US2172198A - Tube having a plurality of grids - Google Patents

Tube having a plurality of grids Download PDF

Info

Publication number
US2172198A
US2172198A US176851A US17685137A US2172198A US 2172198 A US2172198 A US 2172198A US 176851 A US176851 A US 176851A US 17685137 A US17685137 A US 17685137A US 2172198 A US2172198 A US 2172198A
Authority
US
United States
Prior art keywords
anode
tube
screen
potential
grids
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
Application number
US176851A
Inventor
Harnisch Martin
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Siemens and Halske AG
Siemens AG
Original Assignee
Siemens AG
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Siemens AG filed Critical Siemens AG
Application granted granted Critical
Publication of US2172198A publication Critical patent/US2172198A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J19/00Details of vacuum tubes of the types covered by group H01J21/00
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J21/00Vacuum tubes
    • H01J21/02Tubes with a single discharge path

Definitions

  • the invention relates to discharge tubes and especially such tubes with a plurality of grids including tubes having a screen grid therein.
  • An object of the invention is to prevent secondary emission as far as possible and to eliminate the effect of such secondary emission as may be present.
  • Figure 1 is a schematic cross section of the electrodes in a tube constructed according to the invention
  • Fig 2 is a modification of Fig l.
  • Fig 3 is a perspective view of a tube embodying the invention.
  • the characteristic curve representing the anode current as a function of the anode potential in discharge tubes be as far as possible horizontal to make possible a control extending to small values of anode potentials.
  • the wellknown bend in the characteristic curve be in the region of very low anode potentials. Secondary emission at the anode or at the grid has prevented this type of tube characteristic curve. In the region in which the anode potential is smaller than the screen grid potential, secondary electrons are released from the anode and drawn to the screen grid. This results in a very rapid drop in the characteristic curve of the tube, and the bend point, which is the measure of the extent of the control, is projected into the region of higher anode potentials.
  • Another disadvantage of the tube of the usual structure consists in the fact that the hot anodes heat up the control grids and excite these control grids to thermionic emission of electrons, especially in the case in which the ordinary excited coated cathodes are utilized.
  • FIG. 1 is disclosed schematically the electrode system of a tube according to the invention.
  • the cathole I which may be heated directly or indirectly, is enclosed by a control grid 2, and the latter is enclosed by a screen grid 3.
  • the radially arranged anode sheets 4 are disclosed on two opposite sides of the cathode, although more or less members could be utilized and spaced as desired about the cathode.
  • the whole electrode system is preferably enclosed by a screen 5.
  • the function. of the screen is to keep scattered electrons away from the glass walls and finally to influence the form of the equipotential lines in a desired manner.
  • This screen is preferably maintained at a constant potential that is lower than the anode potential.
  • an equipotential 6 is shown dotted.
  • Fig. 2 discloses a similar tube.
  • the cathode 1 is enclosed by a control grid 8 and a screen grid 9.
  • the screen II] or H which, as disclosed in the drawing, may be at cathode potential, preferably encloses the electrode system only in part and leaves open the region around the two anode plates I 2.
  • FIG. 3 A preferred mechanical structure of a tube according to Fig. 2 is disclosed in Fig. 3 in perspec-
  • the cathode I3 is directly heated and has current leads l4 and I 5.
  • the control grid l6 enclosingthe cathode is supported by the supports I! and H3.
  • the screen grid I9 is located around the control grid and is carried by supports 2
  • the two anode plates are supported by the bars 24 and 25.
  • the screens 26 and 21, which are preferably maintained at cathode potential, can also be seen in the figure, enclosing the electrode structure except for the anode plates. All the supporting wires are'fused into the press 28.
  • the heat radiation from the anodes or anode members takes place in such a direction that disadvantageous efiects are not produced by this heat, such as the secondary electron emission of the grids previously mentioned. It is accordingly possible to increase the anode power loss far above the usual value and even to heat the anode sheets to such an extent that they glow during operation.
  • a material for the sheets either molybdenum or tantalum may be selected.
  • the electric field around the electrodes assumes such a form that the secondary electrons formed at the anode are released therefrom only with difiiculty or not at all.
  • the configuration of the potential field becomes more propitious when the screen enclosing the whole electrode system is maintained at a fixed potential, as for example ground potential. This screen need not completely enclose the electrode system, as disclosed in Figs. 2 and 3.
  • a discharge device comprising a cathode, a control grid enclosing said cathode and concentric thereto, an anode comprising at least two plates mounted in a radial direction to said cathode, and a screen enclosing approximately the discharge space between the inner ends of said anode plates but not the plates.

Description

Sept. 5 1939. M. HARNISCH TUBE HAVING A PLURALITY OF GRIDS "Filed Nov. 27, 1957 iililil INVENTOR Marta)? 'fiarm'sc/z ATTORNE WITNESSES:
Patented Sept. 5, 1939 UNITED STATES PATENT OFFICE TUBE HAVING A PLURALITY 0F GRIDS Application November 27, 1937, Serial No. 176,851
In Germany November 30, 1936 1 Claim.
The invention relates to discharge tubes and especially such tubes with a plurality of grids including tubes having a screen grid therein.
An object of the invention is to prevent secondary emission as far as possible and to eliminate the effect of such secondary emission as may be present.
Other objects and advantages of the invention will be apparent from the following description and drawing, in which:
Figure 1 is a schematic cross section of the electrodes in a tube constructed according to the invention;
Fig 2 is a modification of Fig l; and,
Fig 3 is a perspective view of a tube embodying the invention.
It is desirous that the characteristic curve representing the anode current as a function of the anode potential in discharge tubes be as far as possible horizontal to make possible a control extending to small values of anode potentials. In other words, it is desirous that the wellknown bend in the characteristic curve be in the region of very low anode potentials. Secondary emission at the anode or at the grid has prevented this type of tube characteristic curve. In the region in which the anode potential is smaller than the screen grid potential, secondary electrons are released from the anode and drawn to the screen grid. This results in a very rapid drop in the characteristic curve of the tube, and the bend point, which is the measure of the extent of the control, is projected into the region of higher anode potentials. W'hen smaller anode potentials are utilized, there are then too: large distortions in the output potential. If the anode potential is larger than the applied screen grid potential, then the anode current rises at the expense of the screen grid current, weakened by secondary emission. The secondary screen currents make the characteristic curve more steep instead of horizontal. The strength of the secondary emission also fluctuates with the life of the tube and the constants of the tube are thus varied.
Another disadvantage of the tube of the usual structure consists in the fact that the hot anodes heat up the control grids and excite these control grids to thermionic emission of electrons, especially in the case in which the ordinary excited coated cathodes are utilized.
Various attempts heretofore made to suppress the desired phenomena of secondary electron emission involved complicating the electrode tive.
thus distinguishing clearly from the case in which anodes either wholly or in part enclose the other electrodes and project their heat into the discharge space.
In Figure 1 is disclosed schematically the electrode system of a tube according to the invention. The cathole I, which may be heated directly or indirectly, is enclosed by a control grid 2, and the latter is enclosed by a screen grid 3. The radially arranged anode sheets 4 are disclosed on two opposite sides of the cathode, although more or less members could be utilized and spaced as desired about the cathode. The whole electrode system is preferably enclosed by a screen 5. The function. of the screen is to keep scattered electrons away from the glass walls and finally to influence the form of the equipotential lines in a desired manner. This screen is preferably maintained at a constant potential that is lower than the anode potential. To explain the course of the field, an equipotential 6 is shown dotted.
Fig. 2 discloses a similar tube. Here also the cathode 1 is enclosed by a control grid 8 and a screen grid 9. The screen II] or H, which, as disclosed in the drawing, may be at cathode potential, preferably encloses the electrode system only in part and leaves open the region around the two anode plates I 2.
A preferred mechanical structure of a tube according to Fig. 2 is disclosed in Fig. 3 in perspec- The cathode I3 is directly heated and has current leads l4 and I 5. The control grid l6 enclosingthe cathode is supported by the supports I! and H3. The screen grid I9 is located around the control grid and is carried by supports 2|] and 2|. The two anode plates are supported by the bars 24 and 25. The screens 26 and 21, which are preferably maintained at cathode potential, can also be seen in the figure, enclosing the electrode structure except for the anode plates. All the supporting wires are'fused into the press 28.
The heat radiation from the anodes or anode members takes place in such a direction that disadvantageous efiects are not produced by this heat, such as the secondary electron emission of the grids previously mentioned. It is accordingly possible to increase the anode power loss far above the usual value and even to heat the anode sheets to such an extent that they glow during operation. As a material for the sheets, either molybdenum or tantalum may be selected.
The electric field around the electrodes assumes such a form that the secondary electrons formed at the anode are released therefrom only with difiiculty or not at all. The configuration of the potential field becomes more propitious when the screen enclosing the whole electrode system is maintained at a fixed potential, as for example ground potential. This screen need not completely enclose the electrode system, as disclosed in Figs. 2 and 3.
The application of the invention is not limited to tubes which have the number of electrodes illustrated in the drawing. In particular, a large number of anode plates, control grids, or also a space discharge grid may be provided. In fact, many modifications may be made in the form and arrangement of the elements disclosed, and accordingly, the following claim is not to be limited except as is necessitated by the prior art.
I claim as my invention:
.A discharge device comprising a cathode, a control grid enclosing said cathode and concentric thereto, an anode comprising at least two plates mounted in a radial direction to said cathode, and a screen enclosing approximately the discharge space between the inner ends of said anode plates but not the plates.
MARTIN HARNISCH.
US176851A 1936-11-30 1937-11-27 Tube having a plurality of grids Expired - Lifetime US2172198A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
DE2172198X 1936-11-30

Publications (1)

Publication Number Publication Date
US2172198A true US2172198A (en) 1939-09-05

Family

ID=7988496

Family Applications (1)

Application Number Title Priority Date Filing Date
US176851A Expired - Lifetime US2172198A (en) 1936-11-30 1937-11-27 Tube having a plurality of grids

Country Status (1)

Country Link
US (1) US2172198A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2604600A (en) * 1947-05-28 1952-07-22 Well Surveys Inc Radiation detector
US3315119A (en) * 1963-07-19 1967-04-18 Albert W Friend Cathode ray tube control circuit having multi-function vacuum tube

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2604600A (en) * 1947-05-28 1952-07-22 Well Surveys Inc Radiation detector
US3315119A (en) * 1963-07-19 1967-04-18 Albert W Friend Cathode ray tube control circuit having multi-function vacuum tube

Similar Documents

Publication Publication Date Title
GB838078A (en) Thermometer type voltage indicator tube
US2172198A (en) Tube having a plurality of grids
US2173267A (en) Electron discharge device
US2254128A (en) Electron multiplier
US2459861A (en) Electrode structure for electrical space discharge tubes
US2285126A (en) Electron multiplier
GB2065962A (en) Improvements in or Relating to Thyratrons
US2206954A (en) Electron discharge device
US2273800A (en) Fluorescent type indicator tube
US2340631A (en) Secondary electron amplifier
US2134407A (en) Electron discharge device
US2879430A (en) Electron discharge devices
US2141303A (en) Electric discharge tube
US2111256A (en) Electron discharge tube
US2143916A (en) Electron discharge device
US2006716A (en) Electron discharge device
US2459072A (en) Beam power tube
US1927475A (en) High vacuum discharge vessel in particular X-ray tubes
US2264624A (en) Image analyzing tube
US2084734A (en) Electron discharge device
US2932754A (en) Electron tubes
US2022212A (en) Low capacity thermionic tube
US2205500A (en) Electron discharge device
US2236012A (en) Electron discharge device
US2526054A (en) Electrode assembly for very highfrequency electron discharge devices