Electric furnace and method for its operation

Abstract: The present invention relates to a furnace for very high working temperatures, and to a method of operating such a furnace. This high temperature - above 1800°C - is achieved by using resistor elements of stabilized zirconium dioxide. An electrically heated furnace according to the invention includes an inner furnace chamber (15) provided with resistor elements (2) of stabilized zirconium dioxide, and an outer furnace chamber (13) in which further resistor elements (17) that can work at temperatures above 1800°C in an oxygen-containing atmosphere are provided. The outer resistor elements (17) are conveniently of a molybdenum silicide type, for instance elements marketed under the designation KANTHAL Super. Those walls (22,23,19,24) that delimit the inner furnace chamber are comprised of zirconium dioxide material or some other suitable material that has a low specific thermal conductivity and capable of withstanding the high working temperature and the occurrent temperature swings. The outer chamber, which completely surrounds the inner chamber, is delimited to the surroundings by conventional walls (5,8,9,12,14) insulated, e.g., with ceramic fibres and/or high-temperature durable brick.

Description: The present invention relates to a method pertaining to the operation of high-temperature electric furnaces. The invention also relates to a furnace of this kind. More specifically, the present invention relates to a furnace for very high operating temperatures, viz temperatures in the range of 1800-2000°C and higher, and also to a method of operating such furnaces. Temperatures in excess of 1800°C are achieved with the aid of electric resistor elements, for instance resistor elements comprised of stabilized zirconium dioxide. Resistor elements for electric furnaces are made of different materials. Metallic materials can be used for temperatures up to about 1400°C. It is possible to use elements of molybdenum disilicide for temperatures up to about 1850°C. For temperatures higher than these temperatures, the elements may be comprised of graphite, stabilized zirconium dioxide and other materials. When used in oxidizing atmospheres, the resistors may be comprised solely of oxidic material, such as stabilized zirconium dioxide, for instance. Neither stabilized zirconium dioxide nor resistor elements based on stabilized zirconium dioxide are electrically conductive at room temperature. The material, however, becomes conductive at higher temperatures, and marked current strengths are obtained through a zirconium dioxide element in the temperature range of 700-1000°C. The conductor resistance of the material thereafter falls with rising temperatures. The material thus has a negative temperature coefficient. Consequently, in order to be able to use zirconium dioxide resistor elements in electrically heated furnaces, it is necessary to pre-heat the elements so that they are able to reach a temperature at which they are sufficiently electrically conductive to begin to work. Hitherto, this pre-heating of the elements has been achieved by using metallic resistor elements in different furnace constructions. In furnace constructions for working temperatures above 1800°C, ceramic material based on stabilized zirconium dioxide is also used for the walls, floor and ceiling of the furnace since it is found that this material is able to withstand these high temperatures better than other materials. Furnace constructions that include zirconium dioxide elements thus comprise an inner furnace chamber which is delimited by walls, floor and ceiling comprised of stabilized zirconium dioxide material. One or more resistor elements of stabilized zirconium dioxide are mounted in the inner furnace chamber. The inner walls are surrounded by an external insulation, preferably a ceramic fibre insulation. Metallic resistor elements, e.g. elements made of an iron-chromium-aluminium alloy, are embedded in this insulation at a sufficient distance from the inner furnace chamber. It is also known to arrange the latter resistor elements in an outer furnace chamber which is insulated from the surroundings. The aforesaid outer elements are used to pre-heat the furnace to a temperature at which the zirconium dioxide elements can begin to work. Because the maximum temperature to which the metallic elements can be subjected is considerably lower than the working temperature in the inner furnace chamber, the thickness of the insulation must be such as to ensure that the maximum temperature capable of being with-stood by the metallic elements will not be exceeded. This results in high thermic inertia of the furnace and consequently very long pre-heating and cooling times. It is also necessary to halt the supply of energy to the metallic elements when the furnace is in operation, in order to prevent overheating of said elements. The zirconium dioxide elements are produced in the form of straight rods or tubes. The elements have a hot zone in the centre thereof and are provided at each outer end with a wire lead-in having a cross-sectional area which is larger than the hot zone. Both the hot zone and lead-ins are preferably comprised of yttrium stabilized zirconium dioxide, mutually of the same composition. To enable the transfer of energy from an external source of electric current to the elements, platinum wires are wound around the lead-ins at a suitable distance from the hot zone, and passed out through openings in the furnace chamber. Because of the high working temperature, the supply of energy to the elements cannot be controlled in a usual manner with a temperature sensor mounted in the furnace. One method of regulating the furnace is to control the power supplied as a function of time on the basis of values obtained with experience. This method does not provide any absolute control over the temperature in the furnace chamber and results in a high degree of uncertainty, among other things because the properties of the elements vary with time. The object of the present invention is to enable the use of zirconium dioxide elements in a manner which lengthens the useful life of said elements and of the platinum windings on the lead-ins. Another object of the invention is to enable the working temperature in the furnace chamber to be controlled and adjusted more accurately. Still another object of the invention is to provide a furnace construction which affords shorter start-up times and more rapid heating, and also more rapid cooling. The present invention thus relates to a method of operating an electrically heated furnace having an inner chamber provided with inner resistor elements of stabilized zirconium dioxide, and an outer chamber having outer resistor elements comprised of another material, wherein the invention is characterized in that the outer chamber wall that is proximal to the surroundings has a higher thermal conductivity than the outer chamber wall that is proximal to the inner chamber of said furnace; and in that for the purpose of maintaining a predetermined operating temperature in the inner chamber of the furnace, the resistor elements in the outer furnace chamber are supplied with power sufficient to maintain a requisite temperature in the outer furnace chamber at a predetermined power input to the resistor elements in the inner furnace chamber, and therewith maintain a heat balance between the inner chamber, the outer chamber and the surroundings. The invention also relates to a furnace of the aforesaid kind having essentially the features set forth in Claim 12. The invention will now be described in more detail, partly with reference to an exemplified embodiment of the invention, and also with reference to the accompanying drawings, in which Figure 1 is a vertical cross-sectional view of an inventive furnace as seen from the front; Figure 2 is a horizontal cross-sectional view of an inventive furnace as seen from above; Diagram 1 illustrates temperature as a function of time during a working cycle; Diagram 2 illustrates the development of power in the furnace shown in Figures 1 and 2; and Figure 3 illustrates schematically control means. An electrically heated inventive furnace includes an inner furnace chamber provided with resistor elements comprised of stabilized zirconium dioxide, and an outer furnace chamber provided with further resistor elements which can operate at temperatures of up to 1800°C in an oxygen-containing atmosphere. The outer resistor elements are suitably of a molybdenum disilicide type, for instance resistor elements marketed under the designation KANTHAL Super. The walls, ceiling and floor defining the inner chamber are comprised of stabilized zirconium dioxide material or some other appropriate ceramic material, such as a material chosen from the group hafnium dioxide, thorium dioxide or yttrium oxide or other oxides or oxide combinations that have low thermal conductivity and are able to withstand the aforesaid high temperature and occurrent temperature changes. A typical value with regard to the thermal conductivity of stabilized zirconium dioxide at 1650°C is 0.144 W / m °K. The outer furnace chamber completely surrounds the inner furnace chamber and is delimited to the surroundings by high-grade fibre ceramic material on the front and the rear side of said furnace chamber. Externally of the inner furnace chamber is a chamber in which the molybdenum disilicide elements are placed. The outer side walls of this outer furnace chamber are comprised of a material that has a considerably higher thermal conductivity than stabilized zirconium dioxide, such as aluminium oxide brick, for instance. The outer resistor elements are freely mounted in the furnace chamber, i.e. are not embedded in the insulating material. The outer elements will preferably have a length such that radiation emitted thereby will directly reach parts of the lead-in conductors of the zirconium dioxide elements. The outer elements are of a conventional kind and include a U-shaped hot zone and lead-in conductors which are made from the same material as the hot zone but are larger or coarser than said zone. The outer side walls of the outer furnace chamber, comprised of aluminium oxide, are freely radiating on the outside so as to permit sufficiently effective heat emission from the molybdenum silicide elements, such that said elements will remain activated during a full working cycle. The temperature is controlled with the aid of a PtRh 6/30-type thermocouple in the outer chamber for regulating the supply of energy to the outer resistor elements, and with optical temperature control in the inner chamber, for regulating or controlling the supply of energy to the zirconium dioxide elements. According to one preferred embodiment of the invention, the thermal conductivity of the outer furnace chamber wall that faces or lies proximal to the surroundings will preferably be so high in comparison with the thermal conductivity of the outer furnace chamber wall that faces towards or lies distal to the inner furnace chamber that when a predetermined operating temperature prevails in the inner furnace chamber, the resistor elements in the outer furnace chamber will be operated with at least 10% of maximum power, so as to maintain a predetermined temperature in the outer furnace chamber. According to another preferred embodiment, which may exist simultaneously with the aforesaid embodiment, there is maintained in the outer furnace chamber a temperature which is at least 50%, preferably 75%, of the temperature in the inner furnace chamber measured in degrees Celsius, at a predetermined operating temperature in the inner furnace chamber. The furnace illustrated in Figures 1 and 2 has an inner furnace chamber 15 and an outer furnace chamber 13. The inner furnace chamber is delimited by a ceiling 6, a bottom 7 and side walls 1. The side walls, ceiling and bottom are suitably comprised of ceramic material, preferably stabilized zirconium dioxide. The inner furnace chamber rests on beams and columns made of zirconium dioxide material 10. The inner furnace chamber is supported at each of the four corners by aluminium-oxide corner pillars 12. The ceiling and bottom of the inner furnace chamber are provided with holes through which lead-ins 3 pass to respective zirconium dioxide elements, whose hot zones 2 are located in the inner furnace chamber. The lead-ins 3 are comprised of the same material as the hot zones 2, i.e. of yttrium oxide stabilized zirconium dioxide. Electrical energy is supplied through lead-ins 4 comprised of platinum/rhodium wires. The wires are wound round the lead-ins 3 at the position where said lead-ins pass through the ceiling of the outer furnace chamber, and the platinum wires extend therefrom out of the furnace. The outer furnace chamber is delimited by a ceiling 11, which has a self-supporting construction, a bottom or floor 16, and walls 14. According to one preferred embodiment of the invention, the walls that delimit the outer furnace chamber from the surroundings are comprised of one of the materials aluminium oxide brick and aluminium oxide fibre material. The outer furnace chamber has provided therein resistor elements 17 which are preferably comprised of molybdenum disilicide material. The lead-ins to these elements extend out through the ceiling 11 of the outer furnace chamber. The elements are typically U-shaped. Arranged in the outer furnace chamber 13 is a thermocouple 18 for sensing the temperature in the outer furnace chamber. The temperature of the outer furnace chamber is controlled with the aid of this thermocouple. The temperature in the inner furnace chamber is controlled with the aid of an optical pyrometer which measures the temperature with the aid of fibre optics. According to one preferred embodiment in which the temperature of the outer furnace chamber is measured with the aid of a thermocouple, the temperature of the inner furnace chamber is measured with the aid of a pyrometer connected to the inner furnace chamber by means of a fibreoptic cable (21). It is preferred that the temperature in the outer furnace chamber is measured at a point located between the outer resistor elements and the wall of the inner furnace chamber. The furnace is provided with an outer insulation of fibre material 5. The furnace opening is comprised of an outer door 9 and an inner door 19. The illustrated and described furnace is a box-type furnace. Moving of the furnace opening to the bottom of the furnace makes the construction suitable for an elevator furnace. It will be understood, however, that the present invention is not restricted to any particular type of furnace and that it can be applied to all types of furnace. According to one highly preferred embodiment of the invention, at least a part of the outer furnace chamber wall 15, 27 that lies proximal to the surroundings has a thermal conductivity which is higher than the thermal conductivity of the remainder of said wall 5; 8, 9, where resistor elements 17 are provided at least at and inwardly of said part of the wall of said outer furnace chamber 13. According to one highly preferred embodiment of the furnace, in which the aforesaid embodiment is applied and also the method of operating said high temperature furnace, the outer resistor elements 17 are provided at two first opposing sides 22, 23 of the walls of the inner furnace chamber, while the two remaining, second opposing sides 24, 25 of the walls of the inner furnace chamber are devoid of outer resistor elements. The walls of the outer furnace chamber facing the surroundings are constructed so that the thermal conductivity of the two opposing walls 26, 27 of the outer furnace chamber that are placed externally of said first sides 22, 23 of the inner furnace chamber will be higher than the thermal conductivity of the two opposing walls 28, 29 of the outer furnace chamber that are placed externally of said second sides 24, 25 of the inner furnace chamber. Consequently, in the locations where the outer resistor elements are placed, the thermal conductivity of the outer walls will be higher than the thermal conductivity of the two remaining walls. As a result, there is obtained a "wall" at the first opposing sides of the inner furnace chamber which includes the outer furnace chamber and its outer wall whose "insulating capacity" against the inner furnace chamber can be regulated or controlled by means of the temperature in the outer furnace chamber, this temperature being regulated or controlled by the supply of energy to the outer resistor elements. By permitting considerable heat transport through those parts of the outer wall of the outer furnace chamber where the molybdenum elements are placed, it is feasible to say that the insulating capacity of said wall can be controlled electrically by the supply of energy to the molybdenum elements. That which is regulated or controlled in actual fact is the temperature on the outside of the wall of the inner furnace chamber, which in turn controls the temperature gradient and therewith the transportation of heat through the wall of the inner furnace chamber. One advantage afforded by the described and illustrated furnace construction is that a uniform and effective temperature control is achieved on the outtake parts of the zirconium dioxide elements and the platinum wire connections thereto, via the communicating spaces above and beneath the inner furnace chamber. This also means that the temperature will be smoothly controlled in the absence of shocks or surges, therewith contributing towards improving the useful life span of the components in the furnace construction. A furnace construction of the aforedescribed kind also enables the use of zirconium dioxide elements of much larger dimensions than is possible in the earlier known furnace constructions. This affords additional advantages in the form of considerably improved mechanical properties. Because the aforesaid insulating capacity can be regulated by the power applied to the outer elements, the furnace can be cooled much more quickly than known furnaces of this kind. Because the mass in the insulation of the outer furnace chamber to the surroundings is low in comparison with known furnaces, the start-up time is also shorter than in the case of these known furnaces. According to one preferred embodiment, the supply of energy to the inner resistor elements is regulated and controlled by measuring the temperature in the inner furnace chamber. Similarly, the supply of energy to the outer resistor elements is regulated or controlled by measuring the temperature in the outer furnace chamber. According to one preferred embodiment of the invention, as illustrated below, the supply of energy to the inner and the outer resistor elements respectively is regulated in accordance with the prevailing temperature in both the inner and the other furnace chamber, at least time-wise. A control device which functions to this end is described below. Diagram 1 illustrates the course followed by the temperature during a working cycle of a furnace according to Figure 1, and for zirconium dioxide elements and molybdenum silicide elements in the furnace. One important advantage afforded by an inventive furnace is that part of the energy is supplied during the whole of the working cycle with the aid of resistor elements in the outer furnace chamber. Thus, these elements are not switched-off when the furnace reaches its working temperature, as in the case of earlier known furnace constructions of this kind. The outer furnace chamber is also heated to high temperatures, although not higher than to prevent the use of a conventional thermocouple for sensing the temperature in said chamber, and also not higher than the temperature that has been preset for this chamber. This presumes that the material in the wall of the inner furnace chamber will have very low thermal conductivity, wherewith stabilized zirconium dioxide is a suitable material also for this reason. The energy delivered by the outer resistor elements is regulated with the aid of the sensed temperature. The temperature in the inner and the outer furnace chambers is controlled with the aid of a respective control instrument, each of which is provided with an individual program. The supply of energy to the inner elements is controlled and regulated with the aid of an optical sensor which measures the temperature in the inner furnace chamber with the aid of fiber optics. The supply of energy to the outer furnace chamber is controlled and regulated with the aid of a thermocouple. Each of the two sensors is connected to a respective conventional control instrument. The temperature control instruments are connected to one another in a manner such as to enable said instruments to send signals to one another at given pre-programmed temperatures. The furnace is preferably controlled so that energy is supplied to the outer resistor elements 17 when starting-up the furnace and so that energy is also supplied to the inner resistor elements 2 when the inner furnace chamber 15 has been heated to a predetermined temperature. When the temperature in both furnace chambers has reached approximately the same level during the heating process, the energy supplied to the outer element 17 is lowered to a level which is less than half of the earlier power input. However, the inner resistor elements can be supplied with energy right from the very beginning. Diagram 2 shows the power development in a furnace according to Figure 1, both totally and for the inner and the outer resistor elements individually. The power development has been plotted as a function of time during a working cycle. The total power supplied to the furnace comprises the sum of the power delivered to the outer and the inner resistor elements. The power development in the inner resistor elements is shown in the diagram by a line P ZrO2 . The power development in these elements does not begin until a temperature of 700-1000°C is reached, prior to which the material has no marked electrical conductivity. The power development then rises continuously up to the working temperature obtained, whereafter the power development is held constant. The resistor elements in the outer furnace chamber show a rising power development, particularly during the first part of the starting-up period. The power development in the outer resistor elements reduces markedly before or after reaching working temperature in the inner furnace chamber, due to the heat delivered through the wall of the inner furnace chamber to the outer furnace chamber, and reaches a state of equilibrium at a value of about 25% of the power development in the inner elements. This is shown by the line marked P MoSi2 . The total power developed in the furnace is shown by the line P Tot . Energy is thus supplied during the whole of the working cycle, also from the outer resistor elements. The energy required to maintain or sustain the temperature in the outer furnace chamber is obtained both from the molybdenum silicide elements and from the energy transported through the wall of the inner chamber of the furnace. This total amount of energy shall balance the energy that is lost through the outer aluminium-oxide wall of the outer chamber of the furnace, so as to maintain the outer chamber of said furnace at the pre-programmed temperature. This contributes towards maintaining a high and well-controlled temperature in the inner chamber of the furnace. Upon completion of the heat treatment process, a signal is sent from the temperature control equipment of the inner chamber to the temperature control equipment of the outer chamber, therewith breaking off the supply of energy to the outer resistor elements. The temperature of the inner resistor elements is also lowered at the same time in accordance with a given programme and the power developed in the inner elements decreases. The temperature can rise extremely quickly when starting-up the furnace, for instance at a rate of 7° per minute. This is considerably quicker than in the case of the known furnace constructions described in the introduction, in which pre-heating is effected with metallic elements, and gives a shorter working cycle than said known constructions. The regulating or control means will now be briefly described with reference to Figure 3. The regulator means may include two different regulating devices, one for the outer chamber 13 and one for the inner chamber 15 of said furnace. Each regulating device includes a control circuit 30, 31 of some suitable known kind. Each control circuit is adapted to detect a real value from respective sensors in the form of said thermocouple 18 or said pyrometer 21. Each control circuit includes a microprocessor or the like programmed to cause the control circuit to activate a power regulating means 32, 33 in accordance with the temperature prevailing in the outer and/or the inner chamber of the furnace. The power regulating devices will suitably comprise thyristors or corresponding devices. The power regulating devices control the power delivered to the elements. When the two control circuits are intended to activate respective elements in accordance with the temperature in both of said furnace chambers, a signal line 34 is provided between the control circuits 30, 31. As will be understood, the two described control circuits 30, 31 can be integrated to form a single control circuit, as indicated by the broken line 35 in Figure 3. Although the invention has been described in the aforegoing with reference to a number of exemplifying embodiments thereof, it will be obvious that variations can be made. For instance, the furnace geometry may be different to that illustrated, and one or more of the furnace walls may comprise other materials having corresponding mechanical strength and thermal properties. The present invention is thus not restricted to the aforesaid exemplifying embodiments thereof, since variations and modifications can be made within the scope of the following Claims.

Claims: A method of operating an electrically heated furnace having an inner chamber provided with inner resistor elements of stabilized zirconium dioxide, and an outer chamber having outer resistor elements comprised of another material, characterized in that the outer chamber wall (5, 8, 9, 12, 14) which delimits the outer chamber from the surroundings has a higher thermal conductivity than the inner chamber wall (1, 19) which delimits the inner chamber (15) of said furnace; and in that for the purpose of maintaining a predetermined operating temperature in the inner chamber of the furnace, the resistor elements (17) in the outer furnace chamber are supplied with power sufficient to maintain a requisite temperature in the outer furnace chamber (13) at a predetermined power input to the resistor elements (2) in the inner furnace chamber (15), and therewith maintain a heat balance between the inner chamber (15), the outer chamber (13) and the surroundings. A method according to Claim 1, characterized in that at least a part of the outer chamber wall (14, 27) that is proximal to the surroundings has a thermal conductivity which is higher than the thermal conductivity of the remainder (5; 8, 9) of said wall; and in that resistor elements (17) are provided at least at and inwardly of said part of the outer chamber wall. A method according to Claim 1 or Claim 2, characterized in that the thermal conductivity of the outer chamber wall (5, 8, 9, 12, 14) that is proximal to the surroundings is so high in comparison with the thermal conductivity of the outer chamber wall (1, 19) that is proximal to the inner chamber (15) that at a predetermined operating temperature in the inner chamber the resistor elements in the outer chamber will be operated with at least 10% of the maximum power in maintaining a predetermined temperature in the outer chamber (13). A method according to Claim 1, 2 or 3, characterized in that a predetermined operating temperature in the inner chamber (15), there is maintained in the outer chamber (13) a temperature which is at least 50%, preferably 75%, of the temperature in the inner chamber (15) measured in degrees Celsius. A method according to Claim 1, 2, 3 or 4, wherein the temperature of the outer chamber is measured by means of a thermocouple (18), characterized by measuring the temperature of the inner chamber (15) by means of a pyrometer connected to the inner chamber (15) by means of a fibreoptic cable (21). A method according to Claim 1, 2, 3, 4 or 5, characterized in that the outer resistor elements (17) are located at two first opposing sides (22, 23) of the inner chamber walls; and in that the two remaining, second, opposing sides (24, 25) of the inner chamber walls are devoid of outer resistor elements; in that the thermal conductivity of the outer chamber walls that is proximal to the surroundings is chosen such that the thermal conductivity of the two opposing outer chamber walls (26, 27) that are placed outside said first sides (22, 23) of the inner chamber will be higher than the thermal conductivity of the two opposing outer chamber walls (28, 29) that are placed outside said second sides (24, 25) of the inner furnace chamber. A method according to Claim 1, 2, 3, 4, 5 or 6, characterized in that the supply of energy to the inner resistor elements (2) is controlled and regulated by measuring the temperature in the inner chamber (15). A method according to Claim 1, 2, 3, 4, 5, 6 or 7, characterized in that the supply of energy to the outer resistor elements (17) is controlled and regulated by measuring the temperature in the outer chamber (13). A method according to Claim 8, characterized by measuring the temperature in the outer chamber (13) at a point between the outer resistor elements (17) and the inner chamber wall (23). A method according to any one of the preceding Claims, characterized by controlling the supply of energy to the inner and the outer resistor elements (17) respectively in accordance with the temperature prevailing in both the inner (15) and the outer (13) chamber, at least time-wise. A method according to Claim 10, characterized by delivering energy to the outer resistor elements (17) when starting-up the furnace; delivering energy to the inner resistor elements (2) when a predetermined temperature has been reached in the inner chamber (15); reducing the supply of energy to the outer elements (17) to a level corresponding to less than half the earlier supplied power, when the temperature in the two furnace chambers has reached approximately the same temperature level during the heating process. An electrically heated furnace having an inner furnace chamber with inner resistor elements of stabilized zirconium dioxide and an outer furnace chamber having outer resistor elements of another material, characterized in that the outer chamber (13) wall (5, 8, 9, 12, 14) which delimits the outer chamber from the surroundings has a higher thermal conductivity than the inner chamber wall (1, 19) which delimits the inner furnace chamber (15); in that a control device functions to activate the resistor elements (17) in the outer chamber (13) at a predetermined power input to the resistor elements (2) in the inner chamber (15) such that said resistor elements (17) are supplied with sufficient power to maintain a requisite temperature in the outer furnace chamber and therewith maintain a predetermined operating temperature in the inner chamber, and therewith a heat balance between the inner chamber (15), the outer chamber (13) and the surroundings. An electric furnace according to Claim 1, characterized in that at least a part of the outer chamber wall (14, 27) that is proximal to the surroundings has a higher thermal conductivity than the thermal conductivity of the remainder (5; 8, 9) of said wall; and in that resistor elements (17) are provided at least at and inwardly of said part of said outer chamber wall. An electric furnace according to Claim 12 or Claim 13, characterized in that the thermal conductivity of the outer chamber wall (5, 8, 9, 12, 14) that is proximal to the surroundings is higher than the thermal conductivity of the outer chamber wall (1, 19) that is proximal to the inner chamber (15); and in that control means are provided for supplying the resistor elements (17) in the outer chamber (13) with at least 10% of the maximum power at a predetermined operating temperature in the inner chamber (15). An electric furnace according to Claim 12, 13 or 14, characterized in that at a predetermined operating temperature in the inner chamber (15), said control means functions to maintain in the outer chamber (13) a temperature which is at least 50%, preferably 75%, of the temperature in the inner chamber, measured in degrees Celsius. An electric furnace according to Claim 12, 13, 14 or 15, wherein the temperature of the outer chamber is measured by means of a thermocouple (18), characterized in that the temperature of the inner chamber (15) is measured by a pyrometer connected to the inner chamber by means of a fibreoptic cable (21). An electric furnace according to Claim 12, 13, 14, 15 or 16, characterized in that said outer resistor elements (17) are provided at two first opposing sides (22, 23) of the inner chamber walls; in that the two remaining, second, opposing sides (24, 25) of the inner chamber walls are devoid of such resistor elements; in that the outer chamber walls proximal to the surroundings are adapted such that the thermal conductivity of said two opposing outer chamber walls (26, 27) placed outside said first inner chamber walls (22, 23) will be higher than the thermal conductivity of the two opposing outer chamber walls (28, 29) that are placed outside said second inner chamber sides (24, 25). An electric furnace according to any one of Claims 12-17, characterized in that the outer resistor elements (17) are of a molybdenum disilicide type. An electric furnace according to any one of Claims 12-18, characterized in that the walls (1, 19) dividing the inner chamber are comprised of one of the materials from the group stabilized zirconium dioxide, hafnium dioxide, thorium dioxide or yttrium oxide or mixtures thereof. An electric furnace according to any one of Claims 12-19, characterized in that the walls (5, 8, 9, 12, 14) that delimit the outer chamber (13) against the surroundings are comprised of one of the materials aluminium oxide brick and aluminium oxide fibre material. An electric furnace according to any one of Claims 12-20, characterized in that said control means functions to control the supply of energy to the inner (2) and the outer (17) resistor elements in dependence on the temperature prevailing in both the inner (15) and the outer (13) furnace chamber, at least time-wise.

Inventors: BIZZARRI VENANZIO, BIZZARRI, VENANZIO
Applicants: KANTHAL AB
Application year: 1996
Main classification: F27B17
IPC codes: F27D23, F27D1, H05B3, F27B3, F27D21, F27D11, F27B5