US2335050A - Electron discharge amplifier - Google Patents
Electron discharge amplifier Download PDFInfo
- Publication number
- US2335050A US2335050A US447939A US44793942A US2335050A US 2335050 A US2335050 A US 2335050A US 447939 A US447939 A US 447939A US 44793942 A US44793942 A US 44793942A US 2335050 A US2335050 A US 2335050A
- Authority
- US
- United States
- Prior art keywords
- cathode
- inductance
- anode
- discharge device
- electron discharge
- 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
- 239000004020 conductor Substances 0.000 description 11
- 230000003534 oscillatory effect Effects 0.000 description 9
- 230000007850 degeneration Effects 0.000 description 7
- 238000013016 damping Methods 0.000 description 5
- 230000008929 regeneration Effects 0.000 description 4
- 238000011069 regeneration method Methods 0.000 description 4
- 230000008859 change Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000006386 neutralization reaction Methods 0.000 description 1
- 230000008520 organization Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F1/00—Details of amplifiers with only discharge tubes, only semiconductor devices or only unspecified devices as amplifying elements
- H03F1/08—Modifications of amplifiers to reduce detrimental influences of internal impedances of amplifying elements
Definitions
- My invention relates to electron discharge amplifiers and particularly to such amplifiers operating at frequencies at which difiiculties are encountered due to low input resistance of the discharge device.
- An object of my invention is to reduce the degeneration produced by oscillatory currents of the output circuit of the amplifier flowing in this common lead to the cathode.
- a further object of my invention is to provide means to maintain the cathode of an electron discharge device operating at such frequencies at ground potential.
- Another object of my invention is to provide means to produce neutralization of the voltage on this cathode lead.
- FIG. 1 of the drawing I have shown therein an amplifier I having a cathode 2, a control electrode 3, a screen electrode 4, asuppressor electrode 5 and an anode 6. Between the control electrode 3 and cathode 2 is connected a tuned circuit 1, which I have indicated as being coupled to a receiving antenna 8, although, of course, any desired means may be employed for exciting in this circuit 1 oscillatory electromotive forces to be amplified by amplifier I. These oscillatory electromotive forces are amplified by the discharge device I and may be supplied through a coupling condenser 9 to the control grid of a subsequent amplifier I0, if desired.
- the anode 6 of the discharge device is supplied with operating potential from a source of anode voltage the positive terminal of which is indicated at H and the negative terminal 01 which may be grounded as at l2.
- This circuit may include a suitable resistance l3, high frequency choke coil l4 and tuning inductance IS.
- the inductance l5 may be proportioned to resonate with such capacity as exists between the anode and cathode of the discharge device I plus the capacity across the tending within the discharge device.
- discharge device !0 This latter capacity is indicated in dotted lines at IS.
- the cathode of the discharge device I is connected to ground through a lead conductor having unavoidable inductance, although this conductor may be made as short' as conditions of practice permit.
- This inductance is represented at I! and I8.
- a substantial portion of this inductance may be that comprised by the lead ex- Oscillatory electromotive force produced on these inductances I1 and I8 exists between the control electrode 3 and cathode 2 and hence reduces the resistance of the discharge device for reasons that are well understood in the art.
- FIG. 2 This character of the circuit is better portrayed in Fig. 2 in which the reference characters employed' in Fig. 1 are applied to corresponding elements.
- the inductance I is shown as having one terminal connected to the anode of the discharge device I and its lower terminal connected to the point on the cathode lead between inductances I1 and I8.
- the input capacitance of discharge device II) is indicated at I6 and the total capacitance between the anode and cathode of the discharge device I is indicated at 2I. Since inductance I5 resonates with capacitances 2I and I 6, the current may be considered as flowing downward through the inductance I5 and then dividing and flowing in opposite directions through inductances I1 and I8 and hence upward through condensers I6 and 2
- inductances IT and I8 have a ratio to each other which is the inverse of that between capacitances 2I and I6, then zero voltage exists between the cathode 2 of discharge device I and ground I2.
- the screen grid 4 of the discharge device I of Fig. 1 is shown as supplied with operating potential from the terminal through a resistance 22 and an inductance 23 and as being connected directly to cathode 2 through a large bypass condenser 24.
- the suppressor grid 5 is shown connected directly to the cathode 2 of the discharge device.
- an electron discharge device having an anode and cathode, a capacitive load connected between said anode and cathode through an inductance and a second inductance connected between said anode and an interme- 5 diate point on said first inductance, said point cathode is at ground potential at the operating frequency.
- an electron discharge device having an anode, and a cathode, a capacitive load contacted between said anode and ground, an inductance between said cathode and ground and an inductance between said anode and a point dividing said first inductance into two parts having a ratio therebetween equal to the ratio of the capacity between said anode and cathode to the capacitance of said load.
- a pair of electron discharge devices connected in cascade, one of said devices having a cathode; and output electrode and th other having a cathode and input electrode, the latter of said cathodes being grounded, an inductance between said cathodes, and a second inductance having one terminal connected to said input and output electrodes and its other termi- 35 nal connected to a point'on said first inductance such that said first cathode is maintained at ground potential atthe operating frequency.
- connection between said anode and cathode including a capacitive load device a connection between said control electrode and cathode including a source of radio frequency electromotive force to be amplified, said connections including a common conductor extending to said cathode, said common conductor having length sufficient toproduce undesired feedback from said anode to said controlelectrode, and an inductance connected between said anode and a point intermediate of the length of said common conductor such that substantially zero voltage exists between the ends of said common conductor.
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Amplifiers (AREA)
Description
NOV. 23, 1943. w FYLER ELECTRON DISCHARGE AMPLIFIER Filed June 22, 1942 Inventor. George W: Fyler, by
JMMI His/Attorney Patented Nov. 23} 1943 2,335,050 ELECTRON DISCHARGE AMPLIFiER George W. Fyler, Stratford, Conn., assignor to General Electric Company, a corporation of New York Application June 22, 1942, Serial No. 447,939
6 Claims. (Cl. 179-171) My invention relates to electron discharge amplifiers and particularly to such amplifiers operating at frequencies at which difiiculties are encountered due to low input resistance of the discharge device.
In amplifiers operating at very high frequencies undesirably low resistance between the control eelctrode and cathode may result by reason of degeneration produced by the oscillatory currents in the output of the discharge device flowing through the unavoidable inductance of the conductor which extends between the cathode of the discharge device and ground. This conductor may be made as short as it is practical to make it but still has some unavoidable length, and therefore some inductance, which is common to the output and input circuits of the discharge device. The voltage on this inductance is present between the control electrode and cathode of the discharge device and operates to reduce the resistance between the control electrode and cathode. This reduction in resistance may occur to such an extent as to damp to a very objectionable degree the input tuned circuit and thus reduce the sensitivity of the amplifier.
An object of my invention is to reduce the degeneration produced by oscillatory currents of the output circuit of the amplifier flowing in this common lead to the cathode. v
A further object of my invention is to provide means to maintain the cathode of an electron discharge device operating at such frequencies at ground potential.
Another object of my invention is to provide means to produce neutralization of the voltage on this cathode lead.
The novel features which I believe to be characteristic of my invention are set forth with particularity in the appended claims. My invention itself, however, both as to its organization and method of operation, together withfurther objects and advantages thereof, may best be understoodby'reference to the following description 1 taken in connection with the accompanying drawing in which Fig. 1 represents an embodiment of my invention and Fig. 2 represents schematically a portion of the circuits of Fig. 1.
Referring to Fig. 1 of the drawing I have shown therein an amplifier I having a cathode 2, a control electrode 3, a screen electrode 4, asuppressor electrode 5 and an anode 6. Between the control electrode 3 and cathode 2 is connected a tuned circuit 1, which I have indicated as being coupled to a receiving antenna 8, although, of course, any desired means may be employed for exciting in this circuit 1 oscillatory electromotive forces to be amplified by amplifier I. These oscillatory electromotive forces are amplified by the discharge device I and may be supplied through a coupling condenser 9 to the control grid of a subsequent amplifier I0, if desired. The anode 6 of the discharge device is supplied with operating potential from a source of anode voltage the positive terminal of which is indicated at H and the negative terminal 01 which may be grounded as at l2. This circuit may include a suitable resistance l3, high frequency choke coil l4 and tuning inductance IS. The inductance l5 may be proportioned to resonate with such capacity as exists between the anode and cathode of the discharge device I plus the capacity across the tending within the discharge device.
input of discharge device !0. This latter capacity is indicated in dotted lines at IS.
The cathode of the discharge device I is connected to ground through a lead conductor having unavoidable inductance, although this conductor may be made as short' as conditions of practice permit. This inductance is represented at I! and I8. A substantial portion of this inductance may be that comprised by the lead ex- Oscillatory electromotive force produced on these inductances I1 and I8 exists between the control electrode 3 and cathode 2 and hence reduces the resistance of the discharge device for reasons that are well understood in the art.
In accordance with myinvention, means are provided whereby this electromotive force is neutralized so that the cathode 2 of the discharge device I is maintained at ground potential and thus the undesired effects of this voltage are obviated. This result is accomplished by connecting the lower terminal of anode tuning inductance l5 through'condenser 20 to a point on the cathode lead dividing the inductance of the cathode lead into the two portions l1 and I8. This capacity 20 may be one of'very high value such' that its impedance is entirely negligible at the frequencies involved. If the inductances I1 and I8 be proportioned with respect to each other so thatkinductance ll bears the same ratio to inductance l8 that the capacity l6 bears to the capacity 2|, then zero voltage exists between the cathode 2 and ground l2. This capacitance 2| is represented in dottedlines in Fig. 1 and comprises such capacity as exists between the anode and cathode of device I.
This character of the circuit is better portrayed in Fig. 2 in which the reference characters employed' in Fig. 1 are applied to corresponding elements. The inductance I is shown as having one terminal connected to the anode of the discharge device I and its lower terminal connected to the point on the cathode lead between inductances I1 and I8. The input capacitance of discharge device II) is indicated at I6 and the total capacitance between the anode and cathode of the discharge device I is indicated at 2I. Since inductance I5 resonates with capacitances 2I and I 6, the current may be considered as flowing downward through the inductance I5 and then dividing and flowing in opposite directions through inductances I1 and I8 and hence upward through condensers I6 and 2|. Thus, if inductances IT and I8 have a ratio to each other which is the inverse of that between capacitances 2I and I6, then zero voltage exists between the cathode 2 of discharge device I and ground I2.
Such proportioning of the circuit is highly desirable since it avoids the degeneration and reduced input resistance of discharge device I previously referred to and thus avoids the undesired damping of the oscillatory circuit 1, 8 of Fig. 1. This permits sharper tuning of this circuit and greater sensitivity of the apparatus.
Of course, if the tuning of the anode circuit of discharge device I be varied by varying either capacitance I6 or 2I a. certain amount of regeneration or degeneration will be produced by reason of unequal voltages on inductances I1 and I8 and a certain amount of damping of the circuit 1, 8 results. However, no such damping, regeneration, or degeneration results from variation of tuning by varying inductance I5 over a considerable range.
The screen grid 4 of the discharge device I of Fig. 1 is shown as supplied with operating potential from the terminal through a resistance 22 and an inductance 23 and as being connected directly to cathode 2 through a large bypass condenser 24. Likewise, the suppressor grid 5 is shown connected directly to the cathode 2 of the discharge device. These connections are conventional in amplifiers operating at such frequency, but it is desirable that the capacitance 24 be reasonably large to prevent oscillatory voltages from appearing on the screen grid 4.
If degeneration, or regeneration results to any appreciable extent from the fact that the lead to the screen grid 4, or those to condenser 24, have finite length, and therefore finite inductance, such regeneration or degeneration can be compensated for by appropriate change in relative values of inductances I1 and I8. Actually this change may be made by sliding the connection of condenser 20 to the cathode lead along the cathode lead until such compensation obtains.
While I have shown a particular embodiment of my invention, it will, of course, be understoodthat I do not wish to be limited thereto since various modifications in the circuit illustrated and instrumentalities employed may be made, and I contemplate by the appended claims to cover any such modifications as fall within the true spirit and scope of my invention.
What I claim as new and desire to secure by Letters Patent of the United States is:
1. In combination, an electron discharge device having an anode and cathode, a capacitive load connected between said anode and cathode through an inductance and a second inductance connected between said anode and an interme- 5 diate point on said first inductance, said point cathode is at ground potential at the operating frequency. I
3. In combination, an electron discharge device having an anode, and a cathode, a capacitive load contacted between said anode and ground, an inductance between said cathode and ground and an inductance between said anode and a point dividing said first inductance into two parts having a ratio therebetween equal to the ratio of the capacity between said anode and cathode to the capacitance of said load.
4. In combination, a pair of electron discharge devices connected in cascade, one of said devices having a cathode; and output electrode and th other having a cathode and input electrode, the latter of said cathodes being grounded, an inductance between said cathodes, and a second inductance having one terminal connected to said input and output electrodes and its other termi- 35 nal connected to a point'on said first inductance such that said first cathode is maintained at ground potential atthe operating frequency.
5. The combination, in an electron discharge radio frequency amplifier having a control electrode, a cathode, and an anode, a connection between said anode and cathode including a capacitive load device, a connection between said control electrode and cathode including an oscillatory input circuit, said connections including a common conductor extending to said cathode, said common conductor having sufficient length to produce feedback resulting in undesired damping of said oscillatory circuit, and an inductance connected between said anode and a point intermediate of the length of said common conductor, said point being chosen to reduce said damping.
6. The combination, in an electron discharge radio frequency amplifier having a control elec trode, a cathode, and an anode, a connection between said anode and cathode including a capacitive load device, a connection between said control electrode and cathode including a source of radio frequency electromotive force to be amplified, said connections including a common conductor extending to said cathode, said common conductor having length sufficient toproduce undesired feedback from said anode to said controlelectrode, and an inductance connected between said anode and a point intermediate of the length of said common conductor such that substantially zero voltage exists between the ends of said common conductor.
GEORGE W. FYLER.
on said first inductance of such value that said- CERTIFICATE OF CORRECTION. Patent No. 2,555,050. November 25, 191;}.
GEORGE W. FYLER.
It is hereby certified that error appears in the printed specification of the above numbered patent requiring correction as follows: Page 2', second colum n, line 19, claim 3, for "contacted" read --connected--; and that the said Letters Patent should. be read with this correction therein that the same may" conform to the record of the case in the Patent Office Signed and sealed. this 25th day of January, A. D. 191m.
Henry Van Arsdale, (Seal) Acting Commissioner of Patents.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| BE474424D BE474424A (en) | 1942-06-22 | ||
| US447939A US2335050A (en) | 1942-06-22 | 1942-06-22 | Electron discharge amplifier |
| GB9808/43A GB564243A (en) | 1942-06-22 | 1943-06-18 | High frequency electron discharge amplifiers |
| FR938658D FR938658A (en) | 1942-06-22 | 1946-10-18 | Improvements to high frequency amplifiers |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US447939A US2335050A (en) | 1942-06-22 | 1942-06-22 | Electron discharge amplifier |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US2335050A true US2335050A (en) | 1943-11-23 |
Family
ID=23778357
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US447939A Expired - Lifetime US2335050A (en) | 1942-06-22 | 1942-06-22 | Electron discharge amplifier |
Country Status (4)
| Country | Link |
|---|---|
| US (1) | US2335050A (en) |
| BE (1) | BE474424A (en) |
| FR (1) | FR938658A (en) |
| GB (1) | GB564243A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2546247A (en) * | 1947-12-17 | 1951-03-27 | William C Wolf | Process of recovering barite from its native materials |
| US2649508A (en) * | 1948-11-12 | 1953-08-18 | Bell Telephone Labor Inc | Interstage coupling circuit for wide band amplifiers |
-
0
- BE BE474424D patent/BE474424A/xx unknown
-
1942
- 1942-06-22 US US447939A patent/US2335050A/en not_active Expired - Lifetime
-
1943
- 1943-06-18 GB GB9808/43A patent/GB564243A/en not_active Expired
-
1946
- 1946-10-18 FR FR938658D patent/FR938658A/en not_active Expired
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2546247A (en) * | 1947-12-17 | 1951-03-27 | William C Wolf | Process of recovering barite from its native materials |
| US2649508A (en) * | 1948-11-12 | 1953-08-18 | Bell Telephone Labor Inc | Interstage coupling circuit for wide band amplifiers |
Also Published As
| Publication number | Publication date |
|---|---|
| GB564243A (en) | 1944-09-19 |
| BE474424A (en) | |
| FR938658A (en) | 1948-10-21 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US2359504A (en) | High frequency selective system and method | |
| US2197124A (en) | Oscillator with amplifier coupling | |
| US2335050A (en) | Electron discharge amplifier | |
| US2729708A (en) | Band-pass amplifier systems | |
| US2368454A (en) | Thermionic amplifier | |
| US2444864A (en) | High-frequency tuned amplifying circuit | |
| US2271519A (en) | Neutralizing system | |
| US2197239A (en) | Stabilized tuned system | |
| US2226259A (en) | Amplifier | |
| US1993783A (en) | Oscillation generator | |
| US1925520A (en) | Frequency multiplication | |
| US2430699A (en) | Amplifier gain control | |
| US2310455A (en) | Ultra short wave amplifier circuit | |
| US2113340A (en) | Ultrahigh frequency oscillator | |
| US2411565A (en) | Low impedance oscillator | |
| US2427241A (en) | Push-pull circuit arrangement for ultra-short waves | |
| US2373184A (en) | Ultra high frequency vacuum tube circuit | |
| US2235198A (en) | Anode neutralizing circuit for short waves | |
| US2314916A (en) | Circuit for the amplification and/or frequency-transformation of electrical oscillations of ultra high frequency | |
| US2026944A (en) | Means for receiving and amplifying electric signals | |
| US2344734A (en) | Neutralizing circuit | |
| US1971919A (en) | Negative conductance circuits | |
| US2228081A (en) | Correction circuits | |
| US2235565A (en) | Tuned circuit system | |
| US2211718A (en) | Ultra-high-frequency signaltranslating stage |