US2108880A - Electric discharge tube - Google Patents

Electric discharge tube Download PDF

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US2108880A
US2108880A US722746A US72274634A US2108880A US 2108880 A US2108880 A US 2108880A US 722746 A US722746 A US 722746A US 72274634 A US72274634 A US 72274634A US 2108880 A US2108880 A US 2108880A
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cathode
anode
screen
electrons
column
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US722746A
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Rene A Braden
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RCA Corp
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RCA Corp
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Priority claimed from US736833A external-priority patent/US1994733A/en
Priority to DE1935R0093176 priority patent/DE694893C/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J31/00Cathode ray tubes; Electron beam tubes
    • H01J31/08Cathode ray tubes; Electron beam tubes having a screen on or from which an image or pattern is formed, picked up, converted, or stored
    • H01J31/10Image or pattern display tubes, i.e. having electrical input and optical output; Flying-spot tubes for scanning purposes
    • H01J31/12Image or pattern display tubes, i.e. having electrical input and optical output; Flying-spot tubes for scanning purposes with luminescent screen
    • H01J31/14Magic-eye or analogous tuning indicators
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J19/00Details of vacuum tubes of the types covered by group H01J21/00
    • H01J19/02Electron-emitting electrodes; Cathodes
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J2893/00Discharge tubes and lamps
    • H01J2893/0001Electrodes and electrode systems suitable for discharge tubes or lamps

Definitions

  • My invention relates to electric discharge tubes of the cathode-ray type and, particularly, to cathode-ray tuning indicators for radio receivers.
  • An object of my invention is to provide a tube of the above-mentioned type in which a column of light is produced having a height which varies in accordance with a control voltage.
  • a further object of my invention is to provide a cathode-ray tube which may be operated at comparatively low voltages.
  • a further object of my invention is to provide a cathode-ray tube in which comparatively small changes in potential applied to a control electrode or defiecting device will have a. large effect upon the electron stream or cathode-ray.
  • a still further object of my invention is to provide improved means for indicating when a radio receiver is tuned exactly to an incoming signal.
  • I utilize, in combination with a radio receiver having automatic volume control, a vacuum tube having a long, straight lament for supplying a narrow stream or band of electrons. These electrons are directed against a' plate or screen coated with fluorescent material whereby a column of light is produced. The height of this column of light is determinedv by the percentage of the filament length which is permitted to supply electrons which reach the fluorescent screen.
  • an evacuated envelope is provided with an electron gun which is located at an acute angle to a fluorescent screen whereby a small defiection of the cathode-beam produces a large change in the position of the resulting light spot on the screen.
  • Figure 1 is a view of aradio receiver which includes one embodiment of my invention.
  • Figs.l 2, 3, and 4 are views showing other em-v bodiments of my improved cathode-ray tube.
  • a radio receiver of the superheterodyne type which includes a radio frequency amplifier I, a first detector and oscillator 3 for converting the incoming signal to an intermediate frequency signal, and an intermediate frequency amplier 5.
  • the output circuit of the intermediate frequency amplifier 5 is connected through a tuned intermediate frequency transformer 'I to a diode 9 which functions both as a second detector and as an auto- 55 matic volume control tube.
  • the diode comprises an indirectly heated cathode I I, which is connected to ground as indicated at 2'I, and an anode I3.
  • the anode I3 is connected through a conductor I5 to one end of the secondary I'I of the transformer l, while the cathode II is connected through a resistor I9 to the other end of the secondary II.
  • the resistor I9 is shunted by an intermediate frequency by-pass condenser 2
  • the audio frequency signal When a modulated intermediate frequency carrier is impressed upon the diode 9, the audio frequency signal will appear across the resistor I9. This signal is impressed upon the input circuit of an audio frequency amplifier 23 by means of a coupling condenser 25 and a connection through ground indicated by the conventional symbols 2l and 29. The output of the amplifier 23 may be supplied to a loudspeaker 3
  • An automatic volume control circuit is provided in order to overcome the effects of fading of an incoming signal'. connection from the anode end or negative end of the resistor I9 through a filter resistor 33 to suitable points in the circuitrof the radio frequency amplifier I, such as the control grids of the radio frequency amplifier tubes which are made more negative as the strength of an incoming signal increases.
  • a filter condenser 35 is connected between one end of the filter resistor 33 and ground for ltering out audio frequency signals whereby the volume control potential applied to the radio frequency amplifier i varies only in accordance with slow variations in signal strength due to fading.
  • indicating means in the form of a vacuum tube 3l comprising a straight elongated cathode 39, a control grid 4I and an anode 43.
  • the anode 43 is preferably in the form of a flat plate which is rectangular in shape.
  • the grid 4I may consist of a fiat rectangular sheet of mesh material. In order to prevent electrons from going around the grid 4 I, it is preferably made wider than the anode 43. If desired, the grid may be made in the form of a mesh cylinder surrounding the filament.
  • the cathode 39 is This circuit includes a vus in the form of a directly heated illame'nt which is supported at each end by suitable supporting 4and u should be amsn in comparison with their length to reduce fringing" of the electrons at their cut-of! point.
  • the reason for this is that there are a certain number of electrons which do not leave the filament at right angles thereto. Therefore, there will be a small fringe of light at the end of the luminous column on the screen I3, this fringe being reduced as the spacing between tube elements is reduced.
  • the cathode may be heated from any suitable source of direct current such as a battery 43.
  • the positive terminal of the battery 43 is connected to the upper end of the cathode 33, this end of the cathode being connected to ground as indicated by the conventional symbol 3l.
  • the anode 43 is supplied with a positive potential from any suitable source of direct current, such as the unit which supplies voltage for the plates o! the radio receiver tubes or a battery 30.
  • the negative terminal oi this direct-current supply unit is connected to ground whereby the potential difference between the upper end of the cathode 33 and the anode 43 is equal to the voltage supplied by the said unit.
  • the potential diilerence between the lower endof the cathode 33 and the anode 43 is equal to the voltage of the said plate supply unit plus the potential drop along :the cathode.
  • the side of the anode 43 which laces the cathode 33 is coated with a fluorescent material 33 so that the face'of the anode glows to form a column of light when it is bombarded by electrons from the cathode 33.
  • the control grid 4I is connected through a con
  • the grid 4I is at such a potential with respect to the upper end of the cathodel 33 that the electrons emitted from the entire length of the cathode strike lthe fluorescent coating 53 to produce a long column of light.
  • the grid 4I becomes more negative, and' by proper adjustment of the voltages in the circuit, the negative grid 4I will prevent the electrons emitted from the upper end of the cathode 33 from striking the iluorescent coating 53.
  • the potential drop along the cathode 33 should be fairly large. For example, in the case illustrated in Fig. 1, ten volts may be applied across the lament.
  • FIG. 2 A still greater control may be obtained by employing the construction shown in Fig. 2 in which figure parts similar to those in Fig. 1 are indicated by the same reference numerals. 'l'.his tuning indicator is the same as the tube 31 shown in Fig. l except that the straight nlament has been replaced by a directly heated illameut Il which has been coiled to increase the length of filament for a given cathode length.
  • a 110 direct-current voltage supply for example, may be connected directly across the filament 33.
  • one end of the coiled nlament may be stretched out" as r.
  • an evacuated envelope lil has an electron gun 32 located therein, this gun comprising an indirectly heated cathode 33 and an anode 35 having an opening therein through which the electrons pass to form the cathode-ray or beam indicated at 31.
  • this gun comprising an indirectly heated cathode 33 and an anode 35 having an opening therein through which the electrons pass to form the cathode-ray or beam indicated at 31.
  • a fluorescent screen 33 is provided which may be in the form of a coating of fluorescent material on the interior of the glass envelope 3l.
  • the axis of the electron gun 32 is positioned at an acute angle with respect to the iluorescent screen 33-as indicated in the drawing. ,I
  • Any suitable means lmay' betprovided for defiecting the cathode-ray such means being illustrated in the drawing' as a pair of electrostatic dei'lecting plates'll. Since the undeected cathode-ray 31 strikes the iluorescent screen 33 at a sharp ⁇ angle, a slight deection of the cathode-ray will produce a comparatively large change in the position of the luminous spot on the iluorescent screen. Therefore, a rather small voltage change produced on the deecting plates 1
  • the cathode-ray tube illustrated in Fig. 4 is the same as that shown in Fig. 3 except for the diierence in shape of the uorescent screen, like parts in the two iigures being indicated by the same reference numerals.
  • a iluorescent screen 13 is illustrated ashaving a curvature such that a voltage applied to the deilecting plates 1i in accordance with a vsquare law causes a linear deflection of theluminous spot on the uorescent screen.
  • the fluorescent screen may be given other shapes in order to cause lthe shift or deflection of the luminous spot thereon to v'ary in a desired relation with respect to the voltage applied to the deecting plates.
  • Either the envelope SI may be shaped to give the screen 'I3 the proper curvature, or the screen 13 may be supported in the envelope 6l upon a separate supporting surface.
  • An electric discharge tube comprising an elongated cathode adapted to emit electrons, an anode, a uorescent material coating upon said anode and in the direct path of theemitted electrons, means for directing said electrons against said screen, and means for selectively preventing a portion of said cathode from supplying electrons which reach said screen.
  • An electric discharge tube including elongated iluorescent screen, an elongated means for developing a stream of electrons and directing said stream upon said screen, said stream being substantiall;7 rectangular in cross-section whereby a column of light is produced on said screen, and means for producing a variable voltage gradient longitudinally of said electron developing means and said screenffor varying the length ofsaid column of light.
  • An electric discharge tube including a iiuorescent screen, means including an elongated cathode for impressing a stream of electrons upon said screen, said stream having a shape in crosssection such that a column of light is produced on said screen, and means for varying the voltage gradient over the length of said cathode and between the cathode and the screen for varying the length of said column.
  • an elongated cathode adapted to emit electrons, an anode, a fluorescent screen material coated upon said anode and positioned to receive said electrons, and control' electrode means intermediate the cathode and the fluorescent coated anode for controlling the length of said cathode which is eiective to supply electrons which reach said screen.
  • an electric discharge tube comprising an elongated cathode consisting of a directly heated filament, means for producing a ow of current .through said iilament which causes one end of the cathode to be at a different potential than the other end, a control electrode, an anode, a iiuorescent material coating upon said anode and positioned to receive directly the electrons emitted from said cathode whereby a luminous column is formed thereon, and means for applying a voltage to said control grid in response to tuning the receiver to an incoming sig-V nal which voltage has a Value such as to change the length of said luminous column.

Description

Feb. 22, 1938.
R, A. BRADEN ELECTRIC DISCHARGE TUBE Filed April 27, 1954 Patented Feb. 22, 1938 UNITED STATES /PATENT OFFICE Rene A. Braden,
Collingswood, N: J., assigner to Radio Corporation of America, a corporation f Delaware Application April 27, 1934, Serial N0. 722,746
6 Claims.
My invention relates to electric discharge tubes of the cathode-ray type and, particularly, to cathode-ray tuning indicators for radio receivers.
An object of my invention is to provide a tube of the above-mentioned type in which a column of light is produced having a height which varies in accordance with a control voltage.
A further object of my invention is to provide a cathode-ray tube which may be operated at comparatively low voltages.
A further object of my invention is to provide a cathode-ray tube in which comparatively small changes in potential applied to a control electrode or defiecting device will have a. large effect upon the electron stream or cathode-ray.
A still further object of my invention is to provide improved means for indicating when a radio receiver is tuned exactly to an incoming signal.
In one embodiment of my invention, I utilize, in combination with a radio receiver having automatic volume control, a vacuum tube having a long, straight lament for supplying a narrow stream or band of electrons. These electrons are directed against a' plate or screen coated with fluorescent material whereby a column of light is produced. The height of this column of light is determinedv by the percentage of the filament length which is permitted to supply electrons which reach the fluorescent screen.
In another embodiment ofA my invention, an evacuated envelope is provided with an electron gun which is located at an acute angle to a fluorescent screen whereby a small defiection of the cathode-beam produces a large change in the position of the resulting light spot on the screen.
Other objects, features and advantages of my invention will appear from the following description taken in connection with the accompanying 40 drawing in which: Figure 1 is a view of aradio receiver which includes one embodiment of my invention; and
Figs.l 2, 3, and 4 are views showing other em-v bodiments of my improved cathode-ray tube.
.Referring to Fig. l, there is shown a radio receiver of the superheterodyne type which includes a radio frequency amplifier I, a first detector and oscillator 3 for converting the incoming signal to an intermediate frequency signal, and an intermediate frequency amplier 5. The output circuit of the intermediate frequency amplifier 5 is connected through a tuned intermediate frequency transformer 'I to a diode 9 which functions both as a second detector and as an auto- 55 matic volume control tube.
(Cl. Z50-40) The diode comprises an indirectly heated cathode I I, which is connected to ground as indicated at 2'I, and an anode I3. The anode I3 is connected through a conductor I5 to one end of the secondary I'I of the transformer l, while the cathode II is connected through a resistor I9 to the other end of the secondary II. In order that the output of the transformer 'I may be impressed across the anode I3 and the cathode II through a low impedance circuit, the resistor I9 is shunted by an intermediate frequency by-pass condenser 2|.
When a modulated intermediate frequency carrier is impressed upon the diode 9, the audio frequency signal will appear across the resistor I9. This signal is impressed upon the input circuit of an audio frequency amplifier 23 by means of a coupling condenser 25 and a connection through ground indicated by the conventional symbols 2l and 29. The output of the amplifier 23 may be supplied to a loudspeaker 3|.
An automatic volume control circuit is provided in order to overcome the effects of fading of an incoming signal'. connection from the anode end or negative end of the resistor I9 through a filter resistor 33 to suitable points in the circuitrof the radio frequency amplifier I, such as the control grids of the radio frequency amplifier tubes which are made more negative as the strength of an incoming signal increases. A filter condenser 35 is connected between one end of the filter resistor 33 and ground for ltering out audio frequency signals whereby the volume control potential applied to the radio frequency amplifier i varies only in accordance with slow variations in signal strength due to fading.
Because of the automatic volume control circuit, it is difficult to tune the receiver exactly to incoming signals merely by listening to the loudspeaker output. It is especially desirable, therefore, to provide the receiver with visual indicating means to indicate when the receiver is tuned exactly to the desired signal.
I have provided such indicating means in the form of a vacuum tube 3l comprising a straight elongated cathode 39, a control grid 4I and an anode 43. The anode 43 is preferably in the form of a flat plate which is rectangular in shape. The grid 4I may consist of a fiat rectangular sheet of mesh material. In order to prevent electrons from going around the grid 4 I, it is preferably made wider than the anode 43. If desired, the grid may be made in the form of a mesh cylinder surrounding the filament. The cathode 39 is This circuit includes a vus in the form of a directly heated illame'nt which is supported at each end by suitable supporting 4and u should be amsn in comparison with their length to reduce fringing" of the electrons at their cut-of! point. The reason for this is that there are a certain number of electrons which do not leave the filament at right angles thereto. Therefore, there will be a small fringe of light at the end of the luminous column on the screen I3, this fringe being reduced as the spacing between tube elements is reduced.
The cathode may be heated from any suitable source of direct current such as a battery 43. In the particular embodiment illustrated, the positive terminal of the battery 43 is connected to the upper end of the cathode 33, this end of the cathode being connected to ground as indicated by the conventional symbol 3l. The anode 43 is supplied with a positive potential from any suitable source of direct current, such as the unit which supplies voltage for the plates o! the radio receiver tubes or a battery 30. It will be understood that the negative terminal oi this direct-current supply unit is connected to ground whereby the potential difference between the upper end of the cathode 33 and the anode 43 is equal to the voltage supplied by the said unit. It will be apparent that the potential diilerence between the lower endof the cathode 33 and the anode 43 is equal to the voltage of the said plate supply unit plus the potential drop along :the cathode. A
The side of the anode 43 which laces the cathode 33 is coated with a fluorescent material 33 so that the face'of the anode glows to form a column of light when it is bombarded by electrons from the cathode 33.
The control grid 4I is connected through a con,
doctor 55, and, if desired, a biasing`battery s1 to the anode end of the resistor I3 whereby the grid 4i becomes more negative in response to the reception of an incoming signal. When thereceiver is not tuned to an incoming signal, the grid 4I is at such a potential with respect to the upper end of the cathodel 33 that the electrons emitted from the entire length of the cathode strike lthe fluorescent coating 53 to produce a long column of light. As the receiver is tuned to an incoming signal, the grid 4I becomes more negative, and' by proper adjustment of the voltages in the circuit, the negative grid 4I will prevent the electrons emitted from the upper end of the cathode 33 from striking the iluorescent coating 53. Thus the column of light on the anode 43 becomes shorter, and the greater the negative potential applied to the control grid 4 I, the shorter the column of light becomes until, when the receiver is tuned exactly to the desired signal, the grid is negative the maximum amount Iand the columnof light has been shortened to its minimum length. From the above description, it will be understood that in tuning the receiver, the indicator tube 31 is watched and the tuning adjusted until the column of light reaches its minimum length.
In order that a varying potential on the control grid 4I shall have a control eiIect of the desired magnitude, the potential drop along the cathode 33 should be fairly large. For example, in the case illustrated in Fig. 1, ten volts may be applied across the lament.
A still greater control may be obtained by employing the construction shown in Fig. 2 in which figure parts similar to those in Fig. 1 are indicated by the same reference numerals. 'l'.his tuning indicator is the same as the tube 31 shown in Fig. l except that the straight nlament has been replaced by a directly heated illameut Il which has been coiled to increase the length of filament for a given cathode length. By utilizing this type of cathode, a 110 direct-current voltage supply, for example, may be connected directly across the filament 33.
If desired, instead of coiling the filament 33 uniformly from one end to the other, one end of the coiled nlament may be stretched out" as r.
indicated in the drawing. This causes most of the potential drop to be along the upper section of the cathode so that if the tube is used in the circuit shown in Fig. l, the light column will'not change greatly until the receiver is tuned almost exactly to the desired signal, at which time the grid 4l will become negative enough to stop the current iiow between the upper end of the cathode and the plate, and thereby suddenly shorten the column of light. I
An `important; advantage o! my /above-described tuningindicator tube is that it may be operated at lower voltages than required forv cathode-ray tubes of the conventional type. This permits the use of the regular radioreceiver voltage supply and the necessity for a special high voltage supply is avoided.
Another embodiment of my invention is illustrated in Fig. 3. In this embodiment, an evacuated envelope lil has an electron gun 32 located therein, this gun comprising an indirectly heated cathode 33 and an anode 35 having an opening therein through which the electrons pass to form the cathode-ray or beam indicated at 31. As such structure is well known inthe art, a detailed description is not believed necessary.
A fluorescent screen 33 is provided which may be in the form of a coating of fluorescent material on the interior of the glass envelope 3l.
In accordance with my invention, the axis of the electron gun 32 is positioned at an acute angle with respect to the iluorescent screen 33-as indicated in the drawing. ,I
Any suitable means lmay' betprovided for defiecting the cathode-ray, such means being illustrated in the drawing' as a pair of electrostatic dei'lecting plates'll. Since the undeected cathode-ray 31 strikes the iluorescent screen 33 at a sharp` angle, a slight deection of the cathode-ray will produce a comparatively large change in the position of the luminous spot on the iluorescent screen. Therefore, a rather small voltage change produced on the deecting plates 1| by the reception of an incoming signal will produce a very Vdecided. change in the position of the luminous spot on the screen to indicate that the receiver has been tuned exactly to the incoming signal.
The cathode-ray tube illustrated in Fig. 4 is the same as that shown in Fig. 3 except for the diierence in shape of the uorescent screen, like parts in the two iigures being indicated by the same reference numerals. In Fig.- 4, a iluorescent screen 13 is illustrated ashaving a curvature such that a voltage applied to the deilecting plates 1i in accordance with a vsquare law causes a linear deflection of theluminous spot on the uorescent screen. It will be understood that the fluorescent screen may be given other shapes in order to cause lthe shift or deflection of the luminous spot thereon to v'ary in a desired relation with respect to the voltage applied to the deecting plates. Either the envelope SI may be shaped to give the screen 'I3 the proper curvature, or the screen 13 may be supported in the envelope 6l upon a separate supporting surface.
From the foregoing description it will be apparentthat various other modifications may be made in my invention Without departing from the spirit and scope thereof and, I desire, therefore, that only such limitations shall be placed thereon as are necessitated by the prior art and set forth in the appended claims.
I claim as my invention:
1. An electric discharge tube comprising an elongated cathode adapted to emit electrons, an anode, a uorescent material coating upon said anode and in the direct path of theemitted electrons, means for directing said electrons against said screen, and means for selectively preventing a portion of said cathode from supplying electrons which reach said screen.
2. 'An electric discharge tube including elongated iluorescent screen, an elongated means for developing a stream of electrons and directing said stream upon said screen, said stream being substantiall;7 rectangular in cross-section whereby a column of light is produced on said screen, and means for producing a variable voltage gradient longitudinally of said electron developing means and said screenffor varying the length ofsaid column of light.
3. An electric discharge tube including a iiuorescent screen, means including an elongated cathode for impressing a stream of electrons upon said screen, said stream having a shape in crosssection such that a column of light is produced on said screen, and means for varying the voltage gradient over the length of said cathode and between the cathode and the screen for varying the length of said column.
4. In an electric discharge tube, an elongated cathode adapted to emit electrons, an anode, a fluorescent screen material coated upon said anode and positioned to receive said electrons, and control' electrode means intermediate the cathode and the fluorescent coated anode for controlling the length of said cathode which is eiective to supply electrons which reach said screen.
5. In a radio receiver, an electric discharge tube comprising an elongated cathode consisting of a directly heated filament, means for producing a ow of current .through said iilament which causes one end of the cathode to be at a different potential than the other end, a control electrode, an anode, a iiuorescent material coating upon said anode and positioned to receive directly the electrons emitted from said cathode whereby a luminous column is formed thereon, and means for applying a voltage to said control grid in response to tuning the receiver to an incoming sig-V nal which voltage has a Value such as to change the length of said luminous column. f
6. An electron discharge tube claimed in claim 4 wherein the control electrode positioned intermediate the cathode and the fluorescent coated anode is of larger dimensions than either the anode or cathode to prevent electron flow between the cathode and anode in a path other than through the control electrode.
RENE A. BRADEN.
US722746A 1934-04-27 1934-04-27 Electric discharge tube Expired - Lifetime US2108880A (en)

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Application Number Priority Date Filing Date Title
US722746A US2108880A (en) 1934-04-27 1934-04-27 Electric discharge tube
DE1935R0093176 DE694893C (en) 1934-04-27 1935-04-26 Voting indicators, especially for radio receivers

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Application Number Priority Date Filing Date Title
US722746A US2108880A (en) 1934-04-27 1934-04-27 Electric discharge tube
US736833A US1994733A (en) 1934-07-25 1934-07-25 Tuning indicator tube

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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2465041A (en) * 1942-12-12 1949-03-22 Svenska Elektronror Ab Electron discharge device
US2640093A (en) * 1949-12-22 1953-05-26 Rca Corp High voltage measuring device
US2763814A (en) * 1952-04-22 1956-09-18 Sebel S A Electronic fluorescent illuminating lamp
US2802128A (en) * 1952-06-21 1957-08-06 Int Standard Electric Corp Tuning indicator valve
US2820916A (en) * 1940-07-23 1958-01-21 Int Standard Electric Corp Tuning indicator valve of small dimension and a high sensitivity

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE950873C (en) * 1951-03-08 1956-10-18 Lorenz C Ag Vacuum tubes for measuring and displaying electrical voltages, in which a light sector is generated on a fluorescent screen

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2820916A (en) * 1940-07-23 1958-01-21 Int Standard Electric Corp Tuning indicator valve of small dimension and a high sensitivity
US2465041A (en) * 1942-12-12 1949-03-22 Svenska Elektronror Ab Electron discharge device
US2640093A (en) * 1949-12-22 1953-05-26 Rca Corp High voltage measuring device
US2763814A (en) * 1952-04-22 1956-09-18 Sebel S A Electronic fluorescent illuminating lamp
US2802128A (en) * 1952-06-21 1957-08-06 Int Standard Electric Corp Tuning indicator valve

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