axis of the spring like member will be at a minimum. Therefore, the length of the

ribbon suspensions

20 and 22 can be reduced with respect to prior art suspensions while retaining the low spring constant which is very desirable from a current sensitivity standpoint. The current sensitivity is defined again as the ratio of the coil deflection to the input current. Since the resonant frequency of a long slender member is inversely proportional to its length, the shorting of the

ribbon suspensions

20 and 22 produces the results of a much higher resonant frequency for the galvanometer assembly than for a long ribbon. This factor, too, increases the frequency response characteristic of the galvanometer.

Therefore the circular cross section of the

circular suspension ribbons

20 and 22, contributes to the high frequency response in two ways, one, by reducing the moment of inertia and, two, by reducing the spring constant and thereby the length of the suspension required.

Thus, it may be seen that there has been provided, in accordance with the present invention, an improved galvanometer structure which is characterized by a very high frequency response, which exhibits a high current sensitivity and which is resistant to so called hot spots.

The embodiments of the invention in which an exclusive property or privilege is claimed are defined as follows:

1. A galvanometer structure comprising a coil of fine wire,

a suspension ribbon means including a first and a second wire suspension member,

said wire suspension members each being circular in cross section and having one flattened end,

said flattened end each having a small aperture formed therein,

pin suspension means inserted through each of said apertures in said flattened ends and protruding from both sides thereof,

said coil of fine wire being formed in two equal but electrically continuous parts,

said parts of said coil being mounted on and supported between said pins and on opposite sides, respectively, of said flattened ends,

opposite ends of said fine wire of said coil being electrically connected to said suspension members, respectively,

means for producing a magnetic field with lines of flux transverse to the longitudinal axis of said coil, and support means connected to said suspension means for supporting said coil in said magnetic field.

2. The invention as set forth in claim 1 and including rod means fastened to said suspension ribbon means whereby said suspension ribbon is mechanically short and exhibits a high resonant frequency.

3. A galvanometer structure as set forth in claim 2 and further including galvanometer mirror means fastened to said rod means.

said flattened end of each of said suspension members having a small aperture formed therein, and

said coil of fine wire being formed into substantially equal and electrically continuous parts,

said parts of said coil being mounted on and supported between said pins and] on opposite sides, respectively, of said flattened ends, with opposite ends of said fine wire of said coil being electrically connected to said first and second suspension 63 2 5321 553? ti s t r ii tme as set forth in clam 5 and including rod means fastened to said suspension ribbon means whereby said suspension ribbon means is mechanically short and exhibits a high resonant frequency.

7. A galvanometer structure as set forth in claim 5 and including means for producing a magnetic field with lines of flux transverse to the longitudinal axis of said coil, and

support means connected to said suspension ribbon means for supporting said coil in said magnetic field.

8. A galvanometer structure as set forth in claim 6 and including galvanometer mirror means fastened to said rod means.

Claims

1. A galvanometer structure comprising a coil of fine wire, a suspension ribbon means including a first and a second wire suspension member, said wire suspension members each being circular in cross section and having one flattened end, said flattened end each having a small aperture formed therein, pin suspension means inserted through each of said apertures in said flattened ends and protruding from both sides thereof, said coil of fine wire being formed in two equal but electrically continuous parts, said parts of said coil being mounted on and supported between said pins and on opposite sides, respectively, of said flattened ends, opposite ends of said fine wire of said coil being electrically connected to said suspension members, respectively, means for producing a magnetic field with lines of flux transverse to the longitudinal axis of said coil, and support means connected to said suspension means for supporting said coil in said magnetic field.

4. The invention as set forth in claim 1 wherein said means for Producing a magnetic field includes a first and second shaped magnetic pole piece located on respective sides of said coil.

5. A galvanometer structure comprising a coil of fine wire, a suspension ribbon means including a first and a second suspension member, said first and second suspension members each being circular in cross section and having one flattened end, said flattened end of each of said suspension members having a small aperture formed therein, and pin suspension means inserted through each of said apertures in said flattened ends and protruding from both sides thereof, said coil of fine wire being formed into substantially equal and electrically continuous parts, said parts of said coil being mounted on and supported between said pins and on opposite sides, respectively, of said flattened ends, with opposite ends of said fine wire of said coil being electrically connected to said first and second suspension members, respectively.

6. A galvanometer structure as set forth in clam 5 and including rod means fastened to said suspension ribbon means whereby said suspension ribbon means is mechanically short and exhibits a high resonant frequency.

7. A galvanometer structure as set forth in claim 5 and including means for producing a magnetic field with lines of flux transverse to the longitudinal axis of said coil, and support means connected to said suspension ribbon means for supporting said coil in said magnetic field.