US354781A - goedon - Google Patents

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US354781A
US354781A US354781DA US354781A US 354781 A US354781 A US 354781A US 354781D A US354781D A US 354781DA US 354781 A US354781 A US 354781A
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inductive
resistance
lamps
coil
lamp
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    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05BELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
    • H05B41/00Circuit arrangements or apparatus for igniting or operating discharge lamps
    • H05B41/14Circuit arrangements
    • H05B41/16Circuit arrangements in which the lamp is fed by dc or by low-frequency ac, e.g. by 50 cycles/sec ac, or with network frequencies
    • H05B41/20Circuit arrangements in which the lamp is fed by dc or by low-frequency ac, e.g. by 50 cycles/sec ac, or with network frequencies having no starting switch
    • H05B41/23Circuit arrangements in which the lamp is fed by dc or by low-frequency ac, e.g. by 50 cycles/sec ac, or with network frequencies having no starting switch for lamps not having an auxiliary starting electrode
    • H05B41/232Circuit arrangements in which the lamp is fed by dc or by low-frequency ac, e.g. by 50 cycles/sec ac, or with network frequencies having no starting switch for lamps not having an auxiliary starting electrode for low-pressure lamps

Definitions

  • This invention has for its object to provide improved means for enabling electric are lamps to be used advantageously in parallel circuit with one another or with incandescent r lamps when they are fed with an alternating current.
  • the current will pass without material waste, and having a maximum coeflicient of self-induction, so that if the resistance of the lamp be cut out-as, for instance, when the carbons of the lamp touch or approach too closely together-the amount of current which can then pass will rapidly reach a maximum of but moderate strength in excess of that previously required for the lamp.
  • I may state that with an inductive coil which I have used, and whose true resistance was three'tenths of an ohm, and using an alternat- 0 ing current with eighty-six volts electro-motive force, the current passing through the resistance and an arc lamp was sixteen amperes. On short-circuiting the lamp the current only increased to nineteen amperes, whereas with 4 5 a non-inductive resistance of three-tenths ohm it would have risen to two hundred and eightysix amperes.
  • the inductive resistance may be placed at the point where the branch to the arc lamp leaves the main, in which case it acts instead ofa fusible cutoff in preventing undue heat- 7 ing of the branch wires if a short circuitshould take place. This is an advantage, as it is well .known that fusible cut-offs cannot conveniently be used with arclamps.
  • the shape of the coil should be such that for a given quantity of wirethat is, for a given true resistance-the inductive resistance should be as great as possible-that is, so that with the desired inductive 6 5 resistance the quantity of wire and the true resistance should be as small as possible.
  • Professor Clerk Maxwell has shown. (see Maxwells Electricity 2d Ed. Vol. II, Sec. 706, p. 316) that the coil of maximum self-induc- 7Q tion is a circular coil with the wire wound in a channel of square section the mean diameter of thercoili. 0., the diameter at the center of the wire-channelbeing three-sevenths times the side of the wire-channel.
  • Figure 1 of the drawings annexed shows a cross-section of such an inductive coil formed with a core of cast-iron.
  • Fig. 2 is a side view of the same.
  • Fig. 3 is a diagram view showing such inductive resistance-coils used in a system of electric lighting ,by arc-lamps in parallel circuit with one another or with incandescent lamps.
  • Fig. 4 is a similar diagram View showing two are lamps in each branch circuit.
  • Figs. 1 and 2 are the cast-iron core, which forms the bobbin on which the coils of insulated wire I) are wound.
  • the core is hollow in the center, and is slit to stop the cireulationof currents in theiron.
  • One of the flanges is made with lugs extending from it to enable the coil to be fixed to a wall.
  • the inner sides of the square channel may be covered with a layer, 0, of asbestus, to protect the wire from the heat generated in the iron.
  • An inductive 5 resistance such as shown in the drawings is of a size suitable for being used with are lamps fed with a current of a strength, say, from fifteen to twenty amperes, with one hundred volts on the main. If the core a be of wood, I00
  • the diameter of the coil at the center of the wire-channel being three-sevenths times the side of the wire-channo], or thereabout.

Description

(No Model.) Q 2 Sheets-Sheet 2,
' J. E. H. GORDON.
. ELECTRIC LIGHTING. No. 354,781. Patented Dec. 21, 1886.
N. PETERS, Phnwumu her. wnshin mn, n. n.
UNITED STATES 1 PATENT OFFICE.
JAhIES E. H. GORDON, OF 28 COLLINGHAM PLACE, KENSINGTON, COUNTY OF MIDDLESEX, ENGLAND.
ELECTRIC LIGHTING.
SFECIFICATION forming part of Letters Patent No. 354,781, dated December 21, 1886. Application filed August 21, 1886. Serial No. 211,530. (No model.) Patented in England February 27, 1884, No.4,042.
To all whom it may concern:
Be it known that I, JAMES EDWARD HENRY GORDON, a subject of the Queen of Great Britain, residing at 28 Collingham Place, Kensing= 5 ton, in the county of Middlesex, England, electrical engineer, have invented a certain new and useful Improvement in Electric Lighting, (for which I have received Letters Patent in Great Britain, No. 4,042, dated February 27,
I 1884,) of which the followingis aspecification.
This invention has for its object to provide improved means for enabling electric are lamps to be used advantageously in parallel circuit with one another or with incandescent r lamps when they are fed with an alternating current. For this purpose I interpose in each of the parallel branch circuits, in which an arc lamp is placed, an inductive resistancecoil having a minimum of true resistance, so
that the current will pass without material waste, and having a maximum coeflicient of self-induction, so that if the resistance of the lamp be cut out-as, for instance, when the carbons of the lamp touch or approach too closely together-the amount of current which can then pass will rapidly reach a maximum of but moderate strength in excess of that previously required for the lamp.
I am aware that, broadly, the idea is not new, and that it has been proposed to connect in a branch circuit having an arc-lamp a self inductive reactionary coil for a purpose similar to that above mentioned, and I therefore make no broad claim in this case to such sub- 3 5 ject-matter.
In illustration of my present invention I may state that with an inductive coil which I have used, and whose true resistance was three'tenths of an ohm, and using an alternat- 0 ing current with eighty-six volts electro-motive force, the current passing through the resistance and an arc lamp was sixteen amperes. On short-circuiting the lamp the current only increased to nineteen amperes, whereas with 4 5 a non-inductive resistance of three-tenths ohm it would have risen to two hundred and eightysix amperes.
The inductive resistance may be placed at the point where the branch to the arc lamp leaves the main, in which case it acts instead ofa fusible cutoff in preventing undue heat- 7 ing of the branch wires if a short circuitshould take place. This is an advantage, as it is well .known that fusible cut-offs cannot conveniently be used with arclamps.
In case the wires for several lamps branch from one point, care must be taken not to put the inductive resistances close together. They should be six or eight inches apart at least.
If close, their mutual induction causes the lamps to flicker. The shape of the coil should be such that for a given quantity of wirethat is, for a given true resistance-the inductive resistance should be as great as possible-that is, so that with the desired inductive 6 5 resistance the quantity of wire and the true resistance should be as small as possible. Professor Clerk Maxwell has shown. (see Maxwells Electricity 2d Ed. Vol. II, Sec. 706, p. 316) that the coil of maximum self-induc- 7Q tion is a circular coil with the wire wound in a channel of square section the mean diameter of thercoili. 0., the diameter at the center of the wire-channelbeing three-sevenths times the side of the wire-channel.
Figure 1 of the drawings annexed shows a cross-section of such an inductive coil formed with a core of cast-iron. Fig. 2 is a side view of the same. Fig. 3 is a diagram view showing such inductive resistance-coils used in a system of electric lighting ,by arc-lamps in parallel circuit with one another or with incandescent lamps. Fig. 4 is a similar diagram View showing two are lamps in each branch circuit.
In Figs. 1 and 2,a is the cast-iron core, which forms the bobbin on which the coils of insulated wire I) are wound. The core is hollow in the center, and is slit to stop the cireulationof currents in theiron. One of the flanges is made with lugs extending from it to enable the coil to be fixed to a wall. The inner sides of the square channel may be covered with a layer, 0, of asbestus, to protect the wire from the heat generated in the iron. An inductive 5 resistance such as shown in the drawings is of a size suitable for being used with are lamps fed with a current of a strength, say, from fifteen to twenty amperes, with one hundred volts on the main. If the core a be of wood, I00
coils of the nature hereinbefore described.
Having now particularly described and ascertained the nature of my said invention and in what manner the same is to be performed, I declare what I claim is- In a system of electric lighting in which the arc lamps are arranged in parallel circuit with 1 5 one another or with incandescent lamps, the combination, with the circuits and lamps, of an inductive resistance-coil in each arc-lamp branch, the insulated wire coil of which is circular and is wound in a channel of square 2:
section, or approximately so, the diameter of the coil at the center of the wire-channel being three-sevenths times the side of the wire-channo], or thereabout.
J. E. H. GORDON. Witnesses:
W. J. N ORWOOD, WALTER J. SKERTEN.
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