US750807A - Telegraph apparatus - Google Patents

Telegraph apparatus Download PDF

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US750807A
US750807A US750807DA US750807A US 750807 A US750807 A US 750807A US 750807D A US750807D A US 750807DA US 750807 A US750807 A US 750807A
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pole
armature
polarity
permanent magnet
core
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/06Electromagnets; Actuators including electromagnets
    • H01F7/08Electromagnets; Actuators including electromagnets with armatures
    • H01F7/121Guiding or setting position of armatures, e.g. retaining armatures in their end position
    • H01F7/122Guiding or setting position of armatures, e.g. retaining armatures in their end position by permanent magnets

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  • the object of my invention is to so arrange I the controlling or actuating electromagnets or electromagnet in connection with a relatively permanent magnetic system as to produce the maximum efiect from given sources of energy acting on the apparatus and in addition to the minor advantages described hereinafter to secure a more sensitive electromagnetic control in instruments of the class described.
  • an instrument constructed in' accordance with my invention will have greater sensitiveness and require less energy for its operation than an instrument constructed in the older forms.
  • M is an elevation of a permanent magnet, having, for example, a south pole at its base and a north pole a at its upper end.
  • a soft-iron core a carrying a coil and being a simple electromagnet.
  • the soft-iron yoke m of the pair of cores s and s both of which also carry coils and are wound so as to produce unlike polarities at their free ends under the influence of a current flowing around their coils.
  • Core s is prolonged at its upper end, and at Z) is pivoted an armature u, also of soft iron, which armature will, of course, under the influence of the permanent magnet. take the position shown in the drawing.
  • the free end of the armature will be then strongly attracted downward when the lower coils are energized, and there will be also a repulsion from a, acting on the induced north pole in the free end of the armature.
  • the permanent magnet need not ordinarily be of great relative strength, merely sufiieient to cause a quick return of the armature to its normal position when the coils cease to act. In this way it takes the place of a return-spring, although a spring can be used, if desired, in any of the well-known methods.
  • One or more of the coils can be dispensed with for certain uses, leaving only one coil on one of the lower couple.
  • the distinctive difference between the apparatus shown and a polar relay is that in a polar relay the armature is adjusted to play between two polar faces of one like polarity, while the armature has a normal induced polarity opposite to both; but in this apparatus the armature has a polarity opposite only to one of the adjacent polar faces, and though in the polar relay the armature has two positions of rest- (1., against either polar face-in my device there is only one rest position.
  • the armature only moves toward the nor- 1 mally like polar face when the magnetic system has been modified by the coils. Reversals of the current, unless, as shown above, these reversals are of considerably greater relative strength, do not affect the instrument nor cause the armature to leave its rest position. It is only when the abnormal current impulse is of considerable strength that there is any action from current impulses of the wrong direction, and it is only when the attractive effect of the lower pair of polar faces is very strong that the armature will be drawn away from its normal position through the influence of a reverse-current impulse.
  • a permanent magnetic system having one of its poles divided into two pole-pieces of like polarity, an armature pivoted on one of said pole-pieces and free to play between the other pole-piece and the other pole of said magnetic system, and a winding adapted when energized to modify the action of said permanent magnetic system, substantially as described.
  • a permanent magnet having one of its poles divided into two pole-pieces of like polarity, an armature pivoted on one of said pole-pieces and free to play between the other pole-piece and the other pole of said magnet, and a winding adapted when energized to modify the action of said permanent magnet substantially as described.
  • a permanent g magnet inducing normally a like polarity in l both poles of the core of an electromagnet, an armature pivoted on one pole of said core and free to play between the other pole of said core and the pole of the permanent magnet of unlike polarity to that of said cores, and a winding on said cores adapted when energized to modify the action of said permanent magnet on said armature, substantially as described.
  • a permanent magnet normally inducing in both poles of the core of an electromagnet a like polarity, an armature pivoted on one pole of said core and free to play between the other pole of said core and a pole-piece of said permanent magnet of unlike polarity to the induced polarity of said cores and normally attracted to said unlike pole-piece of said permanent magnet, and windings adapted when energized to move said armature in opposition to the attraction of said unlike pole-piece of said permanent magnet, substantially as described.
  • a permanent magnetic system a core of an electromagnet both poles of which are induced with like polarity from said permanent magnetic system, an armature pivoted on one pole of said core and normally held away from the other pole of said core by said permanent magnetic system and a winding adapted when energized to move said armature in opposition to such normal position, substantially as described.
  • an electromagnet an armature pivoted on one pole of said electromagnet, a permanent magnet normally attracting said armature and normally inducing like polarities in the poles of said electromagnet, the winding of said electromagnet adapted when energized in one direction electrically to cause said armature to move in opposition to the attraction of said permanent magnet.

Description

No. 750,807. PATENTED FEB. 2, 1904. J. E. GARNEY.
TELEGRAPH APPARATUS.
APPLICATION IILEDIEB. 24, 1903.
n0 MODEL.
WITNESSES //v vE/vmh W A TTOHNE) m: Norms PETERS co, PNOTOAWHGH wAsHmcroN, n c
UNITED STATES Patented February 2, 1904.
PATENT OFFICE.
TELEGRAPH APPARATUS.
SPECIFICATION forming part of Letters Patent N 0. 750,807, dated February 2, 1904.
Application filed February 24,1903. Serial No. 144,665; No model.)
actuated or controlled by electromagnets and is not confined to any special class of apparatus, being applicable, as will appear below,
to sounders, relays, &c., with advantage.
The object of my invention is to so arrange I the controlling or actuating electromagnets or electromagnet in connection with a relatively permanent magnetic system as to produce the maximum efiect from given sources of energy acting on the apparatus and in addition to the minor advantages described hereinafter to secure a more sensitive electromagnetic control in instruments of the class described. In other words, an instrument constructed in' accordance with my invention will have greater sensitiveness and require less energy for its operation than an instrument constructed in the older forms.
Referring to the drawing, M is an elevation of a permanent magnet, having, for example, a south pole at its base and a north pole a at its upper end. To the pole a is secured a soft-iron core a, carrying a coil and being a simple electromagnet. To the south pole of M is attached the soft-iron yoke m of the pair of cores s and s, both of which also carry coils and are wound so as to produce unlike polarities at their free ends under the influence of a current flowing around their coils. Core s is prolonged at its upper end, and at Z) is pivoted an armature u, also of soft iron, which armature will, of course, under the influence of the permanent magnet. take the position shown in the drawing. Suitable stops or contacts are shown; but there is no particular novelty intended in this feature. It is immaterial whether the coils be connected in series or in some other method, the connection depending on questions of expediency. 4 Coil on core a is supposed to be so wound as when energized to strengthen or increase the polarity of the permanent magnet at that point, while coils on s and s are wound so as to pro duce a strong north polarity at 7/ and to divert the south polarity of the permanent magnetic system to s, (or to its free end.) he lower electromagnetic system forms a couple having a soft-iron yoke. The free end of the armature will be then strongly attracted downward when the lower coils are energized, and there will be also a repulsion from a, acting on the induced north pole in the free end of the armature. The permanent magnet need not ordinarily be of great relative strength, merely sufiieient to cause a quick return of the armature to its normal position when the coils cease to act. In this way it takes the place of a return-spring, although a spring can be used, if desired, in any of the well-known methods.
It is obvious that diiferent windings on the core-pieces could be used, which would give in modified degrees the effects sought. Differential winding could be employed or one or more coils could be of higher relative resistance. 1
One or more of the coils can be dispensed with for certain uses, leaving only one coil on one of the lower couple.
A number of constructions can obviously be made embodying the polar distribution of the permanent magnetic system to produce the polarities, as shown.
It will be noticed that while the apparatus has some of the characteristics of a polar relay yet it is not a true polar instrument in that it may be operated by current impulses of either direction of sufficient strength. Its normal use, however, in order to obtain the greatest sensitiveness would be as a polar instrument responding to unidirectional current impulses, when the attractive and repellent influences would act together to produce the maximum effect. A sufficiently-powerful current impulse of the opposite direction would still have power to cause the armature to drop regardless of the permanent magnet and of the effect of the electromagnetic polarity at n. This ca 'iability of acting with an excessive current in a direction opposite to the normal has obvious uses. The distinctive difference between the apparatus shown and a polar relay is that in a polar relay the armature is adjusted to play between two polar faces of one like polarity, while the armature has a normal induced polarity opposite to both; but in this apparatus the armature has a polarity opposite only to one of the adjacent polar faces, and though in the polar relay the armature has two positions of rest- (1., against either polar face-in my device there is only one rest position.
The armature only moves toward the nor- 1 mally like polar face when the magnetic system has been modified by the coils. Reversals of the current, unless, as shown above, these reversals are of considerably greater relative strength, do not affect the instrument nor cause the armature to leave its rest position. It is only when the abnormal current impulse is of considerable strength that there is any action from current impulses of the wrong direction, and it is only when the attractive effect of the lower pair of polar faces is very strong that the armature will be drawn away from its normal position through the influence of a reverse-current impulse.
Having described my invention, what I claim 1. In a telegraph instrument a permanent magnetic system having one of its poles divided into two pole-pieces of like polarity, an armature pivoted on one of said pole-pieces and free to play between the other pole-piece and the other pole of said magnetic system, and a winding adapted when energized to modify the action of said permanent magnetic system, substantially as described.
2. In a telegraph instrument a permanent magnet having one of its poles divided into two pole-pieces of like polarity, an armature pivoted on one of said pole-pieces and free to play between the other pole-piece and the other pole of said magnet, and a winding adapted when energized to modify the action of said permanent magnet substantially as described.
3. In a telegraph instrument a permanent g magnet inducing normally a like polarity in l both poles of the core of an electromagnet, an armature pivoted on one pole of said core and free to play between the other pole of said core and the pole of the permanent magnet of unlike polarity to that of said cores, and a winding on said cores adapted when energized to modify the action of said permanent magnet on said armature, substantially as described.
4. In a telegraph instrument a permanent magnet normally inducing in both poles of the core of an electromagnet a like polarity, an armature pivoted on one pole of said core and free to play between the other pole of said core and a pole-piece of said permanent magnet of unlike polarity to the induced polarity of said cores and normally attracted to said unlike pole-piece of said permanent magnet, and windings adapted when energized to move said armature in opposition to the attraction of said unlike pole-piece of said permanent magnet, substantially as described.
5. In a telegraph instrument a permanent magnetic system, a core of an electromagnet both poles of which are induced with like polarity from said permanent magnetic system, an armature pivoted on one pole of said core and normally held away from the other pole of said core by said permanent magnetic system and a winding adapted when energized to move said armature in opposition to such normal position, substantially as described.
6. In a telegraph instrument an electromagnet, an armature pivoted on one pole of said electromagnet, a permanent magnet normally attracting said armature and normally inducing like polarities in the poles of said electromagnet, the winding of said electromagnet adapted when energized in one direction electrically to cause said armature to move in opposition to the attraction of said permanent magnet.
In testimony whereof I have signed my name to this specification in the presence of two subscribing witnesses.
JOHN EDIVARD ARNEY.
WVitnesses:
V. B. Swm'r'r, E. S. ALEXANDER.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080010706A1 (en) * 2006-05-19 2008-01-10 Mako Surgical Corp. Method and apparatus for controlling a haptic device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080010706A1 (en) * 2006-05-19 2008-01-10 Mako Surgical Corp. Method and apparatus for controlling a haptic device

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