High voltage cable for a winding and electromagnetic induction device comprising the same

Abstract

The present disclosure relates to a cable for a high voltage winding of an electromagnetic induction device. The cable includes a conductor having a width w, and a shield arranged around at least a portion of the conductor, wherein in any cross-section of the conductor the conductor has rounded corners with a radius r in the range w/5<rw/3. A high voltage electromagnetic induction device having a cable forming a high voltage winding is also disclosed.

Claims

1. A cable for a high voltage winding of an electromagnetic induction device, comprising: a conductor having a width w, and a shield arranged around at least a portion of the conductor, wherein in any cross-section of the conductor the conductor has rounded corners with a radius r in the range w/5<r<w/3, wherein a space between the conductor and the shield is defined at the rounded corners, wherein the shield is in contact with an outer surface of the conductor, and wherein the outer surface of the conductor is between the rounded corners.

2. The cable as claimed in claim 1, wherein the magnetic material is a polymer magnet.

3. The cable as claimed in claim 1, wherein the outer surface comprises a first sidewall and a second sidewall that is spaced apart from the first sidewall by the width w, wherein the rounded corners comprise at least four rounded corners, wherein the space between the conductor and the shield includes a plurality of spaces that are arranged at the at least four corners, and wherein the first sidewall is between a first two of the at least four corners and the second sidewall is between a second two of the at least four corners that is different from the first two of the at least four corners.

4. The cable as claimed in claim 1, wherein the space formed outside any rounded corner is filled with a magnetic material.

5. The cable as claimed in claim 4, wherein the magnetic material has a relative magnetic permeability r>1.

6. The cable as claimed in claim 4, wherein the magnetic material is a magnetic gel.

7. The cable as claimed in claim 4, wherein the magnetic material comprises magnetic dust or glue mixed with epoxy.

8. The cable as claimed in claim 4, wherein the magnetic material is a magnetic fluid.

9. A high voltage electromagnetic induction device comprising: a magnetic core having a limb, and a cable including: a conductor having a width w, the cross-sectional shape of the conductor being rectangular except for the corners, wherein the width w is defined as the distance between the long sides of the conductor, and a shield arranged along at least one of the sides of the conductor, wherein in any cross-section of the conductor the conductor has rounded corners with a radius r in the range w/5<rw/3, wherein the cable is wound around the limb, forming a high voltage winding, and wherein a space between the conductor and the shield is defined at the rounded corners, wherein the shield is in contact with an outer surface of the conductor, and wherein the outer surface of the conductor is between the rounded corners.

10. The high voltage electromagnetic induction device as claimed in claim 9, wherein the high voltage electromagnetic induction device is a high voltage transformer or a high voltage reactor.

11. The high voltage electromagnetic induction device as claimed in claim 9, wherein a space between the conductor and the shield is defined at the rounded corners, wherein the space formed outside any rounded corner is filled with a magnetic material and wherein the magnetic material is a polymer magnet.

12. The high voltage electromagnetic induction device as claimed in claim 9, wherein a space between the conductor and the shield is defined at the rounded corners, wherein the space formed outside any rounded corner is filled with a magnetic material, and wherein the magnetic material is a magnetic gel.

13. The high voltage electromagnetic induction device as claimed in claim 9, wherein a space between the conductor and the shield is defined at the rounded corners, and wherein the magnetic material comprises magnetic dust or glue mixed with epoxy.

14. The high voltage electromagnetic induction device as claimed in claim 9, wherein a space between the conductor and the shield is defined at the rounded corners, wherein the space formed outside any rounded corner is filled with a magnetic material, and wherein the magnetic material is a magnetic fluid.

15. The high voltage electromagnetic induction device as claimed in claim 9, wherein the outer surface comprises a first sidewall and a second sidewall that is spaced apart from the first sidewall by the width w, and wherein the shield contacts the first and second sidewalls between the spaces.

16. The high voltage electromagnetic induction device as claimed in claim 9, wherein the space formed outside any rounded corner is filled with a magnetic material.

17. The high voltage electromagnetic induction device as claimed in claim 16, wherein the magnetic material has a relative magnetic permeability r>1.

18. The high voltage electromagnetic induction device as claimed in claim 16, wherein the magnetic material is a polymer magnet.

19. The high voltage electromagnetic induction device as claimed in claim 16, wherein the magnetic material is a magnetic gel.

20. The high voltage electromagnetic induction device as claimed in claim 16, wherein the magnetic material comprises magnetic dust or glue mixed with epoxy.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The specific embodiments of the inventive concept will now be described, by way of example, with reference to the accompanying drawings, in which:

(2) FIG. 1 shows eddy current losses for a prior art cable for a winding of an electromagnetic induction device;

(3) FIG. 2 shows a cross-section of an example of a cable for a winding of an electromagnetic induction device;

(4) FIG. 3 depicts a cross-section of an example of cable for an electromagnetic induction device;

(5) FIG. 4a shows a plot of the power loss in a cable for a winding of an electromagnetic induction device, which cable is without shield and without magnetic material acting as filler in the wedges, for different corner radii;

(6) FIG. 4b shows a plot of the power loss in a cable for a winding of an electromagnetic induction device, which cable includes a shield but is without magnetic material acting as filler in the wedges, for different corner radii;

(7) FIG. 4c shows a plot of the power loss in a cable for a winding of an electromagnetic induction device, which cable includes a shield and magnetic material acting as filler in the wedges, for different corner radii;

(8) FIG. 5 is a plot of the power loss in a cable for a winding of an electromagnetic induction device under the same premises as in FIG. 4c however with area compensation; and

(9) FIG. 6 is a sectional view of a portion of a high voltage electromagnetic induction device comprising a winding having been made of a cable shown in FIG. 2 or 3.

DETAILED DESCRIPTION

(10) The inventive concept will now be described more fully hereinafter with reference to the accompanying drawings, in which exemplifying embodiments are shown. The inventive concept may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein; rather, these embodiments are provided by way of example so that this disclosure will be thorough and complete, and will fully convey the scope of the inventive concept to those skilled in the art. Like numbers refer to like elements throughout the description.

(11) The present disclosure relates to a cable for a high voltage winding of an electromagnetic induction device, such as a high voltage transformer or a high voltage reactor. The design of the cable reduces eddy current losses. Eddy current losses may be reduced by providing rounded corners in any cross-section of the cable. The rounded corners may have a radius in the range w/8<rw/2, where w is the width of the conductor forming part of the cable. Typically all of the rounded corners have the same radius.

(12) By rounding the cable corners, the cross-sectional area is decreased, resulting in higher DC losses if the radius of the rounded corners is too large. DC loss is a function of the cross-sectional area of a cable for a winding; the higher the cross-sectional area, the lower the DC loss.

(13) According to one aspect disclosed herein, DC loss compensation for round-cornered conductors is provided by compensating, in the design phase, for any cross-sectional area reduction obtained due to rounding of the corners. DC loss compensation is obtained by, in the design phase, selecting larger conductor dimensions, in particular one of the height and width dimensions of the conductor, or both, with a corresponding amount that has been removed by the rounding of the corners or will be removed by rounding the corners. The cross-sectional area may thus in the design phase be selected so that it after having been provided with rounded corners corresponds to the cross-sectional area of a conductor which has rectangular corners. In this manner both reduced eddy current losses and maintained the DC loss may be provided.

(14) FIG. 1 shows a computer simulation in which high currents flow through a plurality of conductors C1-C4 having a rectangular cross-section and forming part of a high voltage winding. As can be seen, there are high losses in the corners. These losses occur due to the induction of eddy currents by the leakage flux.

(15) With reference to FIGS. 2 and 3 examples of a cable for a high voltage winding of an electromagnetic induction device will now be described.

(16) FIG. 2 shows a cross-section of an example of a cable for a high voltage winding. The exemplified cable 1 comprises a shield 3, and a conductor 5.

(17) The cable 1 may furthermore include an encapsulation configured to encapsulate the shield 3 and the conductor 5, and solid insulation, provided around the encapsulation. The encapsulation may for example comprise an epoxy and the solid insulation may for example comprise a cellulose-based material, such as paper.

(18) The conductor 65 may for example be made of copper or aluminum. In cross-section, each corner 5a of the conductor 5 is rounded, having a radius r. The radius r of each corner 5a is in the range w/8<rw/2. The radius r of each corner 5a may for example be in the range w/6<rw/2, such as w/5<rw/2, or w/4rw/2, or w/4rw/3.

(19) According to the present example, the conductor 5 has a generally elongated cross-sectional shape. The cross-sectional shape is substantially rectangular, except for the corners 5a. The conductor 5 has a width w, which is defined as the distance between the long sides of the conductor 5. The conductor 5 also has a height h defined as the distance between the short sides. According to the present example the width w is smaller than the height h. The height h of the conductor 5 forms part of the height of one winding disc of a winding having been created by means of the cable 1. The width w of the conductor 5 forms part of the width of a winding turn of a winding having been created by means of the cable 1.

(20) The shield 3 at least partly surrounds the conductor 5. The shield 3 is preferably arranged in the leakage flux direction, i.e. parallel with the leakage flux. This typically means that the shield 3 is arranged along a long side of the conductor 5. The shield 3 comprises a magnetic material. The shield 3 is configured to provide magnetic shielding of the conductor 5. The magnetic material of the shield 3 preferably has a relative magnetic permeability r in the range 2 to 100 000. The shield 3 may for example have a thickness which is at least 100 m, preferably in the range 200 to 800 m. Examples of suitable materials and suitable characteristics of the shield 3 are provided in WO2012136754.

(21) According to the present example, the shield 3 is provided along both long sides of the conductor 5. The shield 3 could alternatively be provided around the entire conductor, or it could be provided along the short sides of the conductor, instead of the long sides, or along only one of the long sides or only along one of the short sides.

(22) Since the corners 5a of the conductor 5 are rounded having a radius r, a space 7 is obtained outside each rounded corner 5a. According to one variation, this space 7 is filled with a magnetic material 9. The magnetic material 9 acts as a filler, filling space 7. The magnetic material 9 is preferably a soft magnetic material, by which are meant materials that are deformable, to easily obtain the shape of a space 7. The magnetic material 9 may be any soft magnetic material that has a relative magnetic permeability r greater than 1. The magnetic material may for example be a magnetic gel, or it may comprise magnetic dust or glue mixed with epoxy, or it may be a magnetic fluid such as a ferrofluid. The magnetic material 9 could also be a polymer magnet. Hereto, the encapsulation may according to one variation be a polymer magnet, which fills the spaces 7.

(23) FIG. 3 shows a cross-section of another example of a cable for a winding. Cable 11 is a multi-strand cable and comprises a plurality of conductors 5 arranged in a plurality of rows. According to the present example the number of rows is two, but there could of course instead be more rows than two or less rows than two. Each conductor 5 forms a strand of the cable 11. Each conductor 5 is at least partly surrounded by a shield 3, and all of the conductors 5 have rounded corners, as described in FIG. 1. The cable 11 furthermore comprises an encapsulation 13, for example an epoxy encapsulation, enclosing the conductors 5, and solid insulation 15 enclosing the encapsulation 13.

(24) FIG. 4a shows a plot that illustrates the losses of a cable for a high voltage winding that has no shield and no magnetic material in the spaces 7. The x-axis shows different radii of the corners 5a, from essentially no radius at all at the origin, i.e. a rectangular-shaped conductor, to the maximum radius of half the width, and the y-axis shows the power loss as a function of the radius, from no power loss at all at the origin. Curve 17 shows the DC loss in the conductor. As expected, the DC loss increases with the increase in radius r, since the total cross-sectional area of conductor decreases as the corners are made more and more round. Curve 19 shows the eddy current loss, which decreases as the radius r increases. Curve 21 shows the total loss, i.e. both eddy current losses and DC losses. The total loss is slightly reduced as the corner radius of the conductor is increased, even for the maximum radius, although the DC loss slightly offsets the efficiency provided by the rounded corners.

(25) FIG. 4b shows a plot that illustrates the losses of a cable for a high voltage winding that has a shield 3 but no magnetic material in the spaces 7. The x-axis and the y-axis describe the same parameters as indicated in the previous example. Curve 23 shows eddy current losses in the shield, and curve 25 shows hysteresis losses in the shield, both of which are constant with respect to changes in the radius r of the corners 5a. Curve 27 shows the eddy current loss in the conductor, which again decreases as the radius increases. Curve 29 shows the DC loss in the conductor, which increases with the radius r. Curve 31 shows the total loss, which decreases as the radius increases. The combination of shield and curved radius however provides a much smaller total loss than in the case shown in FIG. 4b; in the present example, the total loss for any radius is about half of the total loss in the example of FIG. 4a.

(26) FIG. 4c shows a plot that illustrates the losses of a cable for a high voltage winding that has a shield 3 and magnetic material in the spaces 7. The x-axis and the y-axis describe the same parameters as indicated in the two previous examples. Curves 33 and 35 show the eddy current losses and the hysteresis losses in the magnetic material, i.e. the filler material, respectively. Curve 37 shows the eddy current loss in the shield, and curve 39 shows the hysteresis loss of the shield in this case. Curve 41 shows the eddy current loss in the conductor, which again decreases with an increased radius. Curve 43 is the DC loss in the conductor, and curve 45 is the total loss. Again, the total loss decreases as the radius r of the corners of the conductor increases. However, with both the magnetic material acting as fillers in the spaces 7 and the shield 13 arranged at least partly around the conductor 5, the total loss has a minimum which is substantially smaller than in the case shown in FIG. 4b. This minimum is located in a radius range r, which corresponds to about w/5 to about w/3 of the conductor 5, i.e., between about one fifth of the width w of the conductor 5 to a width w of about one third of the conductor 5.

(27) The area reduction of the conductor 5 obtained when providing the conductor with rounded corners during manufacturing may be compensated for. The area reduction may be compensated for by using conductor material which has a slightly larger cross-sectional area than what is desired for DC loss purposes, prior to the rounding of the corners. If for example the rounding of the corners reduces the total cross-sectional area by say 3%, one could start with a conductor that has a cross-sectional area of about 103.1% of the desired cross-sectional area. When the corners are rounded, 100% of the desired cross-sectional area will be obtained.

(28) FIG. 5 shows a plot that illustrates the losses of a cable for a high voltage winding that has a shield 3 and magnetic material in the spaces 7, with area compensation of the conductor during production thereof. The x-axis and the y-axis describe the same parameters as indicated in the previous examples. Curves 47 and 49 show the eddy current losses and the hysteresis losses in the magnetic material, i.e. the filler material, respectively. Curve 51 shows the eddy current loss in the shield, and curve 53 shows the hysteresis loss in the shield in this case. Curve 55 shows the eddy current loss in the conductor, which again decreases with an increased radius. Curve 57 shows the DC loss in the conductor, which in the area-compensated case is constant for any radius r. It does not increase with increased an increased radius, like in the non-compensated case shown in FIG. 4c. The total loss shown by curve 59 will therefore be lower for larger radii than in the case without area compensation shown in FIG. 4c.

(29) FIG. 6 shows a portion of a high voltage electromagnetic induction device 61 comprising a magnetic core 63 made of e.g. a plurality of laminated sheets of steel, and a high voltage winding 65. The magnetic core 63 has a limb around which the high voltage winding 65 is wound. The high voltage winding 65 comprises a plurality of turns and windings discs, and comprises a cable with rounded corners of the type disclosed herein. The high voltage winding 65 may hence comprise a cable such as cable 1 or cable 11.

(30) The cable disclosed herein is adapted for being used to construct a high voltage winding of a high voltage electromagnetic induction device, where eddy current losses are non-negligible. Such an electromagnetic induction device may for instance be a transformer such as a power transformer, an HVDC transformer, a reactor or a generator. Hereto, the cable may advantageously be used for high voltage applications.

(31) The inventive concept has mainly been described above with reference to a few examples. However, as is readily appreciated by a person skilled in the art, other embodiments than the ones disclosed above are equally possible within the scope of the inventive concept, as defined by the appended claims.