Coil unit for inductively charging a vehicle

Abstract

A coil unit for inductively charging a vehicle is provided. The coil unit includes a coil, wherein the coil includes multiple windings of at least two electric lines. The electric lines are connected in parallel. Each of the electric lines has a respective winding part, in which the windings are formed, and an additional part, in which an additional inductor unit having a predefined electric inductance is arranged.

Description

BACKGROUND AND SUMMARY OF THE INVENTION

The invention relates to a coil unit for inductively charging a vehicle.

Many modern vehicles are hybrid vehicles or electric vehicles. Precisely such vehicles often have electrical energy stores with a high charging capacity. To simplify a charging procedure of the electrical energy stores, it is advantageous if the electrical energy stores are able to be charged wirelessly

An object on which the invention is based is to provide a coil unit for inductively charging a vehicle, which coil unit is very efficient.

This and other objects are achieved by a coil unit in accordance with embodiments of the invention.

The invention is distinguished by a coil unit for inductively charging a vehicle. The coil unit includes a coil, wherein the coil includes a plurality of windings of at least two electrical lines. The electrical lines are connected in parallel. Each of the electrical lines has a respective winding part in which the windings are formed and an additional part in which an additional inductance unit is arranged that has a prescribed electrical inductance.

The coil unit is arranged for example in or on the vehicle and the coil is what is known as a secondary coil. As an alternative, the coil unit is arranged for example outside the vehicle and the coil is what is known as a primary coil.

Due to the number of at least two electrical lines, a high current-carrying capacity is able to be achieved since the current is distributed over the parallel electrical lines. The additional inductance unit may contribute to the current being distributed evenly over the parallel electrical lines. The number of electrical lines is in principle able to be selected freely, and as many electrical lines as desired may therefore be used in order to achieve a high current-carrying capacity.

The electrical lines are in particular HF litz wires. An HF litz wire, also called high-frequency litz wire, is a litz wire that includes a relatively high number of wires that are insulated from one another. The wires are in particular intertwined such that on average each individual wire as far as possible adopts each position in the overall cross section of the litz wire with the same frequency. As a result, the litz wire has a very high number of conductive surfaces, such that high efficiency is able to be achieved in spite of the skin effect.

According to a refinement, the additional inductance unit has an electrical inductance that corresponds to at least 0.02 times the electrical inductance of the respective electrical line in the winding part.

The smaller the electrical inductance of the additional inductance unit, the lower its effect on system parameters of the coil unit. However, a larger additional inductance unit may possibly contribute more accurately to the current being distributed evenly over the parallel electrical lines. Therefore, a size of at least 0.02 times the electrical inductance of the respective electrical line in the winding part is a good compromise. The respective additional inductance unit has for example an electrical inductance that is in a region of 0.02 times to 0.1 times the electrical inductance of the respective electrical line in the winding part. By way of example, the electrical inductance of the additional inductance unit corresponds to 0.02 times, 0.04 times, 0.06 times, 0.08 times or 0.1 times the electrical inductance of the respective electrical line in the winding part.

According to a further refinement, the number of electrical lines is two and the additional inductance units of the two electrical lines are oppositely coupled.

By virtue of the opposite coupling of the additional inductance units of the two electrical lines, the overall impedance of the coil is not changed by the additional inductance units. The opposite coupling may be achieved for example by forming the two additional inductance units by way of two coils that have a common ferrite and that are oppositely wound.

According to a further refinement, the additional inductance unit is formed as a separate component.

As a result, the manufacture of the coil unit is simplified since the additional inductance unit is able to be added in a separate manufacturing step.

According to a further refinement, the additional inductance unit is formed by winding the respective electrical line so as to form an additional coil.

As a result, the additional inductance unit is able to be formed in a very simple and inexpensive manner.

According to a further refinement, the additional coils of the electrical lines are wound around a common ferrite.

As a result, coupling of the additional coils is able to be achieved in a very simple manner.

According to a further optional refinement, the coil unit additionally has a carrier body that has a number of ferrites that corresponds to the number of electrical lines. A magnetically neutral carrier is in each case arranged between the ferrites. The additional coils of the electrical lines are each wound around the ferrites of the carrier body.

As a result, decoupling of the additional coils is able to be achieved in a very simple manner.

According to a further refinement, the number of electrical lines is two. The electrical inductances of the additional inductance units are prescribed such that it holds true that L_S1+L1=L_S2+L2. L1 is the inductance of a first of the two additional inductance units. L2 is the inductance of a second of the two additional inductance units. L_S1 is the inductance in the winding part of the electrical line that has the first additional inductance unit. L_S2 is the inductance in the winding part of the electrical line that has the second additional inductance unit.

The two electrical lines often have different lengths in the winding part and therefore different diameters in the winding part, in particular in the case of a planar winding. Since, in the case of a planar winding, one of the two electrical lines always runs on the outer side, this has a greater inductance and, due to the longer path, a greater resistance. If the electrical inductances of the additional inductance units are prescribed such that it holds true that L_S1+L1=L_S2+L2, such asymmetry is able to be compensated.

Other objects, advantages and novel features of the present invention will become apparent from the following detailed description of one or more preferred embodiments when considered in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a view of a structure of an inductive charging system.

FIG. 2 is a plan view of a ground unit.

FIG. 3 is a view of one refinement of a primary coil or secondary coil.

FIG. 4 is a view of a coil model.

FIG. 5 is a view of a substitute model.

FIG. 6 is a graph of an imaginary part of currents plotted against a coupling factor.

FIG. 7 is a graph of magnitudes of an absolute part of currents plotted against a coupling factor.

FIG. 8 is a view of a coil unit for inductively charging a vehicle.

FIG. 9 is a view of a substitute model of the coil unit for inductively charging a vehicle.

FIG. 10 is a view of the coil unit for inductively charging a vehicle in which two electrical lines are oppositely coupled.

FIG. 11 is a view of a substitute model of the coil unit for inductively charging a vehicle in which two electrical lines are oppositely coupled.

FIG. 12 is a view of a winding part of the coil unit.

FIG. 13 is a view of a substitute model of the coil unit for inductively charging a vehicle.

FIG. 14 is a view of a substitute model of the coil unit for inductively charging a vehicle.

FIG. 15 is a view of the coil unit for inductively charging a vehicle.

FIG. 16 is a view of the coil unit, wherein additional coils are wound around a common ferrite.

FIG. 17 is a view of the coil unit, wherein additional coils are wound around a carrier body.

DETAILED DESCRIPTION OF THE DRAWINGS

Elements having the same structure or function are referenced using the same reference signs throughout the figures.

FIG. 1 shows a structure of an inductive charging system. The charging system includes a ground unit 100 and a vehicle unit 200 that is connected to a vehicle battery.

The ground unit 100 includes a housing 101, a primary coil 103 and a ferrite 105.

The vehicle unit 200 likewise includes a housing 201, a secondary coil 203 and a ferrite 205.

In a charging procedure, the vehicle unit 200 is arranged at a distance d above the ground unit 100.

FIG. 2 shows a plan view of the ground unit 100. As may be seen, the primary coil 103 is situated on the ferrite 105.

FIG. 3 shows one refinement of the primary coil 103 or secondary coil 203. The refinement of the primary coil 103 or secondary coil 203 includes a plurality of windings of two electrical lines, the electrical lines being connected in parallel. The windings are in particular configured such that the two electrical lines lie as close as possible to one another and possibly even cross so as to create conditions that are as equal as possible for the electrical lines

If a model, as shown in FIG. 4, which includes a resistance R and inductance L, is taken for one of the electrical lines, then the substitute model shown in FIG. 5 results for the refinement of FIG. 3. The two windings may be interpreted as a transformer. Due to the winding type, an approximately equal inductance and a coupling factor very close to 1 results for both windings. The two electrical lines are connected to a terminal.

The following equations result from the substitute model, under the assumption that k≅1, ΔL_1/2≅0, R_1/2≅0, M=k√{square root over (L₁L₂)}=kL=L, k is in this case the coupling factor, L₁ is the inductance of the winding of a first of the two electrical lines, L₂ is the inductance of the winding of a second of the two electrical lines, R₁ is the line resistance of the first electrical line and R₂ is the line resistance of the second electrical line:

$\begin{array}{cc}\left[\begin{array}{c}{U}_1\\ U_1\end{array}\right]=Z\left[\begin{array}{c}{I}_1\\ I_2\end{array}\right]& \left(1\right)\\ Z=\left[\begin{array}{cc}{L}_1+R_1& M\\ M& L_2+R_2\end{array}\right]& \left(2\right)\\ Z=\left[\begin{array}{cc}L+\Delta L_1+R_1& M\\ M& L+\Delta L_2+R_2\end{array}\right]\cong \left[\begin{array}{cc}L& L\\ L& L\end{array}\right]& \left(3\right)\end{array}$

For the sake of simplicity, “L” is written in place of “jwL”.

This gives the following:

$\begin{array}{cc}\left[\begin{array}{cc}L& L\\ L& L\end{array}\right]\left[\begin{array}{c}{I}_1\\ I_2\end{array}\right]=\left[\begin{array}{c}{U}_1\\ U_2\end{array}\right]& \left(4\right)\end{array}$ wherein U₁=U₂=U and I₁+I₂=I.

As may be seen, there are infinite solutions for the equation system (4). In practice, this means that the current may be divided in any way between the two windings. This is illustrated in more detail with reference to FIGS. 6 and 7.

FIG. 6 shows the imaginary part of the currents I₁, I₂ depending on the coupling factor k, under the assumption that ΔL₁=1 uH, L1=101 uH, L₂=100 uH, U1=U2=100 V, R1=R2=0 ohm.

If the coupling factor k approaches 1, then the currents run in opposite directions and the individual coil currents exceed the overall current.

FIG. 7 shows the absolute part of the currents I₁, I₂ depending on the coupling factor k, under the assumption that ΔR₁=0.5 ohm, L1=L2=100 uH, L2=100 uH, U1=U2=100 V, R1=0.5 ohm, R2=0 ohm.

If the coupling factor k approaches 1, then the current flows only through one conductor.

This shows that parallel coil windings react in a manner highly sensitive to the deviation of individual parameters. The unequal flow of current rises to a very great extent at a coupling factor close to 1, for example at k>˜0.99. Even in the case of small differences in resistance, the flow of current may be concentrated on one conductor. Different inductances may have even more extreme effects. In this case, the current in one of the electrical conductors 5,7 may even reverse, such that a multiple of the necessary current flows in another of the electrical conductors 5,7. Since in practice the individual electrical conductors 5,7 always exhibit differences, an electrical conductor is for example closer to a ferrite, a parallel connection is only efficient with a great deal of expenditure, since the exact layout of the windings is planned extremely accurately.

FIG. 8 shows a coil unit 1 for inductively charging a vehicle. The coil unit 1 includes a coil 3. The coil 3 may for example be the primary coil 103 of the ground unit 100. In this case, the coil unit 1 is for example the ground unit 100. As an alternative, the coil 3 may be for example the secondary coil 203 of the vehicle unit 200. In this case, the coil unit 1 is for example the vehicle unit 200.

The coil 3 includes a plurality of windings of at least two electrical lines 5,7. Each of the electrical lines 5,7 has a respective winding part 10 in which the windings are formed and an additional part 15 in which an additional inductance unit L_S is arranged that has a prescribed electrical inductance.

The electrical lines 5,7 are connected in parallel. To this end, the two electrical lines 5,7 are for example connected to a terminal.

If the number of electrical lines 5,7 is two, this gives the substitute model of FIG. 9. The following equation results from the substitute model:

$\begin{array}{cc}Z=\left[\begin{array}{cc}{L}_1+L_S+R_1& M\\ M& L_2+L_S+R_2\end{array}\right]& \left(5\right)\end{array}$

Under the assumption that L=L₁=L₂=M(k=1) and R=R₁=R₂, this gives:

$\begin{array}{cc}Z=\left[\begin{array}{cc}L+L_S+R_1& L\\ L& L+L_S+R_2\end{array}\right]& \left(6\right)\end{array}$ and with L_A=(L₁+L_S), L=L₁=L₂ M_A=k_A√{square root over ((L₁−L_S)(L₂+L_S))}=k_A(L+L_S)=L  (7)

This results in the following coupling:

$\begin{array}{cc}{k}_A=\frac{L}{L+L_S}& \left(8\right)\end{array}$

The coupling is thus reduced depending on the size of L_S. When L_s≥0.02 L, a critical range (cf. FIGS. 6 and 7) is avoided since the coupling k_A is then always less than 0.99.

The overall impedance of the coil changes due to the additional inductances. The overall impedance is given by solving the above equation systems with a Z-matrix. For L=L₁=L₂=M(k=1), R=R₁=R₂, the following results:Z_res=L+R/2+L_S/2  (9)

As may be seen, the overall resistance R is reduced by the parallel connection. At the same time, the overall inductance L+L_S/2 increases, but only by the value L_S/2. The reactive power in the system thus rises slightly.

FIG. 10 shows the coil unit 1, in which the number of electrical lines 5,7 is two and the additional inductance units L_S of the two electrical lines 5,7 are oppositely coupled. The opposite coupling may be achieved for example by forming the two additional inductance units L_S by way of two coils that have a common ferrite and that are oppositely wound.

This gives the substitute model of FIG. 11. The substitute model gives the following equation:

$\begin{array}{cc}Z=\left[\begin{array}{cc}{L}_1+L_S+R_1& M-L_S\\ M-L_S& L_2+L_S+R_2\end{array}\right]& \left(10\right)\end{array}$

Under the assumption that L=L₁=L₂=M(k=1), k_S=1 and R=R₁=R₂, this gives:

$\begin{array}{cc}Z=\left[\begin{array}{cc}L+L_S+R_1& L-L_S\\ L-L_S& L+L_S+R_2\end{array}\right]& \left(11\right)\end{array}$ and with L_A=(L+L_S) and M_A=(L−L_S):M=k_A√{square root over ((L+L_S)(L+L_S))}=k_A(L_S)=(L−L_S)  (12)and therefore

$\begin{array}{cc}{k}_A=\frac{L-L_S}{L+L_S}& \left(13\right)\end{array}$

As may be seen from formula 13, in comparison with formula 8, the coupling of the two electrical conductors 5,7 is reduced to a greater extent by L_S. Smaller additional inductance units L_S are therefore necessary to achieve the same effect.

Furthermore, the overall impedance is given for L=L₁=L₂=M(k=1), R=R₁=R₂ by solving the equation system with a Z-matrix:Z=L+R/2  (14)

As may be seen, the overall resistance R is reduced by the parallel circuit. At the same time, the overall inductance L does not increase. The reactive power in the system thus does not rise.

FIG. 12 shows one example of a parallel-wound winding part 10 with two electrical conductors 5,7. Due to the planar winding, the two electrical conductors 5,7 have different diameters. As one of the electrical conductors 7 always runs on the outer side, this has a greater inductance and, due to the longer path, a greater resistance.

Differently sized inductance units may compensate these differences between L₁ and L₂, as visible from the substitute model of FIG. 13:L_S1+L₁=L_S2+L₂  (14)

In the same way, an additional resistor may adjust the value of R₂ to R₁.

As an alternative or in addition, use may be made of a common-mode choke, that is to say oppositely coupled additional inductance units L_S as in FIGS. 10 and 11.

This gives the following Z-matrix, as may be seen from the substitute model of FIG. 14:

$\begin{array}{cc}Z=\left[\begin{array}{cc}{L}_1+L_{S1}+R_1& M-M_S\\ M-M_S& L_2+L_{S2}+R_2\end{array}\right]& \left(15\right)\end{array}$

In this case, the above-described differences may be compensated by way of the following equation:L₁+L_S1+R₁=L₂+L_S2+R₂  (16)

In principle, any desired number of electrical conductors 5,7 may be used. The number 4 is illustrated by way of example in FIGS. 15, 16 and 17. The additive overall inductance of L_S/n decreases with the number of individual lines. For a large n, the additive inductance is negligible.

FIGS. 16 and 17 show a system including a carrier body 20 and a ferrite 30. The carrier body 30 includes a number of ferrites 21, 22, 23, 24 that corresponds to the number of electrical lines 5, 6, 7, 8. Magnetically neutral carriers 25, 26, 27, 28, which may also be referred to as armatures, prevent the ferrites 21, 22, 23, 24 from magnetically coupling.

In FIG. 16, the additional coils of the electrical lines 5, 6, 7, 8 are wound around the common ferrite 30.

In FIG. 17, the additional coils of the electrical lines 5, 6, 7, 8 are respectively wound around the ferrites 21, 22, 23, 24 of the carrier body 20.

The air gaps may then be closed, as indicated by the arrows in FIG. 16.

The common ferrite 30 may be connected to a ferrite of the coil, that is to say for example to the ferrite 105 of the primary coil 103 or the ferrite 205 of the secondary coil 203, or it may be part of this ferrite 105, 205.

In summary, due to the number of at least two electrical lines 5, 6, 7, 8, a high current-carrying capacity is achieved since the current is distributed over the parallel electrical lines 5, 6, 7, 8. The additional inductance unit LS may contribute to the current being distributed evenly over the parallel electrical lines 5, 6, 7, 8. The number of electrical lines 5, 6, 7, 8 is in principle able to be selected freely, and as many electrical lines 5, 6, 7, 8 as desired may therefore be used in order to achieve a high current-carrying capacity.

LIST OF REFERENCE SIGNS

• • 1 coil unit
  • 3 coil
  • 5,6,7,8 electrical lines
  • 10 winding part
  • 15 additional part
  • 20 body
  • 21, 22, 23, 24 ferrites
  • 25, 26, 27, 28 magnetically neutral carriers
  • 30 ferrite
  • 100 ground unit
  • 101 housing
  • 103 primary coil
  • 105 ferrite
  • 200 vehicle unit
  • 201 housing
  • 203 secondary coil
  • 205 ferrite
  • L_S additional inductance unit

The foregoing disclosure has been set forth merely to illustrate the invention and is not intended to be limiting. Since modifications of the disclosed embodiments incorporating the spirit and substance of the invention may occur to persons skilled in the art, the invention should be construed to include everything within the scope of the appended claims and equivalents thereof.

Claims

1. A coil unit for inductively charging a vehicle, comprising: a coil, wherein the coil comprises a plurality of windings of at least two electrical lines, whereinthe at least two electrical lines are connected in parallel,each of the at least two electrical lines has a respective winding part and an additional part in which an additional inductance unit is arranged that has a prescribed electrical inductance that is 0.02 times, 0.04 times, 0.06 times, or 0.08 times an electrical inductance of each of the at least two electrical lines in the respective winding part,the at least two electrical lines are litz wires, andthe additional inductance units of the at least two electrical lines have a common ferrite, but are oppositely wound.

2. The coil unit according to claim 1, wherein a number of electrical lines is two and the additional inductance units of the at least two electrical lines are oppositely coupled.

3. The coil unit according to claim 1, wherein the additional inductance unit is formed as a separate component.

4. The coil unit according to claim 1, wherein the additional inductance unit is formed by winding the respective electrical line so as to form an additional coil.

5. The coil unit according to claim 4, wherein the additional coils of the at least two electrical lines are wound around a common ferrite.

6. The coil unit according to claim 4, further comprising: a carrier body that has a number of ferrites that corresponds to a number of electrical lines, wherein a magnetically neutral carrier is in each case arranged between the number of ferrites and the additional coils of the electrical lines and each of the additional coils of the number of electrical lines wound around the respective ferrite.

7. The coil unit according to claim 1, wherein a number of electrical lines is two and electrical inductances of the two additional inductance units are prescribed such that it holds true that L_S1+L1=L_S2+L2, wherein L1 is an inductance of a first of the two additional inductance units, L2 is an inductance of a second of the two additional inductance units, L_S1 is an inductance in the winding part of an electrical line that has the first of the two additional inductance units and L_S2 is an inductance in the winding part of an electrical line that has the second of the two additional inductance units.