US2237671A

US2237671A - Electron discharge device

Info

Publication number: US2237671A
Application number: US266730A
Authority: US
Inventors: Kallmann Heinz Erwin
Original assignee: EMI Ltd
Current assignee: EMI Ltd; Electrical and Musical Industries Ltd
Priority date: 1939-02-15
Filing date: 1939-04-08
Publication date: 1941-04-08
Anticipated expiration: 1958-04-08

Description

pl 8, 1941- y H. E. KALLMANN 2,237,671

ELECTRON DI S CHARGE DEV ICE Filed April. 8, 1959 I NVEN TOR. HEINZ ERW/N KALLMNN BY v ,qw/L

ATTORNEY.

Patented Apr. L, 1941 ELECTRON DISCHARGE DEVICE Heinz Erwin Kallmann, Ealing, London, England,

assigner to Electric & Musical Industries Limited, Hayes, England, a company of Great Britain Application April 8, 1939, Serial No. 266,739 In Great Britain February 15, 1939 9 Claims.

This invention relates to electron discharge devices, and is more particularly, but not exclusively concerned with electrical methods and means for summing a series of magnitudes.

Various ways are possible in which such summation may be effected, but unless special precautions are taken it is often diicult to avoid unduly loading or coupling the sources of electromotivc force corresponding to the various magnitudes to be summed.

According to the invention, this difficulty is overcome in a patricularly simple manner by employing an electron discharge electrode by means of which electrons may be accelerated in the form of a beam to an anode, there being provided a pluralityof substantially independent deflecting means to which deflecting potentials may be applied, said anode being of such a form that it provides an output dependent on the deflection of said beam so that the magnitude of said output represents the combined effect of said deflecting potentials.

ln order that the said invention may be better understood, and more readily carried into effect, the same will now be described by way of example with reference to the accompanying drawing:

liigure l shows in diagrammatic form a tube in accordance with the invention in which a resistance target anode is employed, and

Figure 2 illustrates a modified form of target anode which may be used in the place of the resistance anode of Figure l.

Referring to Figure l. there are located within the evacuated envelope l an emitting cathode Il heated by the heater element l2; a pair of electrodes i3 and I4, which when suitably biased have at least a rough focusing effect upon the stream of electrons emitted by the cathode Il, the electrode il also acting as an accelerating electrode; the pairs of deilecting plates l5-l5', lli-I6', lll-ll'. lll-IB' shielded from one another by the screening electrodes I9. 2ll and 2l: and the target anode 22 formed by a strip of resistance material and having one end 24 connected to a point of positive potential with respect to the cathode. the other end 23 providing a point from which an output may be taken from the tube.

rl'he deflecting potentials may be applied to the dcilecting plates in various ways. Thus, if the sum of a number of potential differences is required, each potential difference may be applied across a pair of plates, in push-pull fashion, though this is not necessary: an essentially necessary condition if the undlstorted sum of the potential differences is desired is that the sensitivity of all the plates shall be substantially the same. If each potential diierence is to be multiplied by a separate constant, this can easily be effected by suitable spacing of the deflection plates of the respective pairs or by choice of their distances from the target. The same effect may be achieved by suitably dimensioning the sizes of the plates. The deflection sensitivity of the plates may also be controlled by the application of suitable biasing potentials to the screening electrodes i9, 20, 2l. Such potentials may also be ernployed to aid the focussing of the electron beam, though no particularly sharp or well defined spot is required upon the anode 22. For this reason the total accelerating potential may be kept quite small, with the advantage that a high deflecting sensitivity is obtained.

The operation of the anode 22 will be evident from the gure and the previous description. Thus the potential of the end 2d will always be less than that of the end 2t by the fall in potential due to the beam current flowing through that part of the anode between the point at which the beam impinges and the end 24. lf as stated the anode is a uniform resistance strip, changes in potential will be proportional to changes in the angle of deflection of the beam.

In Figure 2 another form of anode is shown. This anode comprises a plate 29 partially overlapping the plate 26, and it is supposed that a very large spot is employed, so that part falls on either plate. Plate 26 is connected directly to a source of positive potential while plate 25 is connected to this source through the resistance 2l. By means of this resistance an output is obtained at the output terminal 28, this output being determined by the extent to which the spot falls on the plate 25. If desired, the collecting anode may be in the form of a plate or sheet adapted to be rendered luminous by the impact of the electron beam so as to afford an indication of the combined effect of the defiecting potentials.

The invention is of particular application as part of a network which forms the subject-matter of co-pending British cognate applications Nos. 19096/38` and 4939/39, wherein it is necessary to provide means for the summation of a number of potentials or potential differences without appreciably coupling or loading the sources from which they are derived. The invention may also be applied to the synthesis of wave-shapes from the various harmonic components, In one particular form of this application the tube may possess a fluorescent screen and a deflection at right angles may be applied which is proportional to the magnitude of the fundamental frequency, the target-anode being omitted. The invention is, ol' course, not limited to these examples, and it has application wherever positive or negative magnitudes required to be added: nor is it limited to the use of an anode providing an output directly proportional to the beam deection; by suitably constructing the anode the device may be arranged to provide an output which is a predetermined function of the sum of variables.

I claim:

1. An electron discharge tube comprising an elongated envelope, an electron emitting cathode at one end of said envelope, a target electrode positioned at the other end of said envelope and in register with said cathode, an electrode system for focusing electrons from said cathode into a beam, said electrode system being positioned intermediate said cathode and said target electrode and in register therewith, at least three deflecting systems each adapted to be excited by an individual source of energy positioned intermediate said electrode system and said target electrode, said deflecting systems being adapted to additively deect said beam of electrons in a single common plane across said target and terminal means connected to said target electrode to derive an output potential in accordance with the deflection of said beam.

2. An electron discharge tube comprising an elongated envelope, an electron emitting cathode at one end of said envelope, a target electrode positioned at the other end of said envelope and in register with said cathode, an electrode system for focusing electrons from said cathode into a beam, said electrode system being positioned intermediate said cathode and said target electrode and in register therewith, at least three deflecting systems positioned intermediate said electrode system and said target electrode, said deecting svstems being adapted to additively deflect said beam of electrons in a single common plane across said target electrode, and electrostatic shielding members intermediate adjacent defiecting syst-ems.

3. An electron discharge tube comprising an elongated envelope. an electron emitting cathode at one end of said envelope. a resistive target electrode positioned at the other end of said envelo'oe and in register with said cathode. an electrode system for focusing electrons from said cathode into a beam. said electrode system being positioned intermediate said cathode and said target electrode and in register therewith. at

least three deflecting systems positioned intermediate said electrode system and said resistive target electrode.. said deflecting systems being adapted to additively deflect said beam of electrops in a single common plane across said iLarget electrode, and terminal means connected to said targetl electrode to derive an output potential in accordance with the deection of said beam.

4. An electron discharge tube comprising an elongated envelope. an electron emitting cathode at one end of said envelope. a resistive target electrode positioned at the other end of said envelope and in register with said cathode. an electrode system for focusing electrons from said cathode into a beam. said electrode system'beinrz positioned intermediate said cathode and said resistive target electrode and in register therewith. at least three deecting systems positioned intermediate said electrode system and said resistive target electrode, said deflecting systems being adapted to additively dcilcct said beam ol' electrons in a single common plane across said target electrode, and electrostatic shielding members intermediate adjacent deecting systems.

5. An electron discharge tube comprising an elongated envelope, an electron emitting cathode at one end of said envelope, a resistive target electrode positioned at the other end of said envelope and in register with said cathode. an electrode system for focusing electrons from said cathode into a beam, said electrode system being positioned intermediate said cathode and said target electrode and in register therewith, and at least three electrostatic deflecting systems positioned intermediate said electrode system and said resistive target electrode, said electrostatic deflecting systems being adapted to additively deect said beam of electrons in a single common plane across said target electrode, and means connected to said target electrode for deriving output potential proportional to the dcection of said beam.

6. An electron discharge tube comprising an elongated envelope, an electron emitting cathode at one end of said envelope, a resistive target electrode positioned'at the other end of said envelope and in register with said cathode, an electrode sysem for focusing electrons from said cathode into a beam, said electrode ,system being positioned intermediate said cathode and said resistive target electrode and in register therewith, at least three electrostatic deilecting systems positioned intermediate said electrode system and said resistive target electrode, said electrostatic deflecting systems being adapted to deect said beam of electrons in a single common plane across said target electrode, and electrostatic shielding members interme'diatc adjacent deflecting systems.

'7. An electron discharge tube comprising an elongated envelope, an electron emitting cathode at one end of said envelope, a resistive target electrode positioned at the other end of said envelope and in register with said cathode, an electrode system for focusing electrons from said cathode into a beam, said electrode .system being positioned intermediate said cathodegand said resistive target electrode and in register therewith, at least three electrostatic deflecting systems positioned intermediate said electrode system and said resistive target electrode, said electrostatic deflecting systems being adapted to additively deflect said beam of ele'ctrons in a single common plane across said target electrode, electrostatic shielding members intermediate adjacent deecting systems, and terminal means for applying potential across said resistive target electrode.

8. An electron discharge tube having an elongated envelope, an electron emitting envelope positioned at one end thereof, a cylindrical electrode surrounding said cathode, a conical accelerating electrode in register with said cathode and displaced longitudinally from said cylindrical electrode, a resistive target member positioned at the end of said envelope opposite to said cathode, said resistive electrode being in register with said cathode, at least three pairs of electrostatic deflecting plates, half of said plates lying in one common plane, the other half of said plates lying in a second common plane, said plates being positioned intermediate said conical electrode and said target electrode, and electrostatic shielding members positioned intermediate adjacent pairs oi' plates. l

9. An electron discharge tube having an elongated envelope, an electron emitting envelope positioned at one end thereof, a cylindrical electrode surrounding said cathode, a conical accelerating electrode in register with said cathode and displaced longitudinally from said cylindrical electrode, a resistive target member positioned at the end of said envelope opposite to said cathode, said resistive electrode being in register with said cathode, at least three pairs of 10 electrostatic defiecting plates, half of said plates lying in one common plane, the other half of said plates lying in a second common plane, said plates being positioned intermediate said conical electrode and said target electrode, electrostatic shielding members positioned intermediate adj acent pairs of plates, and terminal means for applying potential drop across said target electrode.

HEINZ ERWIN' KALLMAN'N.