US1449878A - Modulator - Google Patents
Modulator Download PDFInfo
- Publication number
- US1449878A US1449878A US528846A US52884622A US1449878A US 1449878 A US1449878 A US 1449878A US 528846 A US528846 A US 528846A US 52884622 A US52884622 A US 52884622A US 1449878 A US1449878 A US 1449878A
- Authority
- US
- United States
- Prior art keywords
- winding
- inductance
- modulator
- current
- windings
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 238000004804 winding Methods 0.000 description 30
- 239000000696 magnetic material Substances 0.000 description 6
- 230000008859 change Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 5
- 230000005415 magnetization Effects 0.000 description 4
- 230000011664 signaling Effects 0.000 description 2
- XUKUURHRXDUEBC-KAYWLYCHSA-N Atorvastatin Chemical compound C=1C=CC=CC=1C1=C(C=2C=CC(F)=CC=2)N(CC[C@@H](O)C[C@@H](O)CC(O)=O)C(C(C)C)=C1C(=O)NC1=CC=CC=C1 XUKUURHRXDUEBC-KAYWLYCHSA-N 0.000 description 1
- 235000013382 Morus laevigata Nutrition 0.000 description 1
- 244000278455 Morus laevigata Species 0.000 description 1
- 230000009471 action Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000003475 lamination Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000008520 organization Effects 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03C—MODULATION
- H03C1/00—Amplitude modulation
- H03C1/08—Amplitude modulation by means of variable impedance element
- H03C1/10—Amplitude modulation by means of variable impedance element the element being a current-dependent inductor
Definitions
- My present invention relates to modulators of high freqiiency current, and more particularly to modulators of the type commonly known as magnetic amplifiers.
- the object of my invention is to provide a magnetic modulator which will serve to gontrol the amplitude of the antenna current without appreciably varying the tuning of the antenna.
- I provide a core of magnetic material having two magnetizing coils surrounding two legs of a preferably closed core of magnetic material. I surround these two coils by a winding made up of two portions wound in opposite directions.
- the winding By arranging the winding for the high frequency current in this way the inductance of the winding is greatly reduced and becomes only a small portion of the total inductance of the oscillating circuit.
- small variations in the inductance of the winding with changes in the magnetization of the magnetic core produce such small percentage changes in the total inductance of the circuit that they do not appreciably affect the tuning.
- the high frequency losses in the core vary greatly with variations in the magnetization and as a result the device acts principally as a variable resistance in the antenna circuit.
- Fig. 1 shows diagrammatically the application of my invention to a radio telephone transmitting system
- Fig. 2 is a view of the modulator with a portion of the windings broken away.
- my improved modulator comprises a pair of coils 1 and 2 surrounding the two legs 3 and 4 of a continuous magnetic core made of thin laminations.
- a winding Surrounding the coils 1 and 2 is a winding made up of two portions 5 and 6 wound in opposite directions.
- the winding 5, 6 is connected in series with a radiating antenna 7 which is supplied with high frequency current from a source 8 through the usual coupling transformer 9.
- the source 8 may be of any form desired, either a high frequency altern ator,'an arc generator, or a vacuum tube generator.
- Modulation of the antenna current is effected by supplying a telephone current by means of the transmitter 10 and local battery 11 to the windings 1 and 2.
- the inductance of the modulator may be made to represent a very small percentage of the total inductance of the circuit.
- the modulating effect will not be appreciably reduced since the individual fields are established. by the two halves of the high frequency winding, thus making it possible to vary the effective resistance of the winding by varying the permeability of the core.
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Coils Or Transformers For Communication (AREA)
- Transmitters (AREA)
Description
Mar. 27, 1923.
- 1,449,878. E. AUSTIN.
MODULATOR.
FILED JAN-12,1922
Fig. I.
Inventor:
Edward Austin,
Hi s Att, orhe g.
Patented Mar. 27, 1923.
UNITED STATES PATENT OFFICE.
EDWARD AUSTIN, OF SCHENECTADY, NEW YORK, ASSIGNOR TO GENERAL ELECTRIC COMPANY, A CORPORATION OF NEW YORK.
MODULATOR.
Application filed January 12, 1922. Serial No. 528,846.
To all whom it may concern:
Be it known that I, EDWARD AUsTIN, a citizen of the United States, residing at Schenectady, in the county of Schenectady,
State of New York, have invented certain new and useful Improvements in Modulators, of which the following is a specification. 5
My present invention relates to modulators of high freqiiency current, and more particularly to modulators of the type commonly known as magnetic amplifiers.
Devices of this general type as used in. the past and as described, for example, in United States patent to Alexanderson, 1,206,643, have depended for their action upon the varying inductance of a winding supplied with high frequency current under variations in the magnetization of a core of magnetic material with which the winding is associated.
When such a device has its high frequency windings connected in series with the antenna of a radio transmitting system the effect, if operated in accordance with past practice is to vary the tuning of the antenna. In case a source of high frequency current such a vacuum tube generator is employed, the frequency of which is largely determined by the antenna tuning, this results in a wide change in the wave length transmitted without any appreciable control of the amplitude of the radiated waves. For radio telephony, however, particularly with short wave lengths, it is regarded as better practice to maintain the wave length constant and effect the transmission by varying the amplitude of or modulating the antenna current in accordance with the telephone current.
The object of my invention is to provide a magnetic modulator which will serve to gontrol the amplitude of the antenna current without appreciably varying the tuning of the antenna.
In carrying my invention into effect I provide a core of magnetic material having two magnetizing coils surrounding two legs of a preferably closed core of magnetic material. I surround these two coils by a winding made up of two portions wound in opposite directions. By arranging the winding for the high frequency current in this way the inductance of the winding is greatly reduced and becomes only a small portion of the total inductance of the oscillating circuit. Hence small variations in the inductance of the winding with changes in the magnetization of the magnetic core produce such small percentage changes in the total inductance of the circuit that they do not appreciably affect the tuning. .The high frequency losses in the core, however, vary greatly with variations in the magnetization and as a result the device acts principally as a variable resistance in the antenna circuit.
' The novel features which I believe'to be characteristic of my invention are set forth with particularity in theappended claims. My invention itself, however, both as to its organization and method of operation will best be understood by reference to the following description taken in connection with the accompanying drawing in which Fig. 1 shows diagrammatically the application of my invention to a radio telephone transmitting system, and Fig. 2 is a view of the modulator with a portion of the windings broken away.
As indicated in the drawing, my improved modulator comprises a pair of coils 1 and 2 surrounding the two legs 3 and 4 of a continuous magnetic core made of thin laminations. Surrounding the coils 1 and 2 is a winding made up of two portions 5 and 6 wound in opposite directions. The winding 5, 6 is connected in series with a radiating antenna 7 which is supplied with high frequency current from a source 8 through the usual coupling transformer 9. The source 8 may be of any form desired, either a high frequency altern ator,'an arc generator, or a vacuum tube generator. Modulation of the antenna current is effected by supplying a telephone current by means of the transmitter 10 and local battery 11 to the windings 1 and 2.
While it is possible to vary the antenna current by varying the tuning the control which is obtained in this way over the range necessary for, ;efi'ecting satisfactory voice modulation of the antenna current is nonlinear. Such control therefore induces dis tortion in'the current transmitted and this distortion is increased by the non-linear detuning effect of the receiver. In the case of short wave radio transmitters the inductance of the circuit being comparatively low, a
small change in the inductance of the modulator will produce considerable dlstortlon if the inductance of the modulator QO L- tutes an appreciable percentage of the total inductance of the oscillating circuit. By the arrangement which I have described it will be apparent that the inductance of the modulator may be made to represent a very small percentage of the total inductance of the circuit. The modulating effect, however, will not be appreciably reduced since the individual fields are established. by the two halves of the high frequency winding, thus making it possible to vary the effective resistance of the winding by varying the permeability of the core. The resultant high frequency field, however, which determines the inductance will be very low and the per centage change in this inductance by reason of changes in the magnetization of the core will also be lower by reason of the differential winding. Hence for a large change in the magnetizing current the percentage change in the total oscillating circuit. inductance will be very low and the distortion will be reduced to a minimum.
What I claim as new and desire to secure by Letters Patent of the United States,
1. The combination in a modulator of a closed core of magnetic material having two subtantially parallel legs, winding on each of said legs and a winding surrounding the windings on both of said legs, said last-mentioned winding being composed of two portions wound in opposite directions.
2. The combination in a modulating system of a closed core ofl magnetic material having two substantially parallel legs, windings on each of said legs, means for supplying a modulating current to said windings, a winding surrounding the windings on both of said legs, said last mentioned winding being composed of two portions wound in opposite directions, and means for supplying high frequency currents to said last mentioned winding.
3. The combination in a signaling system of a closed core of magnetic material having two substantially parallel legs, windings on each of said legs, means for supplying audio frequency signaling currents to said windings, a winding surrounding the windings on both of said legs, said last-mentioned winding being composed of two portions wound in opposite directions, a transmitting circuit in which the last-mentioned windings are included and means for supplying high frequency currents to said transmitting circuit.
In witness whereof, I have hereunto set
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US528846A US1449878A (en) | 1922-01-12 | 1922-01-12 | Modulator |
FR556023D FR556023A (en) | 1922-01-12 | 1922-09-13 | Improvements in means of controlling high frequency currents |
GB248/23A GB191723A (en) | 1922-01-12 | 1923-01-03 | Improvements in or relating to magnetic modulators for high frequency currents |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US528846A US1449878A (en) | 1922-01-12 | 1922-01-12 | Modulator |
Publications (1)
Publication Number | Publication Date |
---|---|
US1449878A true US1449878A (en) | 1923-03-27 |
Family
ID=24107426
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US528846A Expired - Lifetime US1449878A (en) | 1922-01-12 | 1922-01-12 | Modulator |
Country Status (3)
Country | Link |
---|---|
US (1) | US1449878A (en) |
FR (1) | FR556023A (en) |
GB (1) | GB191723A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2888637A (en) * | 1955-03-17 | 1959-05-26 | Sperry Rand Corp | Radio frequency or carrier type transverse magnetic amplifier using squarewave power |
US3219918A (en) * | 1962-05-25 | 1965-11-23 | H & T Electrical Products | Current limiting apparatus |
-
1922
- 1922-01-12 US US528846A patent/US1449878A/en not_active Expired - Lifetime
- 1922-09-13 FR FR556023D patent/FR556023A/en not_active Expired
-
1923
- 1923-01-03 GB GB248/23A patent/GB191723A/en not_active Expired
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2888637A (en) * | 1955-03-17 | 1959-05-26 | Sperry Rand Corp | Radio frequency or carrier type transverse magnetic amplifier using squarewave power |
US3219918A (en) * | 1962-05-25 | 1965-11-23 | H & T Electrical Products | Current limiting apparatus |
Also Published As
Publication number | Publication date |
---|---|
GB191723A (en) | 1924-02-21 |
FR556023A (en) | 1923-07-10 |
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