US1297188A - System for amplifying variable currents. - Google Patents
System for amplifying variable currents. Download PDFInfo
- Publication number
- US1297188A US1297188A US11512A US1151215A US1297188A US 1297188 A US1297188 A US 1297188A US 11512 A US11512 A US 11512A US 1151215 A US1151215 A US 1151215A US 1297188 A US1297188 A US 1297188A
- Authority
- US
- United States
- Prior art keywords
- grid
- circuit
- potential
- frequency
- current
- 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
Images
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04L—TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
- H04L25/00—Baseband systems
- H04L25/02—Details ; arrangements for supplying electrical power along data transmission lines
- H04L25/06—Dc level restoring means; Bias distortion correction ; Decision circuits providing symbol by symbol detection
- H04L25/067—Dc level restoring means; Bias distortion correction ; Decision circuits providing symbol by symbol detection providing soft decisions, i.e. decisions together with an estimate of reliability
Definitions
- invention also includes means for securing selectivity in detecting signals, for example, for receiving systems in radio-telegraphy.
- My invention includes a combination of two or more electron discharge devices connected in cascade, the electrode circuit of one device being connected to a resistance, a reactance or transformer across which is connected the grid circuit of a second device.
- My invention also includes other novel features, such as means for integrating high frequency wave trains into impulses or waves of lower frequency, tuning both for group frequency as well as wave frequency,
- Fig. 2 illustrates a tuned system" containing a condenser for integrating oscillations
- Fig. 3 is a diagram illustrating an integrating efl'ect secured with a condenser with the grid circuit.
- an electron discharge device A comprises a gas-tight envelop 1 which may consist of quartz orglass, preferably material pervious to ultra-violet light, and into which are sealed in the usual manner an electron-emitting cathode 2, a cooperating anode 3 and a discharge-controlling grid 4 ordinarily located between the cathode and anode.
- the cathode in this case consists of potassium, sodium; or other metal which emits electrons when illuminated by means of a source of light 5, which may be an incandescent lamp as illustrated or a suitable arc lamp.
- a monochromatic source of light, such as mercury vapor arc in a quartz or glass envelop is advantageous in I giving electrons of uniform velocity.
- anode preferably consists of tungsten and is deprived of gas by electron bombardment during the exhausting process, the envelop beingsealed when the, anode has been thoroughly freed from gas and the pressure in the envelop has been reduced to a value at which no appreciable gas ionization can occur.
- the grid '4 and the cathode 2 are connected respectively by con ductors 6 and 7 to the secondary of a trans former 8, the primary of which is located in circuit with an antenna 9.
- a grounded condenser 10 In the an-' tenna circuit there may be located a grounded condenser 10 but the antenna con:
- a battery 12 having its negative terminal is included a local source of energy, such as sistance 13.
- a local source of energy such as sistance 13.
- sistance 13 In place of this resistance a sufficiently high inductance may be used,
- a second electron-discharge device B having a cathode 14, adapted to be heated to incandescence by means of a battery 15, or other convenient source.
- the grid 16 and the cathode 14 are connected to the resistance 13 respectively by conductors 17 and 18, through a reversing switch 19.
- a local source of energy 22 In the electrode circuit 20, 21, of the device B is included a local source of energy 22 and an electrical detecting device 23, such as any of the known forms of electro-magnetic' recorders or a telephone. In shunt therewith may be placed a condenser 24. In some cases a battery 25 or other source of potential may be included in the 1 grid circuit 17.
- the discharge device A which may have relatively large distances between the grid and the electrodes, is made very sensitlve to changes of grid voltages.
- a comparatively feeble impulse received from the antenna 8 will be accompanied by a change in the current from the local source 12 through the resistance 13.
- the current increases when ;a positive Wave is superimposed on the negatlve grid potential.
- the current flowing through the resistance 13 will be greater than the current received from the antenna, and, therefore, will produce greater variations in the static charge of the grid 16 of the device .B than were originally received by the grid 4-of the device A.
- these potentials may be used to produce greatly amplified signal current.
- the stronger currents flowing in the electrode circuit of the device A can be used to vary the flow of electron discharge current between the cathode 14 and the anode 26 of the discharge device B'which is adapted to co trol relatively a greater amount of energy than the device A although not nece sarily so sensitive to minute voltage changes as the device A.
- the switch 19 is set so as to connect the positive terminal of the IQSlStEIDCG 13to the grid circuit 17, containing. means for making the grid 16 negative, an increase of plate current of device A will produce an increase in the plate current of device B. 1
- the converse is the case when the connections are reversed.
- the variations in the electrode or plate circuit constitutes further amplification of the original signal currents and may be made of great enough to operate an electromagnetic instrument 23, such as a telegraph relay, or in any convenient way to indicate the signals.
- an ordinary telephone may be connected to'the terminals of the conductors 20, 21, to detect the amplified signals.
- Fig. 2 The system shown in Fig. 2 is in some respects similar to the system shown in Fig. 1, for example, in the character of the discharge device used, and therefore need not be again described in detail.
- Each device has a heated cathode 0 .and an unheated anode a, both of which may consist of tungsten.
- ber of discharge devices have been shown connected in cascade and one of the devices is provided with means for integrating the high frequency oscillations of the wave trains so as to transmit in its plate circuit variable current which when transformed to an alternating current will correspond in frequency with the group frequency of the wave trains.
- Such a system permits progressive tuning in each grid circuit whereby the receiving systemwill select only signals having both a predetermined-oscillation frequency and group frequency. This method of operation will be better understood by first considering the connections and then tracing through the method of operation.
- the grid 27 of the discharge tube M is connected to the secondary of the loosely coupled air core transformer 28.
- the primary of the transformer is included in a grounded antenna similar to that shown in Fig. 1.
- a source of potential 30 is included in the grid circuit 29 and across the transformer secondary is connected a condenser 31. which preferably is made adjustable.
- the oscillating circuit constituted thereby may be made resonant to a desired frequency andtherefore will be largely opaque to disturbances.
- the grid will be influenced only to a slight extent by frequencies differing from the desired predetermined frequency.
- oscillations in the plate circuit 32 similar to those in the grid circuit.
- These oscillations having been produced by a local source of current 33 may be stronger than the received oscillations. They are impressed on another In the system shown in Fig. 2 a num- I oscillating circuit 34, 35. by means of an air 4 cor transformer 36.
- the circuit 34, 35 is likewise adjustedto be opaque to undesired oscillations by properly adjusting the con denser 37.
- the oscillations produced in. the plate circuit 38 of the device R by a local source of energy 39 are again transmitted to also tuned, by an air core transformer 41.
- condenser 43 which is shunted by a high resistance 44 and battery 45 which preferably has its negative terminal connected to the grid 46. Both theresistance and the battery are provided with an adjustable shunt 47 so that the potential of the battery and amount of resistance may be both varied or, in fact, entirely eliminated. Even when the grid 46 is not maintained at a predetermined potential it will assume some negative potential as it receives electrons from the cathode 0 and its potential is determined by the surface of the grid 46 and the rate at which the chargemay leak of]? from the condenser plates.
- the capacity of the condenser 43, the potential of the battery'45, if one is used,and the resistance 44 should be so chosen that the grid 46 will have resumed its equilibrium charge before the next wave train is impressed on 1t.
- a variable current will tend to flow therein having a frequency equal to the group frequency of the signals received from the antenna and also having a high frequency component.
- the high frequency component of this current may be eliminated bymaklng the circuit responsive or resonant only to the low frequency. This may be done by pro viding the transformer 52 with an iron core so as to introduce considerable inductance into the circuit 51 and also by shunting the primary circuit of the transformer with a condenser 53.
- a relatively smooth low frequency alternating current will flow in the secondary circuit 54 which may be tuned for the frequency to be selected by an adjustable condenser 55.
- the selectivity of the system thus is made very great as it is opaque not only. to dlsturbances having a different frequency than the oscillations to be received but is also opaque to aerial signals having a different group frequency.
- the number of circuits connected thus in series or in cascade may be increased to any desired number.
- the oscillations of the circuit 54 are impressed on a grid 56, in circuit with which preferably is a source of potential 57.
- the currents in the plate circuit 58 produced by a local source 59 are varied as already exp ained by variations of grid potential.
- the amplified and selected signals may be recorded or detected by any.
- the grids of .tubes M and B may consist of fine wire, closely spaced, the grid of the device S of coarse wire, more widely spaced, and the grid 56 of tube T of fine wire widely spaced but these relations are not essential.
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Elimination Of Static Electricity (AREA)
Description
I. LANGMUIR.
SYSTEM FOR AMPLIFYING VARIABLE CURRENTS.
APPLICATION FILED MAR. 2. I915.
Patented Mar. 11, 1919.
Fig. 5.
Witnesses: Inventor", v $244 47%. Ir-Vin Lan muir', -i i Momey] UNITED STATES" PATENT oFFIoE.
COMPANY, A CORPORATION OF NEW YORK.
SYSTEM FOR A MPLIFYING VARIABLE CURRENTS.
Original application filed October 29, 1913, Serial No. 797,955.
1915. Serial No. 11,51&
To all whom it may concern:
Be it known that I, IRVING LANGMUIR, a citizen of. the United States, residing at Schenectady, county of Schenectady, State of New York, have invented certain new andv useful Improvements in Systems for discharge apparatus utilizing an electron discharge and comprises novel systems of I connection whereby weak variable currents may be reproduced as stronger current-s. My
invention also includes means for securing selectivity in detecting signals, for example, for receiving systems in radio-telegraphy.
The electron-discharge device preferably utilized in accordance with my invention comprises an incandescent, or other electron-emitting cathode, a cooperating gasfree anode and ,a' discharge-controlling conductor, commonly called the. grid, and an inclosing envelop, the space in. the envelop being evacuated below the pressure at which appreciable gas ionization by collision with electrons can occur, but it is to be under stood that my invention is not-limited to this particular apparatus.
My invention includes a combination of two or more electron discharge devices connected in cascade, the electrode circuit of one device being connected to a resistance, a reactance or transformer across which is connected the grid circuit of a second device. My invention also includes other novel features, such as means for integrating high frequency wave trains into impulses or waves of lower frequency, tuning both for group frequency as well as wave frequency,
and other features pointed out with greater particularity in the appended claims.
A more detailed understanding of my invention may be had from the following description taken in connection with the ac companying drawings, which .show for the purpose of illustration my invention as applied to receivmg systems of wireless telegraphy. Flgure 1 illustrates a system Specification of Letters Patent.
Divided and this application filed March 2,
containing a device having an illuminated IRV'ING LANGMUIR, on SCHENECTALDY, NEW YORK, nssronon T0 GENERAL ELECTRIC Patented Mar. 11, 1919.
cathode; Fig. 2 illustrates a tuned system" containing a condenser for integrating oscillations, and Fig. 3 is a diagram illustrating an integrating efl'ect secured with a condenser with the grid circuit. s
In Fig. 1 an electron discharge device A comprises a gas-tight envelop 1 which may consist of quartz orglass, preferably material pervious to ultra-violet light, and into which are sealed in the usual manner an electron-emitting cathode 2, a cooperating anode 3 and a discharge-controlling grid 4 ordinarily located between the cathode and anode. The cathode in this case consists of potassium, sodium; or other metal which emits electrons when illuminated by means of a source of light 5, which may be an incandescent lamp as illustrated or a suitable arc lamp. A monochromatic source of light, such as mercury vapor arc in a quartz or glass envelop is advantageous in I giving electrons of uniform velocity. The
anode preferably consists of tungsten and is deprived of gas by electron bombardment during the exhausting process, the envelop beingsealed when the, anode has been thoroughly freed from gas and the pressure in the envelop has been reduced to a value at which no appreciable gas ionization can occur. The grid '4 and the cathode 2 are connected respectively by con ductors 6 and 7 to the secondary of a trans former 8, the primary of which is located in circuit with an antenna 9. In the an-' tenna circuit there may be located a grounded condenser 10 but the antenna con:
nections and structure may be the usual ones forming no part of my present invention. In the grid circuit 7, there is pref erably included, a source of potential 11,
=;su ch as a battery which preferably is connected .to maintain the grid at a definite negativepotential'," but in some cases the grid may be maintained at a positive potential.
In the circuit connecting the cathode and the anode, also known as the plate circuit,
a battery 12, having its negative terminal is included a local source of energy, such as sistance 13. In place of this resistance a sufficiently high inductance may be used,
.0004 inch, the turns being closely spaced.
To the terminalsof the resistance is connected a second electron-discharge device B, having a cathode 14, adapted to be heated to incandescence by means of a battery 15, or other convenient source. The grid 16 and the cathode 14 are connected to the resistance 13 respectively by conductors 17 and 18, through a reversing switch 19. In the electrode circuit 20, 21, of the device B is included a local source of energy 22 and an electrical detecting device 23, such as any of the known forms of electro-magnetic' recorders or a telephone. In shunt therewith may be placed a condenser 24. In some cases a battery 25 or other source of potential may be included in the 1 grid circuit 17. v
In the system described the discharge device A, which may have relatively large distances between the grid and the electrodes, is made very sensitlve to changes of grid voltages. The fact that the electrons are emitted by the cathode at uniform velocity contributes to its sensitiveness. A comparatively feeble impulse received from the antenna 8 will be accompanied by a change in the current from the local source 12 through the resistance 13. The current increases when ;a positive Wave is superimposed on the negatlve grid potential. The current flowing through the resistance 13 will be greater than the current received from the antenna, and, therefore, will produce greater variations in the static charge of the grid 16 of the device .B than were originally received by the grid 4-of the device A. Hence, these potentials may be used to produce greatly amplified signal current. In other words, the stronger currents flowing in the electrode circuit of the device A can be used to vary the flow of electron discharge current between the cathode 14 and the anode 26 of the discharge device B'which is adapted to co trol relatively a greater amount of energy than the device A although not nece sarily so sensitive to minute voltage changes as the device A. When the switch 19 is set so as to connect the positive terminal of the IQSlStEIDCG 13to the grid circuit 17, containing. means for making the grid 16 negative, an increase of plate current of device A will produce an increase in the plate current of device B. 1 The converse is the case when the connections are reversed. The variations in the electrode or plate circuit constitutes further amplification of the original signal currents and may be made of great enough to operate an electromagnetic instrument 23, such as a telegraph relay, or in any convenient way to indicate the signals.
In some cases an ordinary telephone may be connected to'the terminals of the conductors 20, 21, to detect the amplified signals.
The system shown in Fig. 2 is in some respects similar to the system shown in Fig. 1, for example, in the character of the discharge device used, and therefore need not be again described in detail. Each device has a heated cathode 0 .and an unheated anode a, both of which may consist of tungsten. ber of discharge devices have been shown connected in cascade and one of the devices is provided with means for integrating the high frequency oscillations of the wave trains so as to transmit in its plate circuit variable current which when transformed to an alternating current will correspond in frequency with the group frequency of the wave trains. Such a system permits progressive tuning in each grid circuit whereby the receiving systemwill select only signals having both a predetermined-oscillation frequency and group frequency. This method of operation will be better understood by first considering the connections and then tracing through the method of operation.
The grid 27 of the discharge tube M is connected to the secondary of the loosely coupled air core transformer 28. The primary of the transformer is included in a grounded antenna similar to that shown in Fig. 1. In the grid circuit 29 is included a source of potential 30 and across the transformer secondary is connected a condenser 31. which preferably is made adjustable.
Bv properly proportioning th inductance.
of the transformer secondary and the capac-, ity of the condenser, the oscillating circuit constituted thereby may be made resonant to a desired frequency andtherefore will be largely opaque to disturbances. Hence the grid will be influenced only to a slight extent by frequencies differing from the desired predetermined frequency. As already explained the variations in the grid potential, which is preferably negative, produced,
by the impressed oscillations result in oscillations in the plate circuit 32 similar to those in the grid circuit. These oscillations having been produced by a local source of current 33 may be stronger than the received oscillations. They are impressed on another In the system shown in Fig. 2 a num- I oscillating circuit 34, 35. by means of an air 4 cor transformer 36. The circuit 34, 35, is likewise adjustedto be opaque to undesired oscillations by properly adjusting the con denser 37. The oscillations produced in. the plate circuit 38 of the device R by a local source of energy 39 are again transmitted to also tuned, by an air core transformer 41.
It will be noted that by thus tuning successive-circuits the undesired-oscillations are reduced in each case in geometric proportion.
In the present case, I secure as a novel feature tuning for both oscillation frequency and group frequency, as will be explained.
The grid circuit 42 of the discharge tube S.
contains a condenser 43 which is shunted by a high resistance 44 and battery 45 which preferably has its negative terminal connected to the grid 46. Both theresistance and the battery are provided with an adjustable shunt 47 so that the potential of the battery and amount of resistance may be both varied or, in fact, entirely eliminated. Even when the grid 46 is not maintained at a predetermined potential it will assume some negative potential as it receives electrons from the cathode 0 and its potential is determined by the surface of the grid 46 and the rate at which the chargemay leak of]? from the condenser plates. When the grid is positively charged it will take up electrons at a rate varying with the degree of positive charge and when the grid is negatively charged the rate at which it absorbs electrons decreases with the degree of negative charge until a value is reached at which no 4 the ordinates are grid potentials and the abscissa represents time. The actual number of oscillations in each group, of course, will be much greater than indicated in Fig. 3. When the oscillations are superimposed on the grid, assuming its potential to be 37, Fig. 3, a positive wave 48 will cause it to take up more electrons, which are not discharged during the succeeding negative wave. Each successive wave adds its increment to the negative charge which thus accumulates on the grid'and the plate of the condenser: connected to it. After a certain number'of oscillations have thus been received the grid has received such a negative charge that it no longer takes up more electrons than it loses. When the wave train ceases, the added negative charge leaks ofi asindicated by the line 50, until the grid potential again assumes its original value p.
The capacity of the condenser 43, the potential of the battery'45, if one is used,and the resistance 44 should be so chosen that the grid 46 will have resumed its equilibrium charge before the next wave train is impressed on 1t.
As the current in the plate circuit 51 of thetube S is determined by the, grid charge, a variable current will tend to flow therein having a frequency equal to the group frequency of the signals received from the antenna and also having a high frequency component. The high frequency component of this current may be eliminated bymaklng the circuit responsive or resonant only to the low frequency. This may be done by pro viding the transformer 52 with an iron core so as to introduce considerable inductance into the circuit 51 and also by shunting the primary circuit of the transformer with a condenser 53. A relatively smooth low frequency alternating current will flow in the secondary circuit 54 which may be tuned for the frequency to be selected by an adjustable condenser 55.
The selectivity of the system thus is made very great as it is opaque not only. to dlsturbances having a different frequency than the oscillations to be received but is also opaque to aerial signals having a different group frequency. The number of circuits connected thus in series or in cascade may be increased to any desired number.
In the system illustrated the oscillations of the circuit 54 are impressed on a grid 56, in circuit with which preferably is a source of potential 57. The currents in the plate circuit 58 produced by a local source 59 are varied as already exp ained by variations of grid potential. The amplified and selected signals may be recorded or detected by any.
suitable form of device as indicated at 60.
The grids of .tubes M and B may consist of fine wire, closely spaced, the grid of the device S of coarse wire, more widely spaced, and the grid 56 of tube T of fine wire widely spaced but these relations are not essential.
What I claim as new -and desire to secure by Letters Patent of the United States, is,-
1. The combination in an amplifying system of an electron discharge device having grid and plate circuits, means for supplying currents to be amplified to the grid circult, a. second electron discharge device having plate and grid circuits and a non inductive resistance which is included in the plate c1rcuit of the first device and the grid circuit of the second device. p
2. The combination in an amplifying system of anelectron discharge device having grid and\plate circuits, means for supplying currents to be amplified to the grid circuit, a ource of current and a non-inductive resistance" in the plate circuit, a second electron discharge device having plate and grid circuits, and means for supplying the potential variations between the terminals of said resistance to the grid circuit of the second electron discharge device.
3. The combination in an amplifying system of van electron discharge device having grid and plate circuits, means for supplying currents to be amplified to the grid circuit a source of current anda non-inductive resistance in the plate circuit, a second electron discharge device having plate and grid circuits and means for supplying potential variations produced in the plate circuit of the first device by reason of changes in curi0 rent through said resistance to the grid circuit of the second device.
In Witness whereof, I have hereunto set my-hand this 1st day of March, 1915.
IRVING LANGMUIR.
Witnesses:
EDWARD F. HENNELLY, HELEN ORFORD.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US11512A US1297188A (en) | 1913-10-29 | 1915-03-02 | System for amplifying variable currents. |
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US168893XA | 1913-10-29 | 1913-10-29 | |
US79798513A US1282439A (en) | 1913-10-29 | 1913-10-29 | System for amplifying variable currents. |
US11512A US1297188A (en) | 1913-10-29 | 1915-03-02 | System for amplifying variable currents. |
Publications (1)
Publication Number | Publication Date |
---|---|
US1297188A true US1297188A (en) | 1919-03-11 |
Family
ID=3350027
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US79798513A Expired - Lifetime US1282439A (en) | 1913-10-29 | 1913-10-29 | System for amplifying variable currents. |
US11512A Expired - Lifetime US1297188A (en) | 1913-10-29 | 1915-03-02 | System for amplifying variable currents. |
Family Applications Before (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US79798513A Expired - Lifetime US1282439A (en) | 1913-10-29 | 1913-10-29 | System for amplifying variable currents. |
Country Status (1)
Country | Link |
---|---|
US (2) | US1282439A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2548818A (en) * | 1945-12-10 | 1951-04-10 | William R Rambo | Thermionic overvoltage protection circuit |
-
1913
- 1913-10-29 US US79798513A patent/US1282439A/en not_active Expired - Lifetime
-
1915
- 1915-03-02 US US11512A patent/US1297188A/en not_active Expired - Lifetime
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2548818A (en) * | 1945-12-10 | 1951-04-10 | William R Rambo | Thermionic overvoltage protection circuit |
Also Published As
Publication number | Publication date |
---|---|
US1282439A (en) | 1918-10-22 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US1297188A (en) | System for amplifying variable currents. | |
US1959010A (en) | Screen grid tube circuit | |
US1313094A (en) | System for amplifying variable currents | |
US1819299A (en) | Tuning system | |
US2002201A (en) | Regenerative system and method of operating the same | |
US2108899A (en) | Automatic volume control | |
US1173079A (en) | Selective tuning system. | |
US2060988A (en) | Keying | |
US1730577A (en) | Fornia | |
US1469075A (en) | Electron-discharge apparatus | |
US1464104A (en) | Selective apparatus for signaling circuits | |
US2402188A (en) | Electronic device and circuits | |
US2026944A (en) | Means for receiving and amplifying electric signals | |
US1654977A (en) | kellogg | |
US1910537A (en) | Signal receiving means | |
US1558437A (en) | Electrical discharge apparatus | |
US1800471A (en) | Modulating system and method | |
US2094477A (en) | Circuit arrangement for amplifying and/or frequency transformation of electrical oscillations | |
US1981056A (en) | Method of neutralizing disturbing electric waves | |
US1468116A (en) | Method of and means for amplifying potential variations | |
US2788397A (en) | Wideband communications amplifier | |
US1387986A (en) | Wireless receiving system | |
US1595429A (en) | Control of electrical energy | |
US1828094A (en) | Electrical frequency-changing apparatus of the thermionic type | |
US1931950A (en) | Superregenerative receiver |