DEVICE FOR PROTECTION

Abstract: A device for protecting against overcurrents includes at least one body (10) of an electrically conductive elastomeric material, and two electrodes. The defining surface of the elastomeric body is intended to abut with and be deformed against a surface of at least one other body (11, 12). The device also includes a resistor (15a, 15b, 16a, 16b), which is connected in parallel to the elastomeric body (10).

Description: DEVICE FOR PROTECTION. TECHNICAL FIELD The present invention relates to a protective device for protecting against overcurrents in electric circuits, said device comprising at least one electrically conduc¬ tive body and two electrodes which function to supply circuit current through said conductive body and which lie against the body at corresponding positions either directly or through the medium of an intermediate part, and further comprising pressure means for generating an abutment pressure. The device is primarily intended for use in low voltage systems having an operating voltage of at most 1000 V. BACKGROUND ART Current limiting elements, or when using the terminology of the art, short circuiting protectors. are mainly comprised of fuses and circuit-breakers which most often possess current limiting properties. The technique is known to the art and several standards, such as IEC 269 concerning fuses, and IEC 947-2 concerning circuit-breakers, have been insti¬ tuted. The short-circuiting protector is excited by the short circuiting currents flowing therethrough. The shortcircuiting protector is excited in accordance with two main principles and is therefore divided here into the following groups 1 and 2: 1. Fuses, thermistors with positive tem-perature coef¬ ficients and self-restoring short- circuiting pro¬ tectors described in U.S. Patent Specification 3,886,551 are excited when short- circuiting "cur¬ rents flow therethrough as a result of the increa- sed ohmic power development in the protector. When the applied electrical energy has caused a tempera¬ ture increase in the protector corresponding to the melting point of vital material in the protector an increase in resistance occurs and limitation of the short-circuiting current begins. 2. Arc-based, current limiting cut-outs, for instance circuit-breakers are excited directly, through the conversion of magnetic energy to mechanical energy, by electrodynamic current forces occurring on the electrical contact system included in the circuit- breaker, or indirectly through the medium of a separate excitation device comprised of an electro¬ magnetic release device, a so-called "plunger or schlagstiftanordnung", which is also excited by the main current. An armature included in a magnetic circuit acts on the electrical contact system and/or on a spring mechanism release device which performs an on/off-function. Remote control is also used, for instance in contactors, for maintaining two stable mechanical states of equilibrium, on and off respectively. Electrical contact systems in which electrodynamic current forces act directly on the electrical contacts are earlier known to the art, for instance from Patent Specifications GB 1,519,559, GB 1,489,010, GB 1,405,377. Hybrids in which the two principles are used are dis¬ closed in Patent Specification GB 1,472,412 and in the article "A New PTC Resistor for Power Applications" by R.S. Perkins, et al, published in the journal IEEE Transactions on Components, Hybrids and Manufacturing Technology, Vol. CHMT-5, No. 2, June 1982, pages 225-230 and publications U.S. 3,249,810 and DE 35 446 47, among others . One serious drawback with short-circuiting protectors according to groups 1 and 2 above, particularly in the case of high and steep (= rapidly growing) short cir¬ cuiting currents, resides in the high intrinsic inertia. Thermal inertia has a limiting effect on the short¬ circuiting protectors described under group 1 above whereas in the case of arc-based circuit-breakers it is the mechanical inertia, i.e. the mass inertia, which becomes significant when wishing to separate the elec¬ trical contacts quickly. As a result of the mass iner¬ tia, the arc is delayed on the electrical contacts in arc-based circuit-breakers, and consequently the arc voltage, important in achieving current limitation, will not reach the values at which the otherwise monotonously growing short circuit current is limited until a rela¬ tively long delay time (ms) has lapsed. Furthermore, a very high contact pressure, proportional to the square of the rated or nominal current of the apparatus, is required in order for the electrical contacts to be able to carry rated current under normal operating currents. This also prevents the electrical contacts from separat¬ ing quickly, since the contact pressure is opposed to the electrodynamical repelling and separating forces. The possibility of adjusting the sensitivity of the short-circuiting protectors described under categories 1 and 2 above is highly limited. Consequently, there is required a comprehensive coordination work? with main and subordinate protectors included in electric cir¬ cuits. Standards have therefore been worked-out, for instance DIN 57636 Teil 21/VDE 0636 Teil 21 § 7,12 and IEC 947-2, since erroneous coordination may, among other things, incur selectivity problems which are difficult to rectify (adjust) in existing systems. As a result of the aforesaid drawbacks, and in particu¬ lar inertia, short-circuiting protectors based on the principles disclosed in categories 1 and 2 above are less suited as short-circuiting protectors or current transient protectors for thyristors or electronic equip¬ ment, since they are sensitive to both high current derivatives and high short-circuiting currents can also occur in capacitive circuits or inductive motor circuits with high presumptive short-circuiting currents. Typical values of presumptive short-circuiting currents are Ik = 50-100 kA and corresponding current time deriva¬ tives from 22-44 kA/ms. With a rated current of 100 A, a conventional fuse will then allow a current peak of 2 2 about 16 kA and / i -dt«20 kA s to pass through, which greatly exceeds the permitted values of corresponding thyristors. Consequently, chokes are often included in thyristor circuits in order to reduce current deriva¬ tives, therewith enabling the aforedescribed short¬ circuiting protector to be used. A self-restoring short-circuiting protector is mainly comprised of so-called thermistors. The expression PTC- element is an accepted designation of thermistors whose resistivity has a Positive Temperature Coefficient. Electrically conductive polymer compositions, particu¬ larly PTC-compositions, and devices in which PTC-compo- sitions are included are known to the art. Reference in this regard can be made to U.S. Patent Nos. 2,978,665, 3,351,882, 4,017,715, 4,177,376 and 4,246,468, and also to U.K. Patent No. 1,534,715. Later developments are described, for instance, in German Patent Nos. 2,948,350, 2,948,281, 2,949,174 and 3,002,721, and also in various Patent Applications, such as U.S. Serial Nos. 41,071 (MPO 295), 67,207 (MPO 299) and 88,344 (MPO 701), and Patent Applications? such as U.S. Serial Nos. 141,984 (MP = 712), 141,987 (MPO 713), 141,988 (MPO 714), 141,989 (MPO 715), 141,991 (MPO 720) and 142,054 (MPO 725) . One problem with PTC-elements is that when heated by the current flowing therethrough and the temperature is reached at which the PTC-elements become self-adjusting, the voltage is taken over by a fragment of the PTC- element and the fragment is subjected to very high stresses, which are liable to destroy the PTC-element. PTC-embodiments in which this problem is eliminated are known, for instance, from European Patent EP 0,038,716. PTC-elements for overload protectors are often construc¬ ted of a polymeric material, for instance high-pressure polyethylene, containing particles of an electrically conductive material, for instance lamp black or carbon black, and exhibit a resistivity with high positive temperature coefficient. Ceramic thermistors which exhibit PTC-characteristics are known from Patent Publication GB-A-1,570,138. The most common ceramic thermistors are based on BaTiO or 3 One advantage afforded by the polymer-based thermistor in comparison with the ceramic thermistor is that its resistance increases monotonously with temperature. It is also relatively cheap to produce. However, commer¬ cially available polymer-type thermistors are designed for relatively low rated or nominal voltages and cannot therefore be used readily . in distribution networks for instance. Furthermore, the configuration and electrode connections of the thermistors are normally such that the thermistors are subjected to large repulsion forces at high short-circuiting currents, as a result of " anti- parallel current paths, therewith tearing the electrodes apart. It is also known that sandwich-type, polymer- based PTC-elements do not return to the initial resis¬ tance after passing from a low resistive state to a high resistive state. In more serious cases, when the PTC- elements are subjected to very high electrical stresses, such as short-circuiting currents, bubbles and cracks form in the central parts or in other parts of the polymer composition of the PTC-element, so that the element will no longer function, i.e. the element is destroyed. For these reasons, polymer-based thermistors have not hitherto been used to any appreciable extent in practice within electric power technology, but have mainly only been used to protect electronic equipment, although the thermal inertia limits the fields of possible appli¬ cation. An essential difference between thermistors and fuses is that thermistors will self-restore after a short-cir¬ cuit, i.e. thermistors can be reused after a short- circuit, which also applies to circuit-breakers. Elastomers are comprised of all polymers that exhibit elastic properties which are similar to those exhibited by natural rubber. Elastomers can be compressed or stretched within a relatively large permitted elastic area, and return to their original state when the load is removed. Electrically conductive elastomers are a class of rubber and plastics which have been made elec¬ trically conductive, either by the addition of metal mixtures or by orientating metal fibres under the influ¬ ence of electric fields, or by the addition of different carbon mixtures or ceramics, for instance V203-material dispersed in the manner described in the article "V203 Composite Thermistors" by D. Moffat, et al , published in Proceedings of the Sixth IEEE International Symposium on Applications of Ferroelectrics, 1986, pages 673-676. In rubber, there is used several types of "carbon black", for instance graphite, acetylene black, lampblack and furnace black with particle diameters ranging from 10-300 nm. Examples of appropriate rubber materials which become electrically conductive after adding metal mixtures or carbon mixtures are butyl, natural, poly- chloroprene, neoprene, EPDM, and the most important silicone rubber. Additives of metals and metal alloys in powder form suited as elastomer additives are silver, nickel, copper, silver-plated copper, silver-plated nickel, and silver-plated aluminium. Electrically conductive elastomer are used as pressure transducers within transducer technology. The electrical properties are changed when electrically conductive elastomers are deformed, for instance as a result of being subjected to pressure or tension,' which manifests in a change in resistance. The most common types of carbon or metal-filled plastics are polyethylene and polypropylene. These are used at present for heating cables and for overload protectors, for instance the earlier mentioned polymer-based PTC- thermistors. However, the inclusion of an electrically conductive filler impairs the mechanical properties of the plastic. The material becomes brittle and hard and is therewith not readily deformed. These materials are therefore unsuitable as pressure transducers and also require a relatively complicated contacting technique for PTC-applications. A further limitation of carbon-filled plastics resides in their relatively high resistivity, which is typically one 1 Ohmcm and higher. On the other hand, metal-filled plastics can be produced with signi¬ ficantly lower resistivity, lower than 0.5 Ohmcm, al¬ though voltage or tension stability becomes very poor, and consequently these materials are not suited as overload protectors. Electrically conductive elastomers can be given very low resistances, for instance resistances of 2 mOhmcm or lower, by admixing metal powder. One advantage afforded by elastomers is that they are very soft in comparison with carbon-filled polyethylene and polypropylene, even when containing large quantities of electrically conduc¬ tive filler. Such elastomers will have a typical Shore number of between 20-80, according American Standard ASTM D2240 (Q/C) . DISCLOSURE OF THE INVENTION The object of the present invention is to provide a relatively simple and inexpensive overload protector which is able to limit the highest short-circuiting currents that occur in a low voltage network, even at very high current derivatives, and the release charac¬ teristic of which, i.e. its response sensitivity, can be adapted readily to the object to be protected. This object is achieved in accordance with the invention with a protective device having the characteristic features set forth in the following Claim 1. By deforming at least one curved or convex-defining surface of an electrically conductive elastomeric body included in the current limiting element with the aid of a pressure means, and by integrating electrodes which are active in conducting current through the current limiting element, there is achieved a significantly more effected current limitation than that obtained with conventional short-circuiting protectors described under the heading "Background Art". This results in consider¬ able cost advantages, particularly on the downstream side of the current limiting element. The device can replace both conventional fuses and so-called automatic circuit-breakers (MCB) , and possesses the advantages afforded by both of these types of circuit-breaker without suffering their disadvantages, such as the limited length of life of the fuse and the limited circuit breaking ability of the automatic circuit-break¬ er on short-circuiting occurrences. The device which functions as a current limiting element includes at least one electrically conductive elastomer- ic body and two electrodes. The polymer composition of the elastomeric body may be of any known kind and forms no part of the present invention. Examples of suitable elastomers in this respect are particularly butyl, natural, polychlorpropene, neoprene, EPDM and silicone rubber. The electroconductive powder material is prefer¬ ably comprised of silver, nickel, cobalt, silver-plated copper, silver-plated nickel, silver-plated aluminium, lampblack, conductive soot or carbon black. The powder material will suitably have a particle size of 0.01-10 micro-meters and the powder filler is suitably present in an amount corresponding to 40-90% of the combined weight of the powder filler and elastomeric material. The resistivity of the electric elastomeric body will preferably lie within the range of 0.1 mohmcm-10 Ohmcm. When the device includes more than one electrically conductive elastomeric body, the bodies may be made of mutually the same or mutually different elastomers and then with mutually the same or mutually different fill¬ ers and resistivity. The electrodes are of a convention- al kind, for instance silver-plated copper. The elec¬ trodes are preferably orientated so that repu " - * .:.on forces will occur between the electrodes when high currents pass therethrough. The pressure achieved on the electrodes, for instance with a known pressure device described in U.S. 3,914,727, or by a conventional spring mechanism for the on/off function of an electric switch, deforms the convex abutment surface of the elastomeric body, when the device includes such an abutment surface. This deformation will preferably reach at least 5%. A deformation of 5-30% is particularly preferred, as defined with a starting point from the distance between the bodies that borders on a considered elastomeric body, i.e. if the distance when the pressure is 0 and bordering bodies lie in abutment with the elastomeric body is d and if the distance changes to 0.7•d after the pressure has been applied, the body will have been deformed by 30%. Particularly preferred elastomeric bodies are those which have a hardness between 30-50 IRHD in accord with British Standard BS903/A26, although materials having both a lower and a higher hardness may conceivably be used. Preferred embodiments of the invention are evident from the subordinate claims. It has been found possible by means of the present invention to counteract or totally eliminate the draw¬ backs described under the heading "Background Art", such as insensitivity, etc., 'of the overload protector. The resistance of the current limiting element changes when high short-circuiting currents occur at a lower energy development, therewith reducing the thermal and mechani¬ cal inertia. Furthermore, subsequent to having passed from a low-resistive to a high-resistive state, the current limiting element will return to the original resistance and is therewith reusable even after being subjected to the effect of short-circuiting currents. One conceivable reason for the result achieved by the present invention may be as follows: With the normal passage of current, a low transition resistance is" maintained between those elements which are in contact with one another through the transition surface which is formed when the body having a convex abutment surface or the bodies, when more than one such body is included, are deformed by an external pressure device. When high short-circuiting currents occur, the electrodes will separate as a result of current forces. Furthermore, so- called striction forces occur in the transition between the convex abutment surface of the elastomer bodies, when one such abutment surface is included, and border- ing bodies, due to the configuration of the preferred abutment surface. This results in a reduction of the abutment surface, partly because an elastomeric body having a convex abutment surface can be deformed and partly because the electrodes will separate. As a re- suit, energy development increases more rapidly in the decreasing transition surface, causing the resistance of the elastomeric body at the transition surface to con¬ siderably increase without the remainder of the elasto¬ meric body being subjected to impermisslbly high stress- es. Furthermore, as a result of the cross-sectional configuration of the preferred elastomeric body, the current density is greatest along the symmetry line of the cross-sectional surface between the electrodes, meaning that the material is under the greatest stress in this region, therewith preventing the formation of cracks and bubbles in the cross-section at right angles to the current direction. Among other things, the following advantages are ob- tained in a current limiting device when the physical properties described in the Background Art are combined, for instance such properties as pressure response of electrically conductive elastomers, transition surfaces, the electrodynamic repulsion effect that is achieved by suitable geometric configuration of electrically conduc¬ tive elastomeric bodies and electrodes, together with a suitable choice of electrode material: a) Considerably increased sensitivity at high current derivatives and short-circuit currents, due to a resilient pressure device and preferred electrode configuration, which together with the particularly configured electrically conductive elastomeric body will repel the electrodes. b) The device can be made very low-ohmic, because of deformation of the contact transition between elec¬ trically conductive elastomeric body and electrode. c) A smaller selectivity problem in electric circuits which include main and subordinate protectors. d) The element returns to its initial resistance after passing from a low-resistive state to a high-resis¬ tive state. e) A simple circuit breaking device which may possibly not require the provision of arc shields when the electrodes are connected mechanically to a conven¬ tional on/off mechanism for circuit-breakers which in the on-position maintain the requisite pressure between electrode (= contact) and electrically conductive elastomeric body. f) Eliminated welding risk when a circuit-breaker arrangement according to point e) above is includ¬ ed. g) A vibration-insensitive and rebound-insensitive switch-on function. h) The possibility of adjusting the sensitivity of the device when the pressure maintained by the pressure device can be adjusted and varied in a known man¬ ner, thereby enabling one and the same overload protector to be used in an extended rated current range. i) Very small external dimensions, since the electri¬ cally conducting elastomer material can be given a very low resistivity < 1 mohmcm. j) The provision of exclusive chokes in thyristor circuits can be avoided. BRIEF DESCRIPTION OF THE DRAWINGS The present invention will now be described in more detail with reference to exemplifying embodiments there¬ of and also with reference to the accompanying drawings, in which Figures la-c are central sectional views of three pre¬ ferred embodiments of one part of the invention, this part mainly comprising electrically conductive elastomeric bod- ies and electrodes; Figure 2 illustrates the resistance R as a func¬ tion of the distance d between two elec¬ trodes between which an electrically con- ductive elastomeric body of semi-cylin¬ drical cross-section of radius r is com¬ pressed; Figure 3 illustrates one embodiment of an inven- tive current limiting element connected in an electric circuit; Figure 4 illustrates the course of the current in the event of a short-circuit with an ele¬ ment according to Figure 3; Figure 5 shows a comparison between i I l • •£ ■dt curves for an inventive current limiting element and a conventional protector, such as a fuse and circuit-breaker, MCCB; Figures 6-7 are central sectional views of an inven¬ tive elastomeric body and associated el¬ ectrodes, and also a repulsion means; and Figures 8-19 illustrate further variants of inventive current limiting elements. Figure 20a is a sectional view of an inventive de¬ vice for protecting against overcurrents; Figure 20b shows the device illustrated in Figure 20a connected in an electrical circuit; Figure 20c is a diagram relating to the relationship between ά(A) and t(ms) ; Figure 21a is a slightly modified form of the device illustrated in Figures 20a; Figure 21b is a side view of the device illustrated in Figure 21a; Figures 22a and 22b are slightly modified forms of the device illustrated in Figures 20a and 21; Figure 23 is a modified form of the device illus¬ trated in Figure 22; Figures 24a and 24b illustrate a particularly preferred emb¬ odiment of the novel device; Figure 24c is a curve relating to the relationship between R(ohm) and X(m) ; and Figures 25a-d illustrate arrangements in a further em¬ bodiment of the novel protective device. Figure 6 illustrates a current limiting element in accordance with an arrangement analogous with the ar¬ rangement illustrated in Figure lb. The current limiting element includes a centrally mounted body (10) in the form of a homogenous cylinder having a diameter of 3 mm and length of 10 mm and being made of a" deformable electrically conductive elastomer material, for instance comprising 80 percent by weight silver powder and 20 percent by weight silicone plastic, and two mutually parallel electrodes (11, 12) which are tangential to the body (10) on opposite sides thereof. In the case of the illustrated embodiment, the elastomeric body (10) has a Shore number of 40 according to BS 903/A26. The elec¬ trodes (11, 12) are comprised of angled, silver-coated copper plates having a thickness of 0.7 mm. The elec¬ trodes are held in abutment with the body (10) with the aid of a spring device (14) which exerts pressure on the electrodes (11, 12) in a known manner and therewith deform the abutment surfaces (10 , 10") of the body against respective electrodes, this deformation being about 30%. The sensitivity or response of the arrange- ment can be enhanced by including a repulsion device (13) of the kind described, for instance, in GB 1,519,559 or GB 1,489,010, or the electrodes may be constructed so that they themselves will give rise to repelling electrodynamic current forces. Alternatively, the repulsion device (13) may be a self- activating magnetic circuit of the kind earlier des¬ cribed in U.S. 4,513,270, which is intended to act solely on one electrode and which is directed so that the electrodes will separate from one another under the action magnetic forces or electrodynamic current forces. The resistance across the device is 2 Ohm. When the device is subjected to high short-circuiting currents, preferably currents above 50 A, and more particularly above 500 A, the current density will increase in the deformed abutment surfaces (10', 10"), wherewith the resistance in the element will increase to 100 mOh or more. This is sufficient to limit short-circuiting currents in low voltage systems, which through the agency of the preferred arrangement in "Figure 6 and the circuit illustrated in Figure 3 limits the short¬ circuiting currents and produces the current-time dia¬ gram shown in Figure 4. Figure 7 illustrates a current limiting element which is similar to the element illustrated in Figure 6 and Figure lc with the exception that the elastomeric body (20) is not an homogenous body. Thus, the body of the Figure 7 embodiment includes a cavity (9) which enables deformation of the elastomeric body to be increased to 30% or more, depending on the dimensions of the cavity. This enables a material of relatively high Shore number to be used, for instance a Shore number of 80. The body (20) is preferably deformable so that the resultant convex abutment surface (9') will be in physical contact with the abutment surface (9"). Figure 8 illustrates an embodiment of the invention in which two electrically conductive elastomeric bodies (iθa, 10b) have been stacked one upon the other, whereas the electrically conductive elastomeric bodies (10a, 10b) of the Figure 9 embodiment have been placed side- by-side. Figures lOa-b illustrate an inventive device in which an electrically conductive elastomeric body (10) according to Figure 7 is placed between two electrodes (11, 12) which extend longitudinally parallel with the body (10). The pressure applied to the electrodes and the elasto¬ meric body abutment surfaces (10', 10") is obtained- through the agency of the earlier described resilient pressure device. Figure 11 illustrates an inventive device in which an electrically conductive elastomeric body (10) is placed between two electrodes (11, 12) according to Figures lOa-b. A ferromagnetic repulsion circuit (13) surrounds the longitudinally extending electrodes (11, 12) and the elastomeric body (10), and amplifies the repulsion effect of electrode (11) when overcurrents flow through the current limiting element. Pressure is applied to the electrodes and the elastomeric body abutment surfaces (10', 10") by the aforedescribed resilient pressure device. Figure 12 illustrates a device which is analogous with the device shown in Figures lOa-b with the exception that the electrically conductive elastomeric body (10) is semi-cylindrical in shape and may be firmly anchored to the electrode (12) by means of an electrically con¬ ductive adhesive, or may lie free. Figure 13 illustrates an inventive device • which two electrically conductive elastomeric bodies (10a, 10b) are placed between two electrodes (11, 12), between wltiich a further two elastomeric bodies (10c) and (lOd) respectively have been placed, these further bodies surrounding the electrodes (11, 12). Pressure is applied to the electrodes, and particularly to the elastomeric bodies provided with convex end-surfaces, by the afore¬ said, known pressure device. Figure 14 illustrates a further embodiment of the inven¬ tion according to the Figure 12 and Figure 9 embodi¬ ments, in which the elastomeric bodies (10c, 16a) and (10e, 16b) respective surrounding electrodes (11, 12) are comprised respectively of electrically conductive elastomer material (10c, lOe) and electrically insulat¬ ing elastomeric material (16a, 16b). The respective elastomeric bodies (10c, 16a) and (lOe, 16b) are advan¬ tageously moulded in a two-part mould, so that the elastomeric bodies will be mutually joirned, and the electrodes are electrically insulated..The electrical connections to the electrodes are not shown in the Figure. Figure 15 illustrates an inventive device according to Figures 6 and 7, in which two electrically insulating, polyethylene bodies (15a, 15b) are disposed parallel with an electrically conductive elastomeric body (10). When the device is subjected to pressure, as symbolized by the force F acting on the electrodes (11, 12), the body (10) is deformed and will therewith lie against the defining surfaces (15a') and (15b') of the electrically insulating bodies. There is obtained in this way an electric insulation which prevents flashover in the event of a short-circuit, at the same time as the elec- trically conductive elastomeric body will not flow outwards, which is otherwise a common problem. Figure 16 illustrates an inventive device in which the electrically conductive elastomeric body (10) includes several convex deformable abutment surfaces (10a', 10b', 10c', 10d'), comprising several integrated elastomeric bodies according to earlier Figures. The elastomeric body (10) is coherent and homogeneous. Figure 17 illustrates an inventive device in which the electrically conductive elastomeric body (10) has a convex deformable abutment surface in a "spline configu¬ ration" , comprising several integrated elasto e-ric bodies according to earlier Figures. The elastomeric body (10) is thus coherent and several convex surfaces can be activated, for instance by in¬ creasing the pressure with the aid of the pressure device (14) . Figures 18a-b illustrate an inventive device which is comprised of two electrically conductive elastomeric bodies (20a, 20b) having convex deformable abutment surfaces (20a', 20b'), and two electrodes (11, 12). The electrodes are surrounded by concentrical, electrically conductive elastomeric bodies (20a, 20b) whose abutment surfaces (20a', 20b') are in physical abutment with one another. The abutment surfaces (20a', 20b') are deformed by pressure exerted by a pressure device (14). The electrodes (11, 12) are provided with electrical con¬ necting means (31) and (32) respectively. Figure 19 illustrates an inventive device in which the electrically conductive elastomeric bodies (lOal, 10a2, 10a3, 10a4) have convex-defining surfaces which are orientated perpendicularly to the convex-defining sur- faces of the electrically conductive bodies (lObl," 10b2, 10b3, 10b4). The device includes two electrodes (11, 12) for conducting current therethrough, electrodes on which a pressure device exerts pressure such as to deform the abutment surfaces (lOal...lObl... ) . It will be understood that the invention is not restric¬ ted to the illustrated embodiments thereof and that more variants are conceivable within the scope of the follow¬ ing Claims. For instance, the number of mutually stacked electrically conductive elastomeric bodies according to Figure 8 may be considerably more than has been shown. Figure 20a illustrates a device in which two polymer- based thermistors 15a and 15b are connected in parallel to the elastomeric body 10. Also included is a fix resistor 16a, 16b. Figure 20b is a circuit diagram in which the broken line 17 symbolizes the entire protec¬ tive device, i.e. the elastomeric body, electrodes, resistors and thermistors. By suitable mutual dimensioning of the .components 10, 15 and 16 of the inventive device, the polymer-based therm¬ istor 15 will function as an "energy absorber" during short-circuiting. This prevents overloading of the elastomeric body 10. The fix resistor 16 can then be permitted to be much larger than when the thermistor 15 is not found. This will be understood from the following energy consideration (c.f. Fig. 20c). Magnetic energy when the current reaches il is Wl = L*il**2/2. Magnetic energy when the current reaches i2 is W2 = L*il**2/2. Magnetic energy when the current reaches i3 is W3 = L*i3**2/2. The energy, which is absorb-- ' by the elastomeric body 10 in the transition from a low resistive to a high resis¬ tive state, is Wl_2 = Wl -W2. Because the polymer-based thermistor can be allowed to be low resistive during the commutation stage, Wl_2 will be « W1-W3 = Wl_3, where Wl_3 is the energy that is absorbed by the elastomeric body 10 when no polymer-based thermistor is present. The current limiting element according to Figure 20 is readily adapted to circuits which include superordinate and subordinate short-circuiting protectors, i.e. in which full selectivity can be readily achieved in, for instance, distribution systems within the low voltage range. The embodiment illustrated in Figure 20 also enables the elastomeric body 10 to be made thinner, i.e. enables the distance between the electrodes 11 and 12 to be reduced. This fact is utilized in the embodiment illustrated in Figure 21. Figure 21 illustrates a device according to Figure 20 in which the elastomeric body 10 is much thinner than in the Figure 20 embodiment. This improves, the heat trans¬ fer from the elastomeric body 10 to the electrodes, at the same time as power generation is reduced as a result of the thinner elastomeric body. This means that an increase in the rated current of the current limiting element can be allowed. Figure 21b is a side view of the current limiting element. The electrode 12 has been "split up" into several electrodes, referenced 12', 12", 12'" and 12'"'. This results in a current limiting element which is more receptive during short-circuiting, since essentially adiabatic conditions prevail. This receptiveness or sensitivity of the current limiting element is enhanced by the "valve action" indicated by the currents 30 in Figure 21, and the surfaces 31 where current displacement takes place. Figure 22a illustrates a device according to Figures 20- 21 in which the fix resistor 15 is comprised of two excitation coils or a known firing pin? device, found in automatic fuses for instance (=MCB) . The firing pin device or the excitation coils activate a contact system (50), either directly (40) or indirectly (41), via a mechanism according to Figure 22b, so that the circuit will be broken. Figure 23 illustrates a device according to Figure 22. As distinct from the Figure 22 embodiment, the .excita¬ tion coils/firing pin device act on at least one elec¬ trode (11, 12). This is symbolized by the arrow (45) ' in Figure 23. The electrodes are therewith mutually dis- placed during short-circuiting. The elastomeric body therewith "exercised", which has been found advantageous with regard to the return time to a low resistive state for instance. Naturally, certain turns of the coils may be connected in series to the elastomeric body, so as to enhance the responsiveness of the elastpmeric body 10 (see Fig. 23b (45')(and 45")). Figure 24 (a-c) illustrates a particularly preferred embodiment of a polymer-based thermistor (15a, 15b) in the device. The resistance of an infinitesimal element of cross-sectional area dA varies as indicated by the curve in Figure 24c. In the event of a short-circuit, the polymeric material in zones adjacent to the elasto¬ meric body (10) will first pass from a low to a high resistive state. This process continues until the whole of the thermistor (15) is "through-tripped" if the circuit has not previously been broken. This results in gentle commutation of the current (c.f. Figs. 20a-c) and an improved energy absorbing thermistor. Figures 25a-d illustrate an embodiment of the invention in which an internal excitation device (13) is imple¬ mented by electrodes (11 and 12) of helical configura¬ tion. In this case, repulsion forces, Fr, occur between the electrodes (11) and (12) when short-circuit currents flow through the electrodes. These repulsion forces act to mutually separate the electrodes, which results in greater sensitivity of the overcurrent protector. The sensitivity or responsiveness of cascade-coupled ele- ments can be varied by means of separate connecting devices 19a and 19b, as illustrated in Figures -25c-d. In the case of series connection, the repulsion force Fs will be approximately four times greater than that obtained with a parallel coupling Fp at the same current in total.

Claims: CLAIMS 1. A device for protecting against overcurrents in electric circuits, comprising at least one electrically conductive body (10) which is comprised of elastomeric material, and two electrodes (11, 12) which are intended to supply circuit current through said body and each of which is in abutment with the body (10) at corresponding positions, either directly or through the intermediary of an intermediate part, and in which abutment pressure is obtained through the medium of a pressure device (14), characterized in that the body (10) includes elastomeric material; in that the body (10) and/or at least one electrode/intermediate part in the absence of pressure is curved but is deformed by the pressure device at respective abutment sites when subjected to pressure, so that the abutment surface will decrease with passing overcurrents, wherein - with respect to said deformation - the electrode/intermediate part shall also include elastomeric material; and in that the device also includes a resistor (15a, 15b, 16a, 16b) and/or a capacitor connected in parallel with the elas¬ tomeric body (10). 2. A device according to Claim 1, characterized in that the elastomeric bodies included in the device have a Shore number between 20-80. 3. A device according to any one of Claims 1 and 2, characterized in that the resistor is a polymer-based thermistor (15). 4. A device according to Claim 3, characterized in that the thermistor has an increasing resistance charac- teristic (18). 5. A device according to any one of Claims 1-4, char¬ acterized in that the pressure device (14) is resilient; and in that the abutment pressure applied by the pres¬ sure device is preferably adjustable. 6. A device according to any one of Claims 1-5, char¬ acterized in that at least one resistor (16) is an excitation device which includes at least one coil (16', 16") for activation of a contact device (50) and/or one of the electrodes (11, 12). 7. A device according to any one of Claims 1-6, char¬ acterized in that the pressure device (14) is comprised of a spring mechanism which has two mechanically stable states of equilibrium, on and off respectively; and in that at least one electrode (11a) is mechanically coher¬ ent with the spring mechanism (14) for galvanic separa¬ tion between electrodes (11 and 12). 8. A device according to any one of Claims 1-7, char¬ acterized in that the electrodes (11, 12) are construct¬ ed to repel one another under the influence of short circuiting currents. 9. A device according to any one of Claims 1-8, char¬ acterized in that the electrodes (11, 12) are provided with ferromagnetic circuits (13) which function to amplify the repelling force between said electrodes. 10. A device according to any one of Claims 1-10, characterized in that at least one of the electrodes (11, 12) is divided into several electrodes (12', 12", 12'", 12""), of which at least one covers a limited part surface (31) of the total defining surface (32) of the elastomeric body. 11. A device according to any one of Claims 1-10, characterized in that elastomeric bodies (20a, 20b) are expandable over the electrodes (11, 12). 12. A device according to any one of Claims 1-11, characterized in that the pressure device (14) functions to compress the body (10) to at least 5%, preferably to 5-40% when the body is homogenous. 13. A device according to any one of Claims 1-12, characterized in that the elastomeric body (20 includes a cavity (9) .

Inventors: KARLSTROEM PER OLOF, KARLSTROEM, PER, OLOF
Applicants: KARLSTROEM PER OLOF, SELDIM I VAESTERAAS AK, KARLSTROEM, PER, OLOF, SELDIM I VAESTER ANGSTROM S AKTIEBOLAG
Application year: 1993
Main classification: H02H9
IPC codes: H01C7, H01H77, H01H85, H02H9