US1621058A - Electric condenser - Google Patents

Electric condenser Download PDF

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Publication number
US1621058A
US1621058A US8276A US827625A US1621058A US 1621058 A US1621058 A US 1621058A US 8276 A US8276 A US 8276A US 827625 A US827625 A US 827625A US 1621058 A US1621058 A US 1621058A
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dielectric
layer
condenser
resistance
protective layer
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Expired - Lifetime
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US8276A
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Burger Oswald
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CBS Corp
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Westinghouse Electric and Manufacturing Co
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01GCAPACITORS; CAPACITORS, RECTIFIERS, DETECTORS, SWITCHING DEVICES, LIGHT-SENSITIVE OR TEMPERATURE-SENSITIVE DEVICES OF THE ELECTROLYTIC TYPE
    • H01G9/00Electrolytic capacitors, rectifiers, detectors, switching devices, light-sensitive or temperature-sensitive devices; Processes of their manufacture
    • H01G9/15Solid electrolytic capacitors

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  • OSWALD BURGER OF BERLIN-CHARLOTTENBURG, GERMANY, ASSIGNOR TO WESTING- HOUSE ELECTRIC & MANUFACTURING- COMPANY, OF NEW YORK, N. Y., A CORPORA- TION.
  • My invention relates to improvements in electric condensers.
  • this disadvantags is avoided by arranging between the conducting layer and the dielectric layer of the condenser a protective layer of semiconductin material.
  • the resistance which the protective layer oflers to the discharge current is relatively low and consequently also the voltage loss caused by it.
  • the resistance of the protective layer becomes of considerably greater importance in comparison with the diminished resistance of the dielectric.
  • the improved condenser is illustrated in the accompanying drawing, the single figure of which is a sectional view through a portion of a condenser embodying my invention.
  • the eflect of the protective layer will be clear from the following description and explanation.
  • d- is the dielectric layer, s the protective layer according to my invention and m the metal foil or conductive layer.
  • the current which sows from the oint a, across this place a through the die ectric towards the point a finds a resistance in the protective lever a which is in proportion to the thickness of the protective layer and the area of the defectlve place.
  • the resistance is owing to the small extent of the defective zone. If the current were to flow into the defective place a from other places, such as 72, 6 it would be obliged to pass obliquely through the protective layer in order to reach the defective place a. The length of the path of the current and therefore also the resistance which it encounters would thus become greater.
  • the thickness of the protective layer depends-upon the circumstances, and in articular upon its conductivity in comparison with that of the dielectric. In many cases it is advisable to choose for the protective layer, a material which is not too poor 8. condoctor, and to make it of considerably greater thickness than the dielectric.
  • the protective layer may be disposed at one side of the dielectric only, as shown in the illustration, or at both sides.
  • What I claim as my invention is 1..
  • a dielectric layer conducting layers at both sides of said dielectric layer and a layer of semi-conducting protective material between said dielectric and one of said conducting layers, said layer of protective material being of considerably greater thick ness than said dielectric layer.
  • a condenser comprising two conducting sheets separated by a dielectric, at least one of said sheets comprising a layer of good conductivity capable of carrying currents in considerable,
  • a composite plate for an'electric discharge device comprising a layer of good conductivity capable of carrying currents in a direction parallel to its surface and a second layer on one or both of its sides, said second'layer being of such material as to greatly oppose the flow of discharge currents in a direction substantially parallel to its surface, while permitting a relativel easy passage of currents to orfrom sai first-' mentioned layer in a direction normal to its surface;

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  • Power Engineering (AREA)
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Description

ELECTRIC CONDENSER Filed Feb. 10, 1925 March 15 1927.
IIIIIII INVENTOR Oszua/a Burger BY ATTORNEY"- Patented Mar. 15, 1927.
UNITED. STATES 1,621,058 PATENT OFFICE.
OSWALD BURGER, OF BERLIN-CHARLOTTENBURG, GERMANY, ASSIGNOR TO WESTING- HOUSE ELECTRIC & MANUFACTURING- COMPANY, OF NEW YORK, N. Y., A CORPORA- TION.
ELECTRIC connnnsnn.
Application filed February 10, 1925, Serial No. 8,276, and in Germany February 12, 1824.
My invention relates to improvements in electric condensers.
It is well known that the capacity of a condenser is the greater the thinner its dielectric layer. Attempts have therefore been made to keep this layer as thin as possible. These attempts soon reached their limit' owing to the difliculties which arose in producing and finishing the dielectric materials. If the layer is very thin a defective place will naturally form a relatively considerable part of its thickness. Such a weakened place will not be able to sustain the total voltage of the condenser and a puncture will occur which destroys the dielectric layer and thereby the entire condenser. To avoid the danger just mentioned it has hitherto been necessary to make the dielectric layer thicker than was desirable for the capacity of the condenser.
According to my invention this disadvantags is avoided by arranging between the conducting layer and the dielectric layer of the condenser a protective layer of semiconductin material. When the dielectric is in fault ess condition the resistance which the protective layer oflers to the discharge current is relatively low and consequently also the voltage loss caused by it. When, however, there is a defective place in the dielectric which reduces -its resistance, the resistance of the protective layer becomes of considerably greater importance in comparison with the diminished resistance of the dielectric. v p
The improved condenser is illustrated in the accompanying drawing, the single figure of which is a sectional view through a portion of a condenser embodying my invention. The eflect of the protective layer will be clear from the following description and explanation. In the illustration, d-is the dielectric layer, s the protective layer according to my invention and m the metal foil or conductive layer. When the dielectric is in perfectly faultless condition only that resistance of the protective layer comes into lay which it offers to. a current travers ing it at right angles to its surface. Since the resistance is not great, the voltage drop in the protective layer is small. We assume now that at a there is a defective lace in the dielectric d. The current which sows from the oint a, across this place a through the die ectric towards the point a finds a resistance in the protective lever a which is in proportion to the thickness of the protective layer and the area of the defectlve place. The resistance is owing to the small extent of the defective zone. If the current were to flow into the defective place a from other places, such as 72, 6 it would be obliged to pass obliquely through the protective layer in order to reach the defective place a. The length of the path of the current and therefore also the resistance which it encounters would thus become greater. The current intensity at the weakened lace does not therefore, become essentia 1y greater than in other parts of the dielectric so that no temperature rise and no destruction of the dielectric need be feared. From this it follows that when the dielectric is undamaged the resistance of the protective layer and consequently the voltage losses are practically negligible. When, however, the dielectric has become damaged, the protectlve layer comes into full operation. t is therefore possible to make the dielectric thinner than has been permissible heretofore, whereby dielectric material is saved on the one hand while, on the other hand the capacity of the condenser is increase without the danger of short-circuits.
The thickness of the protective layer depends-upon the circumstances, and in articular upon its conductivity in comparison with that of the dielectric. In many cases it is advisable to choose for the protective layer, a material which is not too poor 8. condoctor, and to make it of considerably greater thickness than the dielectric. The protective layer may be disposed at one side of the dielectric only, as shown in the illustration, or at both sides.
What I claim as my invention is 1.. In an electric condenser, the combination of a dielectric layer, conducting layers at both sides of said dielectric layer and a layer of semi-conducting protective material between said dielectric and one of said conducting layers, said layer of protective material being of considerably greater thick ness than said dielectric layer.
2. A condenser comprising two conducting sheets separated by a dielectric, at least one of said sheets comprising a layer of good conductivity capable of carrying currents in considerable,
a direction parallel to its surface and a sec- 0nd layer of such material as to greatly oppose substantially all currents except those owing into the dielectric at approximately right angles to the surface thereof. I
3. A composite plate for an'electric discharge device comprising a layer of good conductivity capable of carrying currents in a direction parallel to its surface and a second layer on one or both of its sides, said second'layer being of such material as to greatly oppose the flow of discharge currents in a direction substantially parallel to its surface, while permitting a relativel easy passage of currents to orfrom sai first-' mentioned layer in a direction normal to its surface;
4. In an electric condenserg the combination of a dielectric layer, conducting layers at both sides of said dielectric layer and a layer of semi-conducting protective material between said dielectric and at least one of,
direction substantially parallel to its surface,
while permitting a relatively easy passage of currents to or from said dielectric in a direction normal to its surface.
In testimony whereof I affix my signature.
OSWALD BURGER.
as to greatly
US8276A 1924-02-12 1925-02-10 Electric condenser Expired - Lifetime US1621058A (en)

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Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2854639A (en) * 1953-06-19 1958-09-30 Itt Electromagnetic delay cable and manufacture thereof
US3047782A (en) * 1958-11-13 1962-07-31 Speer Carbon Company Inc Capacitor
US3066247A (en) * 1954-08-25 1962-11-27 Sprague Electric Co Electrical capacitors
US3166693A (en) * 1965-01-19 Form an oxide
US5447779A (en) * 1990-08-06 1995-09-05 Tokai Electronics Co., Ltd. Resonant tag and method of manufacturing the same
US5589251A (en) * 1990-08-06 1996-12-31 Tokai Electronics Co., Ltd. Resonant tag and method of manufacturing the same
US5695860A (en) * 1990-08-06 1997-12-09 Tokai Electronics Co., Ltd. Resonant tag and method of manufacturing the same
US5789999A (en) * 1996-11-01 1998-08-04 Hewlett-Packard Company Distributed lossy capacitive circuit element with two resistive layers

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3166693A (en) * 1965-01-19 Form an oxide
US2854639A (en) * 1953-06-19 1958-09-30 Itt Electromagnetic delay cable and manufacture thereof
US3066247A (en) * 1954-08-25 1962-11-27 Sprague Electric Co Electrical capacitors
US3047782A (en) * 1958-11-13 1962-07-31 Speer Carbon Company Inc Capacitor
US5447779A (en) * 1990-08-06 1995-09-05 Tokai Electronics Co., Ltd. Resonant tag and method of manufacturing the same
US5589251A (en) * 1990-08-06 1996-12-31 Tokai Electronics Co., Ltd. Resonant tag and method of manufacturing the same
US5682814A (en) * 1990-08-06 1997-11-04 Tokai Electronics Co., Ltd. Apparatus for manufacturing resonant tag
US5695860A (en) * 1990-08-06 1997-12-09 Tokai Electronics Co., Ltd. Resonant tag and method of manufacturing the same
US5789999A (en) * 1996-11-01 1998-08-04 Hewlett-Packard Company Distributed lossy capacitive circuit element with two resistive layers

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