EP0992042A1 - Resistance non lineaire a comportement de varistor et procede permettant de produire cette resistance - Google Patents

Resistance non lineaire a comportement de varistor et procede permettant de produire cette resistance

Info

Publication number
EP0992042A1
EP0992042A1 EP99915429A EP99915429A EP0992042A1 EP 0992042 A1 EP0992042 A1 EP 0992042A1 EP 99915429 A EP99915429 A EP 99915429A EP 99915429 A EP99915429 A EP 99915429A EP 0992042 A1 EP0992042 A1 EP 0992042A1
Authority
EP
European Patent Office
Prior art keywords
particles
varistor
electrically conductive
fraction
filler
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.)
Granted
Application number
EP99915429A
Other languages
German (de)
English (en)
Other versions
EP0992042B1 (fr
Inventor
Petra Kluge-Weiss
Felix Greuter
Ralf Struempler
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.)
ABB Research Ltd Switzerland
ABB Research Ltd Sweden
Original Assignee
ABB Research Ltd Switzerland
ABB Research Ltd Sweden
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 ABB Research Ltd Switzerland, ABB Research Ltd Sweden filed Critical ABB Research Ltd Switzerland
Publication of EP0992042A1 publication Critical patent/EP0992042A1/fr
Application granted granted Critical
Publication of EP0992042B1 publication Critical patent/EP0992042B1/fr
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01CRESISTORS
    • H01C7/00Non-adjustable resistors formed as one or more layers or coatings; Non-adjustable resistors made from powdered conducting material or powdered semi-conducting material with or without insulating material
    • H01C7/10Non-adjustable resistors formed as one or more layers or coatings; Non-adjustable resistors made from powdered conducting material or powdered semi-conducting material with or without insulating material voltage responsive, i.e. varistors
    • H01C7/12Overvoltage protection resistors
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01CRESISTORS
    • H01C7/00Non-adjustable resistors formed as one or more layers or coatings; Non-adjustable resistors made from powdered conducting material or powdered semi-conducting material with or without insulating material
    • H01C7/10Non-adjustable resistors formed as one or more layers or coatings; Non-adjustable resistors made from powdered conducting material or powdered semi-conducting material with or without insulating material voltage responsive, i.e. varistors
    • H01C7/105Varistor cores
    • H01C7/108Metal oxide
    • H01C7/112ZnO type

Definitions

  • the invention is based on a nonlinear resistor with varistor behavior according to the preamble of claim 1.
  • This resistor contains a matrix and a powdery filler embedded in the matrix.
  • the filler contains a sintered varistor granulate with predominantly spherical particles made of doped metal oxide.
  • the particles are made up of crystalline grains separated by grain boundaries. Since complex sintering processes turn out to be much simpler than comparable-acting resistors based on a sintered ceramic, such composite resistors can be produced relatively easily and in a wide variety of shapes.
  • the invention also relates to a method for producing this resistor.
  • This resistor consists of a polymer filled with a powder.
  • the powder used is a granulate which was produced by sintering a spray-dried varistor powder based on a zinc oxide doped with oxides of Bi, Sb, Mn, Co, Al and / or other metals. These granules have spherical particles shaped like a soccer ball with varistor behavior, which are made up of crystalline grains separated by grain boundaries.
  • the diameter of these particles are up to 300 ⁇ m.
  • the electrical properties of the sintered granulate such as the non-linearity coefficient ⁇ B or the breakdown field strength U B [V / mm] can be set over a wide range.
  • a resistance has a higher non-linearity coefficient and a higher breakthrough field strength when the proportion of filler decreases.
  • WO 97/26693 describes a composite material based on a polymeric matrix and a powder embedded in this matrix.
  • a granulate is used as the powder, which was also produced by sintering a spray-dried varistor powder based on a zinc oxide doped with oxides of Bi, Sb, Mn, Co, Al and / or other metals.
  • These granules have spherical particles shaped like a soccer ball with varistor behavior, which are made up of crystalline grains separated by grain boundaries. The particles have a diameter of up to 125 ⁇ m and have a size distribution that follows a Gaussian distribution.
  • This material is used in cable connections and cable terminations and forms voltage-control layers there.
  • US 4,726,991, US 4,992,333, 5,068,634 and US 5,294,374 specify voltage-limiting resistors made of a polymer and a powdery filler material based on conductive and / or semiconducting particles. With these resistors, overvoltage protection is achieved by dielectric breakdown of the polymer. Since relatively high temperatures can occur here, the overvoltage protection should not be reversible and the energy absorption capacity should be relatively low.
  • the invention is based on the object of specifying a resistor of the type mentioned at the outset, which is distinguished by a high power consumption despite a large non-linearity coefficient for good protection characteristics, and at the same time a method create with which such a resistor can be produced in a particularly advantageous manner.
  • a suitable filler electrical properties are achieved in the resistor according to the invention that come relatively close to a varistor based on a ceramic. It is essential here that either a suitably structured conductive additional filler is provided and / or that a varistor granulate is used which enables a particularly high packing density. It is then possible to use a technology known from injection molding, extrusion or casting resin technology to produce resistors with varistor behavior in a comparatively simple manner, which are characterized by good protection characteristics and high power consumption. It is particularly advantageous here that, by suitable choice of the output components and by means of process parameters which are easy to set, varistors can be produced which, with regard to their shape and their physical properties, have a broad spectrum and in particular a relatively high energy absorption or switching capacity.
  • the non-linear resistor according to the invention can advantageously be used as a field-controlling element in cable fittings or as an overvoltage protection element (varistor). It can be used in both low and medium and high voltage technology and, due to its ease of manufacture and further processing, can easily have a complex geometry. If necessary, it can be molded on, for example as a protective and / or control element, by casting directly onto an electrical apparatus, for example a circuit breaker, or applied as a thin lacquer coating. It can also be used in hybrid printing for integrated circuits.
  • the electrically conductive particles provided in addition to the varistor particles in the filler are connected to the varistor particles on their surfaces before the filler and the matrix material are brought together.
  • the electrically conductive particles cannot be detached from the surfaces of the varistor particles with great certainty, so that resistors produced by this method Excellent electrical properties, especially extremely stable current-voltage characteristics.
  • the method according to the invention ensures that the electrically conductive particles are distributed uniformly over the surfaces of the varistor particles and form an atomic bond with the varistor material.
  • the contact effect of the filler is thus significantly improved and it is sufficient to have a relatively small proportion of electrically conductive particles in the filler in order to obtain resistors with excellent electrical properties, such as, in particular, a large current carrying capacity.
  • Nonlinear resistors with varistor behavior designed as varistor composites were produced by mixing polymeric material with a filler. Such mixing processes are well known from the prior art and need not be explained in more detail.
  • the polymers can be thermosets, such as, in particular, epoxy or polyester resins, polyurethanes or silicones, or thermoplastics, for example HDPE, PEEK or ETFE.
  • a gel e.g. silicone gel
  • a liquid e.g. silicone oil, polybutane, ester oil, fats
  • a gas air, nitrogen, SF 6 , ...), a gas mixture and / or a glass
  • a gas mixture and / or a glass can also be used.
  • the filler used here contained varistor particles made of doped metal oxide with a predominantly spherical structure, the particles being composed of crystalline grains separated from one another by grain boundaries.
  • the filler was made as follows:
  • a varistor mixture of commercially available ZnO, doped with oxides of Bi, Sb, Mn and Co as well as with Ni, Al, Si and / or one or more other metals was present as an aqueous suspension or solution processed approximately spherical granules.
  • the granules were sintered in a chamber furnace, for example on an Al 2 O 3 plate coated with ZnO, a Pt film or a ZnO ceramic, or optionally also in a rotary tube furnace.
  • the heating times during sintering were up to 300 h, typically for example 50 ° C / h or 80 ° C / h.
  • the sintering temperature was between 900 ° C and 1320 ° C.
  • the holding times during sintering were between 3 hours and 72 hours. After sintering, cooling was carried out at a rate between 50 ° C / h and 300 ° C / h.
  • the varistor granules produced in this way were subsequently separated in a vibrating device or by light mechanical rubbing. By sieving, granulate fractions with particle sizes between 90 and 160 ⁇ m, 32 and 63 ⁇ m and less than 32 ⁇ m were then produced from the separated granulate.
  • Varistor granules of the different fractions were mixed together in certain weight ratios. Some of these mixtures and some of the fractions were mixed with a metal powder with geometrically anisotropic, in particular scale-shaped, electrically conductive particles with a thickness to aspect ratio of typically 1/5 to 1/100, e.g. B. Ni-flakes, whose length was less than 60 microns on average. In any case, the length of the metal particles was chosen so that on average it was smaller than the radius of an average sized particle of the coarse (90 - 160 ⁇ m) varistor granules. This and a small proportion, typically 0.05 to 5 percent by volume, of the varistor granulate prevented the formation of metallically conductive percolation paths in the mixture.
  • the starting components of the filler were generally premixed in a turbo mixer for several hours. If one of the starting components was the metal powder, its particles lay against the surfaces of the spherical varistor particles, so that particularly low-resistance contacts were created between the individual varistor particles. In addition, smaller particles fall inside the varistor particles, which are designed as a hollow sphere to a small percentage, and thus help to reduce current supply bottlenecks.
  • Fine platelets, easily deformable, soft particles and / or short fibers are also conceivable as metallic fillers.
  • a metallic filler with particles that melt in the area of the highest processing temperatures, preferentially accumulate in the contact points of the varistor particles and lead there to an improved local contact is advantageous.
  • fine powders for example based on silver, copper, aluminum, gold, indium and their alloys, or conductive oxides, borides, carbides with particle diameters preferably between 1 and 20 ⁇ m can also be used as the metallic filler.
  • the particles of these powders can easily be spherical.
  • the electrically conductive particles contained in the filler should be connected to the varistor particles on their surfaces.
  • the content of conductive electrical particles can then be low and have a lower value of 0.05 percent by volume.
  • Such a surface connection can advantageously be achieved by heat treatment.
  • the varistor particles and the electrically conductive particles have been mixed, these particles initially adhere well to the surfaces of the varistor particles.
  • the matrix material for example a polymer, a gel or an oil, for example based on a silicone
  • some of the electrically conductive particles float on the matrix material and then significantly impair the dielectric strength of such a resistance produced in this way .
  • processes initiated by the heat treatment in particular diffusion processes, firmly bond the electrically conductive particles to the surface.
  • floating of the electrically conductive particles on the matrix material is avoided.
  • Loose particles which may be present in the heat-treated filler can preferably be removed by washing, sieving or air sifting before being combined with the matrix material.
  • the temperatures required for the heat treatment are essentially determined by the material of the electrically conductive particles. For silver with a treatment time of approx. 3 h, a heat treatment temperature of approx. 400 ° C has proven to be sufficient. Higher temperatures (up to 900 ° C) are possible, however care must be taken to ensure that the electrical properties of the varistor particles do not change too much. Such changes could occur, for example, through a reaction of the material of the electrically conductive particles with the bismuth phase of the varistor particles.
  • Good surface connections are also obtained in that powder containing varistor particles is dispersed in a metal-containing solution or dispersion, and in that the surface connection is produced by wet-chemical precipitation of the disperse solution or dispersion or by electrochemical or galvanic deposition. This connection can be strengthened by subsequent heat treatment.
  • Solid surface connections between the varistor particles and the electrically conductive particles can also be produced by dispersing a powder containing varistor particles in a metal-containing solution or dispersion, and by subsequent reactive spray drying or spray pyrolysis of the disperse solution or dispersion. Surface coating from the gas phase is also possible, as is advantageously achieved by sputtering, vapor deposition or spraying, for example in a fluidized bed or in a powder stream containing varistor granules and gas.
  • an advantageous surface coating is also achieved by friction contacting.
  • the varistor granules or at least a part thereof and / or the electrically conductive particles in a mixer are added with friction material made of the material to the electrically conductive particles and / or the lining of the mixer contains material of the electrically conductive particles.
  • the surface coating can also be achieved by introducing the varistor granules and the electrically conductive particles into a mechano-fusion system, as is sold, for example, by Hosokawa Micron Europe B.V., 2003 RT Haarlem, Holland.
  • the matrix contains a silicone
  • the adhesive strength of the filler in the matrix is then optimized.
  • adhesion promoters are generally applied to the filler in the form of a thin layer. Suitable adhesion promoters are, for example, silanes, titanates, zirconates, aluminates and / or chelates.
  • the electrically conductive particles can also be added to the adhesion promoter and can therefore be used in an economically particularly advantageous manner in the same application process.
  • Resistor bodies were manufactured, from which test resistors with a volume of a few mm 3 to a few dm 3 were realized by sawing, grinding and attaching two electrodes, for example by coating with a metal such as gold or aluminum. Test specimens were also produced in which the electrodes were cast directly with a casting resin, such as an epoxy or a silicone. The following table shows the compositions of four of these test resistors, where D means the diameter of the particles of the varistor granules.
  • Resistor 1 was state of the art.
  • resistor 3 had a proportion of 5% by volume of the filler in electrically conductive Ni-flakes.
  • the resistor 4 had both a portion of the fine-grained varistor granules amounting to approx. 10% by volume of the filler and an amount of electrically conductive Ni-flakes amounting to approx. 3% by volume.
  • the breakdown field strength U B [V / mm], the nonlinearity coefficient ⁇ B and the maximum power P [J / cm 3 ] were determined on this / ier resistors, as can be seen from the table below.
  • U B and ⁇ a variable DC voltage was applied to the resistors and the resistors were exposed to electrical field strengths between approx. 5 and approx. 500 [V / mm].
  • the current density J [A / cm 2 ] flowing in each of the resistors was determined.
  • the values of U and J determined in this way determined the current-voltage characteristics of the resistors.
  • the breakdown field strength U B of the associated resistor was determined from each of the characteristic curves at a current density of 1.3 ⁇ 3 "4 [A / cm 2 ]. ⁇ 8 was doubled for each of the resistors from the slope of the tangent to the assigned current-voltage characteristic curve taken logarithmically at the point determined by the breakthrough field strength U B.
  • the resistors 2 to 4 with respect to the resistor according to the prior art (resistance 1) ⁇ both by a larger non-linearity coefficient B and are characterized by an increased power consumption P and the lower at the same time the breakdown field strength.
  • this is a result of the improved contacting of the individual varistor particles with one another due to the electrically conductive particles additionally contained in the mixture, and on the other hand, it is a result of a particularly high density of varistor particles.
  • This high density is created by a varistor granulate with two fractions of particles of different sizes, of which the particles of the first fraction have a larger diameter than the particles of the second fraction and are arranged essentially in the form of a dense spherical packing and the particles of the second fraction Fill in the gaps formed by the ball packing.
  • the diameter of the particles of the first fraction are preferably between approximately 40 and approximately 200 ⁇ m. In order to achieve a high density, it is particularly favorable if the diameter of the particles of the second fraction is approximately 10 to approximately 50% of the diameter of the particles of the first fraction, and if the proportion of the second fraction is approximately 5 to approximately 30% by volume the proportion of the first fraction.
EP99915429A 1998-04-27 1999-04-23 Resistance non lineaire a comportement de varistor et procede permettant de produire cette resistance Expired - Lifetime EP0992042B1 (fr)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
DE19824104A DE19824104B4 (de) 1998-04-27 1998-04-27 Nichtlinearer Widerstand mit Varistorverhalten
DE19824104 1998-04-27
PCT/CH1999/000165 WO1999056290A1 (fr) 1998-04-27 1999-04-23 Resistance non lineaire a comportement de varistor et procede permettant de produire cette resistance

Publications (2)

Publication Number Publication Date
EP0992042A1 true EP0992042A1 (fr) 2000-04-12
EP0992042B1 EP0992042B1 (fr) 2005-08-31

Family

ID=7869336

Family Applications (1)

Application Number Title Priority Date Filing Date
EP99915429A Expired - Lifetime EP0992042B1 (fr) 1998-04-27 1999-04-23 Resistance non lineaire a comportement de varistor et procede permettant de produire cette resistance

Country Status (9)

Country Link
US (1) US6469611B1 (fr)
EP (1) EP0992042B1 (fr)
JP (1) JP4921623B2 (fr)
CN (1) CN1145981C (fr)
AT (1) ATE303652T1 (fr)
AU (1) AU751978B2 (fr)
DE (2) DE19824104B4 (fr)
PL (1) PL190068B1 (fr)
WO (1) WO1999056290A1 (fr)

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EP1736998A1 (fr) * 2005-06-21 2006-12-27 Abb Research Ltd. Bande à la propriété de varistor pour le contrôle d'un champ électrique
US7651636B2 (en) 2004-04-06 2010-01-26 Abb Research Ltd Nonlinear electrical material for high and medium voltage applications

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EP1736998A1 (fr) * 2005-06-21 2006-12-27 Abb Research Ltd. Bande à la propriété de varistor pour le contrôle d'un champ électrique

Also Published As

Publication number Publication date
JP2002506578A (ja) 2002-02-26
CN1145981C (zh) 2004-04-14
AU3404399A (en) 1999-11-16
EP0992042B1 (fr) 2005-08-31
ATE303652T1 (de) 2005-09-15
WO1999056290A1 (fr) 1999-11-04
PL337696A1 (en) 2000-08-28
DE19824104B4 (de) 2009-12-24
JP4921623B2 (ja) 2012-04-25
US6469611B1 (en) 2002-10-22
AU751978B2 (en) 2002-09-05
CN1266534A (zh) 2000-09-13
DE59912488D1 (de) 2005-10-06
PL190068B1 (pl) 2005-10-31
DE19824104A1 (de) 1999-10-28

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