ELECTRIC REACTOR OF CONTROLLED REACTIVE POWER AND METHOD TO ADJUST THE REACTIVE POWER

Abstract
An electric reactor of controlled reactive power is formed by a magnetic core, and at least one primary winding to which a main current is supplied to generate a main magnetic flow on the magnetic core. The reactor also includes at least a generator of the magnetic distortion field to which a control current is supplied to generate a field of magnetic distortion on the magnetic core. The magnetic distortion field is opposed to the main magnetic flow generating a distortion of the latter, achieving a change in the magnetic core reluctance and in this way a change in the reactive power of consumption of the reactor. In addition, a method is described to adjust the reactive power in an electric reactor.
Description

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The characteristic details of the present invention are described in the following paragraphs, together with the figures related to it, in order to define the invention, but not limiting the scope of it.



FIG. 1 is a perspective view of an electric reactor of controlled reactive power according to the present invention.



FIG. 2 shows a lateral schematic view of a magnetic core of an electric reactor of controlled reactive power with the presentation of the direction of a main magnetic flow, distorted by magnetic distortion fields according to the present invention.



FIG. 3 shows a schematic view of an illustration presenting a magnetic distortion field generated according to the present invention.



FIG. 4 shows a block diagram of a method to adjust the reactive power of an electric reactor according to the present invention.



FIG. 5 shows a diagram with different magnetizing curves of an electric reactor according to the present invention.





DETAILED DESCRIPTION OF THE INVENTION


FIG. 1 shows an embodiment of the invention referring to an electric reactor with controlled reactive power 10, which has a magnetic core 20 of a column type consisting of a central column 30 and two external columns 40 and 50, all remaining mentioned columns being essentially in the same plane. The three columns are interconnected at their superior ends via a superior yoke 60 while their inferior ends are interconnected by an inferior yoke 70. The magnetic core 20 consists advantageously of stacked sheets which are parallel with the plane where the three columns are located (30, 40 and 50). The material, amount and thickness of the sheets that form the different columns (30, 40 and 50) and yokes (60 and 70) may obviously be selected according to the normal criteria for the design of magnetic cores.


At least one main winding 80 is concentrically wound around the central column 30. In the electric reactor the controlled reactive power 10, the main winding 80 may be formed by various concentric layers of turns.


The magnetic core 20 consists of at least one generator of magnetic distortion field 90 that may be formed by a first pair of orifices 100 and a second pair of orifices 110 that pass through the thickness of the magnetic core 20, whether through a column or a yoke of the mentioned structure of a window type so that both pairs of orifices are generally adjacent. The term “orifice”, as used in the context of the present description means an opening, nozzle or orifice that may have any form and passes through an solid part of the magnetic core 20. In the first pair of orifices 100, a first control coil 120 is found wound up, and a second control coil 130 is wound in the second pair of orifices 110. In the three-phase case, it is necessary that each generator of magnetic distortion field 90 is located in a position relative to the magnetic core 20 so that it allows maintaining the magnetic equilibrium of the latter to assure reactive powers of consumption for each balanced phase.


A main current passes through the main winding 80, inducing a main magnetic flow in the magnetic core 20. In order to control the reactor's reactive power of consumption, the main magnetic flow is controlled when an alternate or continual control current passes simultaneously through each generator of the magnetic distortion field 90 to form fields of magnetic distortion of equal intensity in the magnetic core 20, so that each magnetic distortion field combines with the main magnetic flow originating a distortion in the latter while obtaining a resulting magnetic field.


In each generator of a magnetic distortion field 90, the control current is simultaneously provided to the first control coil 120 and to the second control coil 130 through some means to provide control current (not shown) that are electrically connected to these control coils. This control current is provided when a variation is detected in the required consumption of reactive power that varies in relation to the necessities of reactive power compensation of the system to which said reactor is connected. Thus, the reactive power of consumption makes itself corresponding to a current intensity that feeds each of the generators of magnetic distortion fields 90 to form the magnetic distortion fields in order to obtain the desired controlled reactive power of consumption.



FIG. 2 shows a lateral view of a magnetic core 20 of the column type, where magnetic core 20 has a central column 30 and two external columns 40 and 50, interconnected through an upper yoke 60 and an inferior yoke 70.


From the perspective of the magnetic core 20, there is at least one generator of magnetic distortion field 90 formed by a first pair of orifices 100 and a second pair of orifices 110 that pass through the thickness of the magnetic core 20, through a column or a yoke, or through a combination of both. In the first pair of orifices 100, a first control coil 120 is wound with one or more spirals, while in the second pair of orifices 110 a second control coil 130 is wound with one or more spirals.


A main magnetic flow 140 is induced in the magnetic core 20 by the main current circulating in the primary winding (not shown). When a variation in the reactive power occurs in the node where the reactor and/or a variation in the profile of the electric tension of said node occur, then the means to provide control current (not shown) provide simultaneously an alternate or continual control current to each of the generators of magnetic distortion fields 90, supplying simultaneously control current to the first control coil 120 and to the second control coil 130. Thus, the first control coil 120 generates a first magnetic control flow 150 in the magnetic core 20, while the second control coil 130 generates a second magnetic control flow 160 in the opposite direction of the first magnetic control flow 150. Both magnetic control flows 150 and 160 forming a magnetic distortion field 170 in the magnetic core 20 that combine with the main magnetic flow 140. The intensity of the control current supplied to the generators of magnetic distortion fields 90 correspond to the detection of the reactive power of consumption required in relation to the profile of the electric voltage node of the power system to which the reactor is connected. FIG. 3 shows a presentation of the magnetic distortion field 170 generated.


Each of the magnetic distortion fields 170, when combined with the main magnetic flow 140 act in an analogue or equivalent manner to the function of the physical air gap in the magnetic core 20, but with the difference that the size of the magnetic distortion field 170 varies according to the intensity of the control current supplied to the generator of the magnetic distortion field 90, specifically to the first control coil 120 and to the second control coil 130. Therefore, logically, it would be like having the function of an air gap of a variable size according to the operation requirements of the reactor of controlled reactive power 10.


It is important to mention that the generators of magnetic distortion fields 90 must be connected in series or parallel in order to generate the magnetic distortion fields 170 of the same intensity, and located in a position relative to the magnetic core 20 so that the magnetic equilibrium of the latter may be maintained to ensure balanced reactive powers of consumption.


The presence of a magnetic distortion field 170 in a magnetic circuit provokes changes in the reluctance of that field itself. At a bigger amount of and/or intensity of the magnetic distortion field 170, the change in reluctance increases. Therefore, in a controlled reactive power reactor 10, in the presence of a change in reluctance, the main current of the main winding will vary to maintain the main magnetic flow 140 constant. Based on the principle of magnetic stability of an electromagnetic system, and with a variation in the supplied currents to the control windings, a variation in the magnetic distortion is encountered. Therefore, there is a variation in the core reluctance. This originates a variation in the main current to maintain the main magnetic flow constant. Experienced variation of the main current is translated into a variation of the consumed reactive power, which in this case is the variable of the required control for a controlled reactive power reactor according to the present invention.


The above described is expressed mathematically in the following:

    • If a magnetic distortion field 170 is present in the magnetic circuit of a reactor, then a variation in its reluctance is present according to the following equations:







Δ





R

=


Δ





Fmm

φ








Δ





R

=


N


(


I

p





1


-

I

p





0



)


BA





Where:

    • ΔR is the variation of the reluctance.
    • ΔFmm is the variation of the magnetomotive force.
    • φ is the main magnetic flow.
    • N is the amount of turns of the primary winding.
    • Ip1 is the primary winding current after the reluctance variation.
    • Ip0 is the primary winding current before the reluctance variation.
    • B is la magnetic flow density.
    • A is the column area of the magnetic core.
    • Q reactive power consumed by the reactor.


As an example, because of the increase in reluctance, the primary winding current (IP) will increase to maintain the main magnetic flow (φ) constant (cte).

    • IPφ=cte


Such increment in the primary winding current (IP) is translated as an increment in the consumption of reactive power (Q); while a decrease in the primary winding current (IP) is reflected as a decrease in the reactive power consumption (Q) of the reactor.

    • IPQ IPQ


Turning now to FIG. 4, in conjunction with FIG. 2, a block diagram is shown of a method to adjust the reactive voltage of an electric reactor according to the present invention. The method starts in step 180 when a main current is supplied to a primary winding (not shown) to induce a main magnetic flow 140 in the magnetic core 20.


Next, in step 190, the required reactive power of consumption in relation to the requirements of reactive voltage compensation is detected, which demands the voltage system to which the controlled reactive electric voltage reactor 10 is connected, to proceed in step 200 and generate at least one magnetic distortion field 170 in the magnetic core 20 (where in case of a three-phase reactor the magnetic equilibrium is controlled to ensure the balanced reactive consumption voltages). Thus, each magnetic distortion field 170 combines with the main magnetic flow 140, generating a distortion in the latter. In this way the reactive consumption power of said reactor is accomplished, because as the current varies in the main winding, also the reactive voltage will vary, which is the desired control variable.


The magnetic distortion field 170 can be generated when supplying, in step 210, a control current, whether alternate or continual at an intensity that varies in relation to the detection of the reactive power of consumption required in relation to the profile of the electric node voltage of the power system to which the reactor is connected, to a first control coil 120 to generate a first magnetic control flow 150 over the magnetic core 20, where the first control coil 120 is wound in a first pair of orifices 100 in the magnetic core 20. Simultaneously, in step 220, said control current is supplied to a second control coil 130 to generate a second magnetic control flow 160 in the magnetic core 20, where the second control coil 130 is wound in a second pair of orifices 110 in the magnetic core 20 so that the second magnetic control flow 160 has an opposite direction to the first magnetic control flow 150, thus forming the magnetic distortion field 170 whose representation of magnetic field lines is shown in FIG. 3.


An alternative embodiment of this invention, and with the purpose of maintaining the required safety redundancy in the reactor, consists in combining the use of generators of magnetic distortion and the structure of a central column of air gaps. So, in case of failure of the magnetic distortion generators, the central column of air gaps accomplishes its committed safety redundancy. In this case, the electric reactor of controlled reactive power may be formed in a very similar way to the reactor described in FIG. 1, but with the difference that the central column is replaceable by a central column of air gaps that in turn consists of a number of ferro-magnetic doughnuts and air-gap spacers embedded between the ferro-magnetic doughnuts, and as a whole are stacked in the form of a central column. The central column of air gaps is maintained extremely rigid by the union of the ferro-magnetic doughnuts and the air-gap spacers via the use of epoxy glue and of a central bolt that passes completely through the column and maintains it to the upper and inferior yoke through the us of a bolt-nut mechanism, thus allowing to eliminate the vibrations during the operation of the reactor.


In addition to the above, the magnetic core consists of at least one field generator of magnetic distortion that may be formed by a first pair of orifices and a second pair of orifices that pass through the thickness of the magnetic core, whether through an external column or a yoke of the mentioned structure of a window type. In another embodiment of the invention, the magnetic distortion generator may be located in one or more ferro-magnetic doughnuts of the central column of air gaps.


As to the method to adjust the reactive power of an electric reactor described with the use of the safety redundancy according to the former paragraphs, it is similar to the method described in FIG. 4.



FIG. 5 shows different magnetizing curves of an electric reactor with at least one primary winding and a group of “n” generators of magnetic distortion field in its magnetic core, these curves are obtained starting from a value of fixed excitation current in the primary winding and with different values of current I1, I2 and I3 in the generators of the magnetic distortion field. In this way, it can be observed that as the value of the current in the generators of the magnetic distortion field increases, the density of the magnetic flow B reduces to a certain value of excitation in the primary winding. This is equivalent to having a magnetic core with reduced magnetic permeability or the presence of real air spaces in the magnetic core. In other words, it can be observed that, as if a reactor of a variable magnetic permeability were obtained, a parameter that is also controlled through the present invention. It is observed that the value of the initial magnetic permeability is the same in all cases. As the value of the current in the generators of the magnetic distortion field increases, the effect of the magnetic permeability increases.


Control over the magnetizing curves allows control of the saturation level, and as a consequence the harmonics in the current and electric voltage signals. This is, as the saturation level increases, the contents of the harmonics increases, and vice versa.


Although the invention has been described with reference to specific embodiments, this description in not meant to be constructed in a limited sense. The various modifications of the disclosed embodiments, as well as alternative embodiments of the invention, will become apparent to person skilled in the art upon reference to the description of the invention. It is, therefore, contemplated that the appended claims will cover such modifications that fall within the scope of the invention, or their equivalents.

Claims
  • 1. An electric reactor of controlled reactive power comprising: at least one magnetic core; andat least a primary winding having a main current supplied to generate a main magnetic flow in said at least one magnetic core; andat least one generator of a magnetic distortion field, said at least one generator having a control current supplied to generate a field of magnetic distortion on said at least one magnetic core, said control current having an intensity variable in relation to consumption of reactive power required according to compensation necessities of reactive power;wherein the magnetic distortion field combines with said main magnetic flow, generating a distortion of said main magnetic flow, achieving a change in reluctance of said at least one magnetic core and changing reactive power of consumption.
  • 2. The electric reactor of claim 1, wherein said at least one magnetic core is a column type having a central column.
  • 3. The electric reactor of claim 1, wherein said at least one generator is located in a relative position in the magnetic core, maintaining magnetic equilibrium of the magnetic core, ensuring a balanced consumption of reactive power, in a three-phase reactor.
  • 4. The electric reactor of claim 1, wherein said at least one generator of the magnetic distortion field comprises: a first pair of orifices in said magnetic core;a second pair of orifices in said magnetic core;a first control coil wound in said first pair of orifices, having a control current supplied to generate a first magnetic control flow in said magnetic core; anda second control coil wound in said second pair of orifices, having a control current supplied simultaneously to generate a second magnetic control flow in said magnetic core, wherein said second magnetic control flow has an opposite direction to said first magnetic control flow; andwherein the first and second magnetic control flows form said magnetic distortion field.
  • 5. The electric reactor of claim 4, wherein said first pair of orifices and said second pair of orifices are adjacent.
  • 6. The electric reactor of claim 4, wherein said first control coil has at least one spiral.
  • 7. The electric reactor of claim 4, wherein said second control coil has at least one spiral.
  • 8. The electric reactor of claim 1, wherein said main current is alternate current.
  • 9. The electric reactor of claim 1, wherein said control current is alternate current or continual current.
  • 10. The electric reactor of claim 1, wherein said at least one generator controls magnetic permeability of said magnetic core.
  • 11. A method for adjusting reactive power of an electric reactor, the reactor having at least a magnetic core, at least a primary winding, and at least a generator of a magnetic distortion field, the method comprising the steps of: supplying a main current to said primary winding to generate a main magnetic flow in said magnetic core;detecting consumption of required reactive power, being variable in relation to compensation necessities of reactive power; andgenerating at least a magnetic distortion field in said magnetic core, under detection of reactive power consumption, said field of magnetic distortion combining with said main magnetic flow, generating a distortion of the latter, achieving a change in the reluctance of said magnetic core, and a change in reactive power of consumption of said reactor.
  • 12. The method of claim 11, wherein said magnetic core is a column type having a central column.
  • 13. The method of claim 11, wherein said generator is located in a relative position in the magnetic core, maintaining magnetic equilibrium of the magnetic core, ensuring a balanced consumption of reactive power, in a three-phase reactor.
  • 14. The method of claim 11, wherein said step of generating at least a magnetic distortion field in said magnetic core, under the detection of reactive power consumption, comprises the steps of: supplying a control current to a first control coil wound in a first pair of orifices in said magnetic core, generating a first magnetic control flow in said magnetic core; andsupplying a simultaneous control current to a second control coil wound in a second pair of orifices in said magnetic core, generating a second magnetic control flow in said magnetic core where said second magnetic control flow has an opposite direction to said first magnetic control flow;wherein said control current supplied to the first and second control coils has an intensity variable in relation to detection of the required reactive power consumption, the power consumption being variable in relation to compensation necessities of reactive power, said first and second magnetic control flows forming said magnetic distortion field.
  • 15. The method of claim 14, wherein said first pair of orifices and said second pair of orifices are adjacent.
  • 16. The method of claim 14, wherein said first control coil has at least one spiral.
  • 17. The method of claim 14, wherein said second control coil has at least one spiral.
  • 18. The method of claim 14, wherein said control current is alternate current or continual current.
  • 19. The method of claim 11, further comprising the step of: controlling magnetic permeability of said magnetic core.
Priority Claims (1)
Number Date Country Kind
NL/A/2006/000065 Sep 2006 MX national