US338549A - Signor to siemens brothers - Google Patents

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US338549A
US338549A US338549DA US338549A US 338549 A US338549 A US 338549A US 338549D A US338549D A US 338549DA US 338549 A US338549 A US 338549A
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spindle
meter
signor
dial
siemens
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R5/00Instruments for converting a single current or a single voltage into a mechanical displacement
    • G01R5/14Moving-iron instruments

Definitions

  • My invention relates to an electric meter that is to say, an instrument for measuring the electric current in a circuitin which case it maybe termed an electro-dynamometer, or with suitable modifications for measuring the electro-motive force, in which case it may be called a volt-meter.
  • an electro-dynamometer or with suitable modifications for measuring the electro-motive force, in which case it may be called a volt-meter.
  • the principles of action are the same, but the construction is so far modified as to suit two different conditions, the chief modification being in the character of the coils employed.
  • the electrodynamometer a coilconductor of large sectional area and very low resistance is used.
  • the volt-meter coils of fine wire and very high resistance are used.
  • Figure 1 is avertical section
  • Fig. 2 is a sectional plan, of an electro-dynamometer according to my invention
  • Fig. 3 being a front view showing the parts immediately behind the dial, which is supposed to be removed.
  • Fig. 4 is a vertical section
  • Fig. 5 a sectional plan, of the modified form of the instrument constituting a volt-meter
  • Fig. 6 being a transverse section.
  • A is an iron spindle, delicately pivoted atits ends, where there are two iron arms, a a, projecting from it in opposite directions.
  • conducting-coils B consisting for the electrodynamometer, as shown in Figs. 1 and 2, of a few convolutions of copper bar of rectangular section helically wound without contact with each other; but in the volt-meter, as shown in Figs. 4 and 5, consisting of numerous convolutions of fine insulated wire.
  • the spindle A becomes polarized, its armsaa constituting polar extensions of the magnet into which it is converted.
  • the electric current entering by the post 0 passes along a metallic framing, O C" 0", through the coil B, and out by the post D, or in the reverse direction.
  • O C metallic framing
  • the electric current entering by the post 0 passes through a number of convolutions of fineinsulated wire, C C O 0*, wound round a rectangular casing, E, outside the spindle A and its coil B.
  • the current in the parts 0 and G of the rectangular coil is parallel to the arms a a, and tends to deflect them the more the greater the electromotive force.
  • a light index-wire, F which may be of aluminium. It is counterbalanced by an adjustable weight, F, and is bent forward so as to project through a hole in a dial, G.
  • a central spindle, H which can be turned by hand, and which has fixed to its inner end the innermost convolution of a volute spring, K, the outermost convolution of which is connected by an arm, Is, to the index-wire F.
  • an index, M pointing to graduations on the dial. WVhen the instrument is put in circuit, the spindle H is turned by hand until the force of the volute spring K is made to balance the force tending to turn the spindle A by deflecting the arms a a, as can be seen by observing the point of the wire F just vibrating within the hole of the dial through which it passes.
  • the index M will then point to a graduation on the dial G, by which can be ascertained the number of amperes in the current acting on the electro dynamometer or the number of volts in that acting on the volt-meter.
  • a key, N pressed upward by a spring,can be used to put the voltmeter in circuit by pressing down this key by the finger, and thereby bringing into contact two metallic springs, n n, by which the circuit of the instrument is closed.
  • I claim' 1 In an electric meter, the combination of a spindle which is turned by hand, a spring connecting the spindle turned by hand with a magnetic spindle, and a magnetic spindle whereby in each operation the operator in turning the spindle turned by hand puts an' increasing tension upon the spring until it balances the deflecting force of the current, as and for the purposes described.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)

Description

3 Sheets-Shet 1.
(No Model.)
J. S. RAWORTH.
ELECTRIC METER.
No. 338,549. Patented Mar.
(No Model.) 3 Sheets-Sheet 2' J. S. RAWORTH.
ELECTRIC METER.
No. 338,549. Patented Mar. 23, 1886.
bhwwabmus.
N. PETERS Phowhma u lwr, Wuhinglan. D C
(No Model.) 3 Sheets-Sheet 3.
J. S. RAWORTH.
ELEGTRIU METER.
Patented Mar. 23, 1886.
UNiTEn STATES PATENT OFFICE.
JOHN SMITH BAWVORTH, OF MANCHESTER, COUNTY OF LANCASTER, AS-
SIGNOB TO SIEMENS BROTHERS & COMPANY, (LIMITED,) OF 12 QUEEN ANNES GATE, TVESTMINSTER, COUNTY OF MIDDLESEX, ENGLAND.
ELECTRIC METER.
SPECIFICATION forming part of Letters Patent No 338,549. dated March 23,1886.
Application filed February 25, 1885. Serial No. 157,027.
(No model.) Patented in Eng'and May 13. 1884, No. 7,668; in France February 14, 1885, No. 167,046 in Germany February 15,1855, No. 33,950, and in Belgium February 17, 1585, No. 67,920.
To ctZZ whom it may concern.-
Be it known that I, J OHN SMITH RAwoR'rH, a citizen of England, residing at Manchester, in the county of Lancaster, England, have invented a new and useful Electric Meter, (for which I have obtained a patentin Great Britain, dated May 13, 1884, No. 7,668,) of which the following is a specification.
My invention relates to an electric meter that is to say, an instrument for measuring the electric current in a circuitin which case it maybe termed an electro-dynamometer, or with suitable modifications for measuring the electro-motive force, in which case it may be called a volt-meter. For both purposes the principles of action are the same, but the construction is so far modified as to suit two different conditions, the chief modification being in the character of the coils employed. In the one case, for the electrodynamometer a coilconductor of large sectional area and very low resistance is used. In the other case, for the volt-meter coils of fine wire and very high resistance are used.
I will describe both forms, referring to the accompanying drawings, in the several figures of which the same reference-letters are as much as possible employed to indicate corresponding parts.
Figure 1 is avertical section, and Fig. 2 isa sectional plan, of an electro-dynamometer according to my invention, Fig. 3 being a front view showing the parts immediately behind the dial, which is supposed to be removed. Fig. 4 is a vertical section, and Fig. 5 a sectional plan, of the modified form of the instrument constituting a volt-meter, Fig. 6 being a transverse section.
A is an iron spindle, delicately pivoted atits ends, where there are two iron arms, a a, projecting from it in opposite directions. Around the spindle A there are conducting-coils B, consisting for the electrodynamometer, as shown in Figs. 1 and 2, of a few convolutions of copper bar of rectangular section helically wound without contact with each other; but in the volt-meter, as shown in Figs. 4 and 5, consisting of numerous convolutions of fine insulated wire. In either case, when these coils are acted on by electricity, the spindle A becomes polarized, its armsaa constituting polar extensions of the magnet into which it is converted. As shown in Fig. 2, the electric current entering by the post 0 passes along a metallic framing, O C" 0", through the coil B, and out by the post D, or in the reverse direction. In passing along the parts of its circuit Oand (1 which are parallel to the arms a a it tends to deflect them, and so to turn the spindle A partly round with more or less force, according as the current is greater orless. As shown in Figs. 4, 5, and 6, the electric current entering by the post 0 passes through a number of convolutions of fineinsulated wire, C C O 0*, wound round a rectangular casing, E, outside the spindle A and its coil B. In this case also the current in the parts 0 and G of the rectangular coil is parallel to the arms a a, and tends to deflect them the more the greater the electromotive force.
At the front end of the spindle A is fixed a light index-wire, F, which may be of aluminium. It is counterbalanced by an adjustable weight, F, and is bent forward so as to project through a hole in a dial, G. Through this dial passes a central spindle, H, which can be turned by hand, and which has fixed to its inner end the innermost convolution of a volute spring, K, the outermost convolution of which is connected by an arm, Is, to the index-wire F.
On the spindle H, outside the dial G, and protected bya glass, L, there is fixed an index, M, pointing to graduations on the dial. WVhen the instrument is put in circuit, the spindle H is turned by hand until the force of the volute spring K is made to balance the force tending to turn the spindle A by deflecting the arms a a, as can be seen by observing the point of the wire F just vibrating within the hole of the dial through which it passes. The index M will then point to a graduation on the dial G, by which can be ascertained the number of amperes in the current acting on the electro dynamometer or the number of volts in that acting on the volt-meter.
As shown in Figs. 4 and 6, 'a key, N, pressed upward by a spring,can be used to put the voltmeter in circuit by pressing down this key by the finger, and thereby bringing into contact two metallic springs, n n, by which the circuit of the instrument is closed.
No claim is herein made to features described in this application which are claimed in another application, No. 176,931, filed September 12, 1885. v
Having thus described the nature of my invention and the best means I know for carrying it out in practice, I claim' 1. In an electric meter, the combination of a spindle which is turned by hand, a spring connecting the spindle turned by hand with a magnetic spindle, and a magnetic spindle whereby in each operation the operator in turning the spindle turned by hand puts an' increasing tension upon the spring until it balances the deflecting force of the current, as and for the purposes described.
2. The combination of the spindle H, the spring K, connecting the spindle H to the magnetic spindle A, the magnetic spindle A, the indicator F, and the needle M, which turns volute spring K, connected by the arm is to the index-wire, as and for the purposes described. In testimony whereof I have signed my name to this specification, in the presence of two sub scribing witnesses, this 4th day of February, A. D. 1885.
JOHN SMITH RAVORTH.
Witnesses:
WM. S. ROGERS,
105 Oheync l Vulk, S. H. A. SIEMENS, 81 Kensington Garden Square, Bag swarm, London, W.
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