Object of the present invention is a method and an appar¬ atus for the reduction of distance-dependent voltage in¬ crease of electrodes occurring in an apparatus comprising parallel, rod-like electrodes connected to a high-fre¬ quency voltage source.

Electrode structures of said type are used, for example, in heating and/or drying of various material webs, sheets or layers with high-frequency energy. The material to be treated in said machines is passed close to the rod-like electrodes, several of which are placed in parallel es¬ sentially transversely with respect to the travel direc¬ tion of the material.

The parallel electrodes are alternately connected to the high-frequency power supply for the purpose of forming an electromagnetic field between the electrodes to be di¬ rected to primarily influence the material to be treated. If the material to be treated contains moisture or other¬ wise possesses similar dielectric properties, the high- frequency electromagnetic field that is formed between two electrodes mainly is directed to the material to be treated. If the material also has a high dielectric loss factor, the high-frequency field generates a heating ef¬ fect in the material, which, in turn, results in the de- sired heating and/or drying of the material.

Examples of applications for apparatuses of this type are heating of paper web, wood veneer or textile materials with the aim of drying the material or equalizing their moisture content, heating of layers with which the ma¬ terial are coated or which are absorbed in it, after- treatment of bakery products proceeding on a transport conveyor, heating of a powdery or grainy stuff layer pro-

ceeding on a conveyor, etc.

In most applications, the material to be treated passes as a wide web or mat, across which the electrodes must reach in order to bring about the desired effect. Long electrodes are involved with the well known problem of standing waves causing an increase in the voltage with growing distance from the voltage supply point. In many applications, size restrictions of the apparatus and sim- ilar structural factors enable voltage supply to the electrodes only from one end, at the most from both ends of the electrode, thus limiting the possibilities to eli¬ minate the voltage increase.

As is well-known, the above structures have provided a solution for the reduction of voltage increase, in which iductive coils are connected between adjacent electrodes at fixed intervals. This arrangement provides a service¬ able solution for the reduction of voltage increase, in case it is applicable as far as the other apparatus structure is concerned. In paper and wood veneer dryer, for instance, in which some 5-metre electrodes and an alternating voltage frequency of 13.56 MHz are used, the solution is capable of keeping the voltage within the range of ± 5% of the initial voltage (1.5 kV) along the entire electrode. Said solution requires two inductive coil connections along the rods.

The above known technology, based on the use of so-called centralized compensating coils, suffers, however, from certain problems in a system containing several parallel electrodes. The structure is unfavourable in terms of space need. It is also prone to getting dirty, and a dirty apparatus is difficult to clean. Inaccuracy in di- mensioning of the apparatus, caused by the mutual induc¬ tances of the compensating coils further presents a func¬ tional problem.

A solution for the elimination of the voltage increase occurring in the electrodes, based on a different prin¬ ciple, has been introduced in the Finnish patent specifi- cation 55922. In this solution, the electrodes are com¬ bined into groups of two electrodes, and for them is ar¬ ranged a common supply by using a supply conductor lo¬ cated between the electrodes at an equal distance from them. Supply points are favourably chosen at several points between the ends of the electrodes. By taking the frequency of the used alternating voltage properly into account when choosing the supply points, a compensating effect to the voltage in the electrodes can be achieved. Compensating of the electrode voltage is also influenced by the fact that the current of the supply cable and the current of the electrode at part of the electrode become opposite, and consequently the resulted induced magnetic fields are also opposite and partly effect in the compen¬ sating of the voltage occurring in the electrode.

The effect of said, known apparatus can be substantially achieved in the desired form only when current is supplied to both ends of the conductor located between the electrodes. Although the apparatus specifically was developed to reduce problems occurring in long electrodes (electrode length smaller than approximately one fifth of the used wavelength) , said current supply inevitably causes problems with such electrodes. Either is an own generator to be used for both supply ends, one at each side of the apparatus, or the other supply end is to be equipped with long conductors. Two separate generators tend to cause problems, the most crucial of which in terms of operation is synchronization of the generators. On the other hand, the use of long conductors may add to the problem of voltage increase, that originally was to be solved.

In this known structure, however, the ^* number of connec¬ tion points between the supply conductors and the elec¬ trodes according to the operating principle of the appar¬ atus is restricted. If current is supplied at both ends of the supply conductor, the supply points are limited to two additional points over the length of the electrodes. If current is supplied to one end of the supply conduc¬ tor, current supply to the electrodes can only be rea¬ sonably implemented at one additional point along the electrode. The circumstances referred to above restrict the maximum length of the electrodes to no more than one fourth of the wavelength, as mentioned in the publica¬ tion.

According to the basic idea of the invention, the same compensating effect of the opposite magnetic fields generated by the reverse currents in compensating of the electrode voltage is used as in publication FI 55922, although implemented in such a way that the restrictions characteristic of the system known from publication FI

55922 can be avoided. According to the basic idea of the invention this can be achieved so that a magnetic field opposite to the magnetic field of the electrode is gene¬ rated by arranging a return path for the electrode cur- rent from the compensating point at a distance from the electrode ensuring the avoidance of any electric dis¬ charges, and reaching to the distance to be compensated, and by connecting this return path essentially at its end with the corresponding return path of each adjacent elec- trode possessing an opposite potential.

The special forms of implementation of the method accord¬ ing to the invention are shown in the enclosed dependent claims.

To the apparatus to implement the method according to the invention, it is characteristic that a compensating con-

ductor is arranged in the vicinity of each electrode, the conductor passing at least at a distance from the elec¬ trode ensuring the avoidance of any electric discharge, and reaching over a part of the length of the electrode; that the compensating conductor is connected to the com¬ pensating point of the electrode at its end away from the current supply point of the electrode, and, at its other end, to the end of the corresponding compensating conduc¬ tor of each adjacent electrode.

The invention is described based on the enclosed sche¬ matic drawing, in which Figure 1 illustrates a principal implementation of the method according to the invention for the heat treatment of web-like material, and

Figure 2 illustrates a modification of the method.

Figure 3 shows a modification of the adjustment of the compensating coil.

Figure 1 shows an apparatus intended for the heating treatment of material 1 passing as a continuous web. Ma¬ terial 1 can be supposed to be, for instance, paper web. The apparatus comprises electrodes 2 arranged to lie across the web and being alternately connected to the opposite potentials of the high-frequency power supply G. According to the invention, a conductor 3 is conducted from the opposite end of each electrode with respect to the power supply end, installed substantially parallel to the electrode. Conductor 3 is conducted at such a dis¬ tance from its electrode 2 that the air gap that is form¬ ed guarantees a sufficient electric breakdown strength. Conductor 3 is stretched over a substantial part of the length of electrode 2, which in practice has proved to be at least two-thirds of the electrode length.

At the end range of the conductors, short-circuit ele-

ments 4 are arranged, by which the conductor can be con¬ nected to the corresponding conductor of the adjacent electrode. Conductor 3 of two adjacent electrodes and the short-circuit element 4 connecting them to each other form a compensating coil. The short-circuit elements can be displaced in longitudinal direction with respect to conductors 3 in order to adjust the compensating induc¬ tance to be accurate in each case.

Many factors must be considered when dimensioning an ap¬ paratus of said type to ensure that the desired end re¬ sult is achieved. The first basic factor is the mutual distance of the electrode rods 2 in the travel direction or web direction of the material to be processed. The need of voltage to be supplied to the electrodes in¬ creases with growing distance. The increased supply volt¬ age, in turn, influences the compensating inductances. When operating the apparatus on radio frequencies, the mutual distance of the electrodes may vary case by case from a few centimetres to tens of centimetres, for example, to dimensions of some 20-30 centimetres. A di¬ mension of 10-15 centimetres can be considered a general value.

The distance of the inductance coil from the electrodes is primarily determined according to the electric break¬ down strength. The distance can also be used to affect the compensating inductance; at the greater a distance the inductance coil is located from the electrodes, the smaller the inductance effect is. This circumstance can be used for adjusting the compensation effect by varying the distance of the inductance conductors from the elec¬ trode at various points of the compensating range. A dis¬ tance of some 20 centimetres can be considered the maxi- mum distance between the electrode and the inductance conductor. The diameter of both the electrode and the inductance conductor also has its own effect on the di-

mensioning of the apparatus. The minimum diameter is de- termiηed by the heating caused by the current to be con¬ ducted. A diameter of some 10-40 mm can be considered conventional, although dimensions even up to some 100 mm occur.

As distinct from the basic implementation form presented in the drawing figures, the electrode rods may also be connected over an inductance or a capasitance to the ad- jacent rod at the opposite end with respect to the cur¬ rent supply end in order to bring about a phase displace¬ ment between the rods. When using long electrodes, the arrangement can be applied in which compensating points are located in sequence over the length of several electrodes 2.

In the implementation of Figure 2, for the sake of sim¬ plicity two parallel electrodes 2 and the compensating inductance coil generated for them are illustrated. In compliance with the solution of Figure 1, the compensat¬ ing inductance coil is formed by conductor 3 connected to the electrode at the compensating point, which is con¬ ducted at least at the distance of said electric break¬ down strength from the electrode. To add the compensat- ing inductance to the coil, the adjacent coil conductors 3 are connected to each other by an additional coil 7, which is equipped with a short-circuit element 4 provided for the adjustment of inductance at its end.

When dimensioning the compensating inductance coil of the voltage increase, the so-called transmission line theory can be applied as a numerical basis, by which, based on given simplifying assumptions, approximative values may be determined for the inductances, and diameter of the inductance conductors and distance from the electrode, if the approximative length according to the two-wire calcu¬ lation model is known. When defining the length, the re-

ducing effect of the inductance coil on the electrode inductance must be considered, which, in addition to other uncertainty factors, results in the need of adding some 10-20% to the calculated length of the inductance coil. The final adjustment of the inductance is carried out by experiments on the displacement of the short-cir¬ cuit element 4.

In the following paragraph, a tangible dimensioning example is presented to illustrate the above.

A stray-field electrode system is given, with which a 4- metre wide, thin material web, e.g. paper web is heated by using the current supply frequency of 13.56 MHz. Diam- eters of the electrodes are 50 mm and their mutual dis¬ tance is 200 mm. The voltage value is assumed to be 5 kV. The required air gap between the inductance conductor and the electrode thus is 50 mm (1 kV/cm) . A diameter of 15 mm is chosen for the conductors of the compensating in- ductances in order to keep the heat development in the conductors under control. The dimension of 3.5 m of the loop, parallel to the electrode, is numerically achieved. To this dimension, an adjusting margin of some 10% is to be added, and thus it can be established that the coil reaches over some 95% of the electrode length.

As distinct from the above adjustment of the compensating inductances based on varying of the location of the short-circuit elements A , Figure 3 shows an implementa- tion alternative to this adjustment. In the range of the end of each conductor 3, a short-circuited inductance coil is located, which is arranged to be adjusted in the longitudinal direction of conductors 3 at its position. By this adjustment at position, the magnitude of the compensating inductance may be influenced.