US2216209A - Discharge tube - Google Patents

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US2216209A
US2216209A US179094A US17909437A US2216209A US 2216209 A US2216209 A US 2216209A US 179094 A US179094 A US 179094A US 17909437 A US17909437 A US 17909437A US 2216209 A US2216209 A US 2216209A
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anode
cathode
cathodes
anodes
main
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US179094A
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Mutscheller Arthur
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J21/00Vacuum tubes
    • H01J21/20Tubes with more than one discharge path; Multiple tubes, e.g. double diode, triode-hexode
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J2893/00Discharge tubes and lamps
    • H01J2893/003Tubes with plural electrode systems

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  • This invention is for an improved high voltage current rectifier of the hot cathode type having many valuable features and advantages over the old known system of employing several single 5 rectifier units for accomplishing the same result.
  • Fig. 1 shows diagrammatically how, with a diaphragm of insulating material, and by operating at least one set of electrodes at voltage saturation the short-circuiting of electrons from one of the inlet electrodes directly over to the other 45 can be prevented.
  • Big. 2 shows, diagrammatically, how with specially constructed anodes alternating current can be rectified without the electrons short-circuiting from the cathode of one inlet terminal to the 5 anode of the other inlet terminal.
  • Fig.3 is a diagrammatic illustration of an anode and a cathode with which the escape of electrons to the outside of the cooperating anode is prevented.
  • Fig. 4 shows, diagrammatically, how an X-ray tube can be constructed in which both alternating current impulses are utilized for the production of X-rays and how the direct passage of electrons from one inlet electrode to the other has been avoided.
  • FIG. l shows-two ways of preventing electrons from passing directly or short-cir cuiting for example from the cathode of one of the inlet terminals to the anode of the other inlet terminal.
  • One way is to place the inlet cathode and anode in compartments separated by a septum or partition of dielectric material as here, the anodes 3
  • the discharge instead of a direct discharge from cathode 35 to anode ill, or from cathode 34 to anode 3d, the discharge must first be between cathodedfi and anode 33 then from cathode 32 to anode 3i or from cathode 3:1 to anode 33 and from cathode 32 to anode 3t, and the current flowing in the outside circuit from anodes 33 to the cathodes 32 is then unidirectional.
  • the other way is to operate the discharge from cathodes Mend 35 to the anodes 33 at voltage saturation and the discharge from the cathodes 35 32 to the anodes 3i and 36 below voltage saturation and therefore so that the electron emission from the. cathodes 32. is larger than that from the cathodes 3i and and that the voltage applied to the terminals til and 31 is sufficiently high to produce voltage saturation between cathodes 34 and'35 and the anodes 33.
  • Fig. 2 and Fig. 3 a third way of preventing the. direct a passage of electrons between the cathodes and the anodes of the inlet terminals is illustrated.
  • the anodes l2, l6, l8 and 1B are of special design so that even if operated below saturation, the direct passage of electrons from one of the inlet terminals to the other is prevented.
  • These anodes are shaped to surround the coop- 5o crating cathodes to such an extent, that the negative potential onthe lead-in wires to the emittingcathode which pass through the center of openings in the anode is sufficient to prevent the escape of electrons along the lead-in wires and out of the enclosing anode.
  • the electron emitting cathodes 14, 13, 11 and 15 are caged-up within the receiving anodes 12, 19, 18 and 16 and the construction of the opening in the anode is so adjusted, that its diameter is smaller than the inside diameter of the anode. Still, if the anode is made tubular having a length dimension in the direction of the cathode lead-in wires greater than the diameter and closed at one end, it may not be necessary to make the opening for the cathode lead-in wires smaller than the lumen of the tubular anode.
  • Fig. 2 two pairs of such anodes surrounding the cooperating cathodes: are shown connected to form an alternating current rectifier which operates on the principle above outlined.
  • the inlet terminals 82 and H receive alternating current impulses; the negative impulse from terminal 82 passes from cathode TI to anode 18 out through outlet terminal 89 through an outside circuit back to inlet terminal 8
  • the opening in the anodes and the diameter of the cathode lead-in wires must be so adjusted, that if the voltage in the outside circuit is as large as that of the alternating current in-put, that no electrons can escape from the anodes that encage the cooperating cathodes.
  • is spherical and provided with an opening having rounded and extended edges 92 which is smaller in diameter than the spherical anode.
  • the cathode 96 is either a flat spiral, loops or a mushroom-shaped coil to leave a substantially equally spaced distance between the cathode and the anode;
  • the cathode is supported by the lead-in wires 93 and 94 and a disc having rounded edges 95 may be placed so as to form an electrostatic shield to prevent electrons from escaping the anode.
  • the enclosing anode therefore, shields off all outside fields and the shield increases the electrostatic shielding effect of the cathode lead-in Wires which are negatively charged so that no electrons can get out of the anode no matter how high the positive potential on the anode of the other inlet terminal may be.
  • the discharge from the cathodes 34 and 35 is controlled directionally with a focusing device 39 so that the discharge therefrom will fall uponan anode placed into the path of the accelerated cathode stream, and then adjusting the cathodes 32 to operate with the cooperating anodes below voltage saturation so that the voltage drop between these is less than the voltage drop between the cathodes 34 and 35 of the inlet terminals and the anodes 33; or the anodes may be formed to surround the electron emitting parts of the cathodes as shown in Fig. 2 and Fig.
  • An electric discharge tube comprising an envelope having therein a main anode having hollow electron receiving sections and a main thermionic cathode having electron emitting sections, an auxiliary hollow anode substantially enclosing each of said electron emitting sections, additional thermionic cathodes each being substantially enclosed by one of said hollow electron receiving sections, independent leads connected tween each auxiliary hollow anode and one only of said additional thermionic cathodes.
  • An electric discharge tube comprising an envelope having therein a main anode having electron receiving sections, and a main thermionic cathode having electron emitting sections, an auxiliary anode adjacent each of said electron emitting sections, additional thermionic cathodes being adjacent to said main anode and each having a focusing shield about each of said additional thermionic cathodes to direct the electron discharge therefrom upon the electron receiving sections of said main anode, independent leads connected to said main cathode and to each of said auxiliary thermionic cathodes, a conductive lead between said main anode and said main cathode and a conductive connection between each auxiliary anode and one only of said additional thermionic cathodes.
  • An electron discharge tube comprising an envelope having therein a main anode having electron receiving sections, and a main thermianode and one only of said additional thermionic cathodes, and a partition of dielectric material between non-adjacent electrodes as a shield against electron discharges between non-adjacent anodes and cathodes.
  • An electric discharge tube comprising an envelope having therein a main anode having electron receiving sections and a main thermionic cathode having electron emitting sections, an auxiliary hollow anode substantially enclosing-each of said electron emitting sections, ad-
  • thermionic cathodes each being adjacent one of said electron receiving sections and having a focusing shield for directing the electron discharge upon said main anode, independent leads connected to said main cathode and to each of said thermionic cathodes, a lead connecting said main cathode and said main anode together, and a conductive connection between each auxiliary hollow anode and one only of said additional thermionic cathodes.
  • An electron discharge tube comprising an envelope having therein a main anode having electron receiving sections, and a main thermionic cathode having electron emitting sections,
  • auxiliary anode adjacent each of said electron emitting sections, additional thermionic cathodes one adjacent each of said electron receiving sections, independent leads connected to said main and to each of said additional thermionic cathodes, a lead connected to said main anode, a conductive connection between each auxiliary anode and one only of said additional thermionic cathodes, there being means for preventing electronic discharges between said ad- 10 ditional cathodes and said auxiliary anodes.

Description

Oct. 1, 1940.
A. MUTSCHELLER- mscnmem TUBE Original Filed Dec. 10, 1937 IN V EN TOR.
Patented Oct. 1, 1940 PATENT or'ricr.
DISCHARGE TUBE Arthur Mutscheller, New York, Y.
Application December 10, 1937, Serial No. 179,094
Renewed March 4, 1940 5 Claims. (01. 250-2125) This invention is for an improved high voltage current rectifier of the hot cathode type having many valuable features and advantages over the old known system of employing several single 5 rectifier units for accomplishing the same result.
More specifically stated, I have discovered how a number of rectifiers of the high vacuum type can be combined into one unit and therewith the same result obtained as with the much more 10 cumbersome and expensive old system in which several rectifiers must be interconnected, me-
chanically assembled and insulated from each other.
. As an example, we have in the well known 15 Graetz system for rectifying high voltage alternating current,- a transformer having connected to each of its high voltage producing terminals two valve tubes one with its anode and the other with its cathode. The free anodes of these two 20 pairs of valve tubes and alsothe free cathodes are connected together and from these then a high voltage pulsating unidirectional current is obtained. This kind of rectified high voltage current is usable for many purposes as for the 25 excitation of X-ray tubes, dust precipitation, furnishing of plate voltage to radio circuits etc.
To obviate the requirement of connecting, supporting and insulating from one anotherof four tifier mounted in one envelope can be con structed.
40 Fig. 1 shows diagrammatically how, with a diaphragm of insulating material, and by operating at least one set of electrodes at voltage saturation the short-circuiting of electrons from one of the inlet electrodes directly over to the other 45 can be prevented. a
Big. 2 shows, diagrammatically, how with specially constructed anodes alternating current can be rectified without the electrons short-circuiting from the cathode of one inlet terminal to the 5 anode of the other inlet terminal.
. Fig.3 is a diagrammatic illustration of an anode and a cathode with which the escape of electrons to the outside of the cooperating anode is prevented.
5 Fig. 4 shows, diagrammatically, how an X-ray tube can be constructed in which both alternating current impulses are utilized for the production of X-rays and how the direct passage of electrons from one inlet electrode to the other has been avoided. I 5
If electrons should directly traverse the evacuated space, for instance in Fig. 2 from cathode ll to anode llhthcn there could be no rectification as it is intended and the circuit through the discharge device would be short-circuited Without delivering rectified current to the outlet terminals fill and ill. Therefore, this direct transfer of electrons from one inlet terminal to the other must be prevented.
How this can be done is shownin the diagram Fig. l, which shows-two ways of preventing electrons from passing directly or short-cir cuiting for example from the cathode of one of the inlet terminals to the anode of the other inlet terminal. One way is to place the inlet cathode and anode in compartments separated by a septum or partition of dielectric material as here, the anodes 3| and 3% are on one side of the partition 39 and the cathodes 3t and 35 are on the other side of it. Therefore, instead of a direct discharge from cathode 35 to anode ill, or from cathode 34 to anode 3d, the discharge must first be between cathodedfi and anode 33 then from cathode 32 to anode 3i or from cathode 3:1 to anode 33 and from cathode 32 to anode 3t, and the current flowing in the outside circuit from anodes 33 to the cathodes 32 is then unidirectional. The other way is to operate the discharge from cathodes Mend 35 to the anodes 33 at voltage saturation and the discharge from the cathodes 35 32 to the anodes 3i and 36 below voltage saturation and therefore so that the electron emission from the. cathodes 32. is larger than that from the cathodes 3i and and that the voltage applied to the terminals til and 31 is sufficiently high to produce voltage saturation between cathodes 34 and'35 and the anodes 33.
In Fig. 2 and Fig. 3 a third way of preventing the. direct a passage of electrons between the cathodes and the anodes of the inlet terminals is illustrated. The anodes l2, l6, l8 and 1B are of special design so that even if operated below saturation, the direct passage of electrons from one of the inlet terminals to the other is prevented. These anodes are shaped to surround the coop- 5o crating cathodes to such an extent, that the negative potential onthe lead-in wires to the emittingcathode which pass through the center of openings in the anode is sufficient to prevent the escape of electrons along the lead-in wires and out of the enclosing anode. Thus the electron emitting cathodes 14, 13, 11 and 15 are caged-up within the receiving anodes 12, 19, 18 and 16 and the construction of the opening in the anode is so adjusted, that its diameter is smaller than the inside diameter of the anode. Still, if the anode is made tubular having a length dimension in the direction of the cathode lead-in wires greater than the diameter and closed at one end, it may not be necessary to make the opening for the cathode lead-in wires smaller than the lumen of the tubular anode.
In Fig. 2", two pairs of such anodes surrounding the cooperating cathodes: are shown connected to form an alternating current rectifier which operates on the principle above outlined. The inlet terminals 82 and H receive alternating current impulses; the negative impulse from terminal 82 passes from cathode TI to anode 18 out through outlet terminal 89 through an outside circuit back to inlet terminal 8| from cathode 14 to anode 12 to inlet terminal ll. Or, if terminal H is negative, the electrons pass from cathode 13 to anode 19 to outlet terminal 80, through an outside circuit back to terminal 8!, from cathode 15 to anode !6 to inlet terminal 82. The opening in the anodes and the diameter of the cathode lead-in wires must be so adjusted, that if the voltage in the outside circuit is as large as that of the alternating current in-put, that no electrons can escape from the anodes that encage the cooperating cathodes.
How this is done is illustrated in the diagrammatic Fig. 3. The anode 99 supported on a stem 9| is spherical and provided with an opening having rounded and extended edges 92 which is smaller in diameter than the spherical anode. The cathode 96 is either a flat spiral, loops or a mushroom-shaped coil to leave a substantially equally spaced distance between the cathode and the anode; The cathode is supported by the lead-in wires 93 and 94 and a disc having rounded edges 95 may be placed so as to form an electrostatic shield to prevent electrons from escaping the anode. The enclosing anode, therefore, shields off all outside fields and the shield increases the electrostatic shielding effect of the cathode lead-in Wires which are negatively charged so that no electrons can get out of the anode no matter how high the positive potential on the anode of the other inlet terminal may be.
The aforegoing description should serve to show, that there are numerous ways of preventing the direct passage of electrons from the cathode of one of the inlet terminals to the anode of the other inlet terminal which are connected to the alternating current source. Several of these have been described and illustrated. For instance by shielding with dielectric substance in Fig. l; by operating, at least one pair of cathodes and anodes at saturation as is shown in Fig. 1, where the discharge from the cathodes 34 and 35 is controlled directionally with a focusing device 39 so that the discharge therefrom will fall uponan anode placed into the path of the accelerated cathode stream, and then adjusting the cathodes 32 to operate with the cooperating anodes below voltage saturation so that the voltage drop between these is less than the voltage drop between the cathodes 34 and 35 of the inlet terminals and the anodes 33; or the anodes may be formed to surround the electron emitting parts of the cathodes as shown in Fig. 2 and Fig. 3 to the extent that no electrons can be pulledout oi the surrounding anode even if the voltage delivered into the Working circuit in the form of unidirectional pulsating current impulses is equal to the voltage of the energizing alternating current. This same object may be obtained by providing a third or grid electrode having a voltage that prevents any electrons from escaping from within the anode through the opening through which the cathode lead-in wires are passing. All these are methods which in principle are well understood in the art and which any person skilled in this art can carry out successfully with these instructions Without requiring further aid or instruction.
Having thus described several ways according to which my invention can be carried out, I hereby declare that other ways may exist with which the same results may be obtained and which may be substituted for those herein disclosed without having to do additional inventing.
Therefore, I claim,
1. An electric discharge tube comprising an envelope having therein a main anode having hollow electron receiving sections and a main thermionic cathode having electron emitting sections, an auxiliary hollow anode substantially enclosing each of said electron emitting sections, additional thermionic cathodes each being substantially enclosed by one of said hollow electron receiving sections, independent leads connected tween each auxiliary hollow anode and one only of said additional thermionic cathodes.
2. An electric discharge tube comprising an envelope having therein a main anode having electron receiving sections, and a main thermionic cathode having electron emitting sections, an auxiliary anode adjacent each of said electron emitting sections, additional thermionic cathodes being adjacent to said main anode and each having a focusing shield about each of said additional thermionic cathodes to direct the electron discharge therefrom upon the electron receiving sections of said main anode, independent leads connected to said main cathode and to each of said auxiliary thermionic cathodes, a conductive lead between said main anode and said main cathode and a conductive connection between each auxiliary anode and one only of said additional thermionic cathodes.
3. An electron discharge tube comprising an envelope having therein a main anode having electron receiving sections, and a main thermianode and one only of said additional thermionic cathodes, and a partition of dielectric material between non-adjacent electrodes as a shield against electron discharges between non-adjacent anodes and cathodes.
4. An electric discharge tube comprising an envelope having therein a main anode having electron receiving sections and a main thermionic cathode having electron emitting sections, an auxiliary hollow anode substantially enclosing-each of said electron emitting sections, ad-
ditional thermionic cathodes each being adjacent one of said electron receiving sections and having a focusing shield for directing the electron discharge upon said main anode, independent leads connected to said main cathode and to each of said thermionic cathodes, a lead connecting said main cathode and said main anode together, and a conductive connection between each auxiliary hollow anode and one only of said additional thermionic cathodes.
5. An electron discharge tube comprising an envelope having therein a main anode having electron receiving sections, and a main thermionic cathode having electron emitting sections,
an auxiliary anode adjacent each of said electron emitting sections, additional thermionic cathodes one adjacent each of said electron receiving sections, independent leads connected to said main and to each of said additional thermionic cathodes, a lead connected to said main anode, a conductive connection between each auxiliary anode and one only of said additional thermionic cathodes, there being means for preventing electronic discharges between said ad- 10 ditional cathodes and said auxiliary anodes.
ARTHUR MUTSCHELLER.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2458577A (en) * 1945-07-02 1949-01-11 Rca Corp High-potential power supply

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2458577A (en) * 1945-07-02 1949-01-11 Rca Corp High-potential power supply

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