APEC Active and Passive Electronic Components 1563-5031 0882-7516 Hindawi Publishing Corporation 10.1155/2014/951624 951624 Research Article Analysis of the Coupling Coefficient in Inductive Energy Transfer Systems http://orcid.org/0000-0002-5635-1390 Mendes Duarte Rafael Klaric Felic Gordana Ghibaudo Gerard The University of Melbourne Parkville, VIC 3010 Australia unimelb.edu.au 2014 1762014 2014 08 01 2014 04 06 2014 17 6 2014 2014 Copyright © 2014 Rafael Mendes Duarte and Gordana Klaric Felic. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

In wireless energy transfer systems, the energy is transferred from a power source to an electrical load without the need of physical connections. In this scope, inductive links have been widely studied as a way of implementing these systems. Although high efficiency can be achieved when the system is operating in a static state, it can drastically decrease if changes in the relative position and in the coupling coefficient between the coils occur. In this paper, we analyze the coupling coefficient as a function of the distance between two planar and coaxial coils in wireless energy transfer systems. A simple equation is derived from Neumann’s equation for mutual inductance, which is then used to calculate the coupling coefficient. The coupling coefficient is computed using CST Microwave Studio and compared to calculation and experimental results for two coils with an excitation signal of up to 10 MHz. The results showed that the equation presents good accuracy for geometric parameters that do not lead the solution of the elliptic integral of the first kind to infinity.

1. Introduction

Wireless power systems transfer the energy without wire connection between a source and a load. This provides several advantages specially for applications involving implantable devices [1, 2] or devices that need to be hermetically sealed during operation . For the first, the use of batteries presents issues in terms of periodic replacement which may require complex surgical procedures. For the latter, a connection through wires becomes unfeasible. Among the many classes of wireless systems, energy transfer via inductive link has been widely studied due to high efficiency and high transmission power capability .

In inductive coupled systems, a power amplifier supplies an alternative current to the primary coil, which produces a magnetic field at the secondary coil. The produced field induces a current and voltage at the secondary branch, which can be rectified and supplied to a load. An important parameter for inductive links is the coupling coefficient k, which measures how much power from the generated electromagnetic (EM) field is induced in the secondary coil. The coupling coefficient is related to the reflected impedance from the secondary on the primary side. Therefore, variations on k change the output impedance of the power amplifier, removing it from its optimum operation condition and decreasing its efficiency .

Previous studies on the magnetic coupling suggest that the coupling coefficient can be affected mostly due to variations in the distance between the coils , relative angle between the coils, and magnetic properties of the material surrounding the coils. This is particularly important for systems where the two coils are not in a fixed relative position. For such systems, the efficiency can be seriously compromised due to inefficient operation of the power amplifier. Hence, analyzing the behavior of the coupling factor as a function of these critical parameters can help to maintain the system efficiency stable as the coupling between the coils varies.

Numerical simulations provide highly accurate results but require long computational time and extensive memory usage. Although the analytical methods based on the closed form expressions lack high accuracy, they offer fast solutions and explicit control over the design parameters.

In this paper, we derive a simple formula for the mutual inductance as a function of the distance between two planar and coaxial coils. The equation is obtained from Neumann’s equation for the mutual inductance, using power series as approximated solutions of the elliptic integrals, which are usually computationally expensive to obtain. We also give theoretical insight about the correlation between magnetic field distribution and coupling coefficient. The presented equation is compared to simulation and experimental results of two designed coils with excitation signals at frequencies of up to 10 MHz.

In Figure 1, a simple diagram of an inductive link is shown. A primary coil is excited by a power amplifier (PA), usually operating in class E due to its high efficiency. Power is transmitted to the load via magnetic coupling between inductors L1 and L2. The system efficiency is defined as the ratio between the power dissipated on the load and the power supplied to the power amplifier. In addition to losses in the inductors, due to finite resistance of the coils, the PA efficiency plays a major role in degrading overall efficiency.

In order to design the PA, the impedance seen at its output (Zin in Figure 1) must be taken into account. In most designs, the inductance of the primary coil is used as a component for the output filter of the power amplifier while the output resistance is considered the load of the amplifier. The values of these output components are tightly related to the amplifier efficiency, once optimum operation state is achieved for determined component values . Therefore, variations on the output impedance can significantly decrease the amplifier efficiency and, as a consequence, the system efficiency.

For a generic load ZL connected to the secondary coil, the impedance Zin can be defined as (1)Zin=R1S+jwL1+w2M2jwL2R2S+ZL, where R1S represents the series resistance of L1 and M is mutual inductance, related to the coupling coefficient k according to (2)k=ML1L2, where L1 and L2 are the self-inductance of coils 1 and 2.

Equations (1) and (2) express the dependence of the output impedance on the coupling coefficient of the inductive link. As the mutual inductance varies, the third term of (1), which can have an imaginary and real part, varies and modifies the impedance Zin shown in Figure 1.

3. Coupling Coefficient Calculation

The mutual inductance between two circular loops separated by a distance d and with radii a and b, as depicted in Figure 2, can be calculated using Neumann’s equation : (3)M=μ4πcosϵrdsds, where ds and ds are the incremental sections of the circular filaments and r is the distance between these two sections, which are defined as (4)r=a2+b2+d2-2acos(ϕ-ϕ),ϵ=ϕ-ϕ,ds=adϕ,ds=bdϕ. The substitution of (4) in (3) results in (5)M=μ4π02πabcos(ϕ-ϕ)a2+b2+d2-2acos(ϕ-ϕ)dϕdϕ. The integral in (5) can be rewritten using elliptic integrals, yielding (6)M(m)=2μabm[(1-m22)K(m)-E(m)], where K(m) and E(m) are the elliptic integrals of first and second kind, respectively, and m is defined as (7)m=4ab(a+b)2+d2 assuming values between 0 and 1.

Two coaxial coils with radii a and b.

3.1. Solution of the Elliptic Integrals

The solutions of the elliptic integrals of the first and second kind can be approximated  using (8) and (9). The approximation and the solution obtained through numeric integration are depicted in Figures 3 and 4. For low values of m, the power series representation shows reasonable accuracy. However, m increases both curves diverge from the numeric integration values. For the elliptic integral of the first kind, as m approaches the unity, the solution asymptotically tends to infinity much faster than the solution calculated by numeric integration: (8)K(m)=π2+π8m21-m2,(9)E(m)=π2-π8m2.

Comparison between numerical integration and power series approximation for elliptic integral of the first kind.

Comparison between numerical integration and power series approximation for elliptic integral of the second kind.

The second term of (8) tends to infinity as m tends to 1: (10)m=4ab(a+b)2+d2=1 which leads to the following relation between the coils radius and the distance between the coils: (11)d2=(a-b)2.

Hence, (8) is not valid when the distance between the two coils approaches the value expressed by (11). In order to avoid this limitation, a high number of terms would be required for the series approximation (8), making the final expression of the mutual inductance too complex and extensive. Alternatively, the solution of the elliptic integral of the first kind can be approximated by a logarithm function . However, the logarithm approximation leads to issues related to the signal of (6) and to an extensive resultant expression for the mutual inductance. Therefore, in this paper, we only use approximations (8) and (9), analyzing its limitations.

3.2. Mutual Inductance Calculation

The substitution of (8) and (9) in (6) yields (12)M(m)=μπab8m31-m2. Next, substituting (7) in the expression above results in the expression for the mutual inductance as a function of the distance between two circular coaxial loops: (13)M=μπa2b2(a+b)2+d2[(a-b)2+d2].

For two coils with n1,2 turns, the expression can be adjusted , yielding (14)M=μπn1n2a2b2(a+b)2+d2[(a-b)2+d2] which express the mutual inductance of two coils with n1,2 as a function of distance d, the magnetic permeability of the material surrounding the coils μ and the inner radius of the two coils.

4. Coupling Coefficient Measurement Technique

In this section, we discuss the methodology used to infer the coupling coefficient in simulations. The circuit schematic of the inductive link is shown in Figure 5 and its equations can be written as (15)V1=jw(I1L1+MI2),(16)V1=jw(I2L2+MI1).

Circuit schematic of the inductive link.

Assuming the secondary coil is shorted, (16) becomes (17)I2=-MI1L2.

Substituting (17) in (15) yields (18)V1=jwI1(L1-ML2). Assuming (19)Ls=L1-ML2, equation (18) becomes (20)V1=jwI1Ls. Hence, the inductance Ls is the inductance measured when the secondary coil is shorted. Rearrange (19) in terms of the mutual inductance: (21)M=L2(L1-Ls).

Finally, combining (21) and (2) results in the expression of the coupling coefficient in terms of the self-inductance L1 and the inductance measured when the secondary coil is shorted, Ls: (22)k=1-LsL1.

5. Results

Simulation results were used to check the accuracy of (14). In addition, experimental results were analyzed for two coils with geometries that lead the coefficient m close to unity for short separation distances between the coils.

5.1. Mesh Properties

To evaluate the coil impedance, it is necessary to take into account the geometry and curvature of the coils, as well as the interaction between the traces of each turn. Thus, circular coils are computational expensive since a very fine mesh is required to precisely create the EM model for the circular shapes of the coils. In order to achieve reasonable accuracy and reliable results, the mesh cell size was decreased to a point where no further variation in the results was observed. In addition, the accuracy of curvature elements in CST was also increased until stable results were achieved.

5.2. Simulation

In order to analyze the accuracy of (14), the coupling coefficient between two coils, with dimensions given by Table 1, was computed using CST. Parameters s and w are the spacing between traces and trace width, respectively; h is the trace height and n is the number of turns. The coupling coefficient was measured according to the method explained in Section 4, for an excitation signal at 1, 6, and 10 MHz. The results are shown in Figure 6.

Dimensions of simulated coils (in mm).

a h w s n
Coil 1 11.5 0.035 0.5 0.5 7
Coil 2 11.5 0.035 0.5 0.5 4

Coupling coefficient as a function of distance for different frequencies.

Equation (14) presented a reasonable accuracy compared to simulation results, specially for large separation distance between the coils (d>20 mm). Also, as (14) predicts, the coupling coefficient is not dependent on the operation frequency, presenting small variations at different frequencies. These small variations can be explained by proximity and skin effects, which are responsible for slightly changing the impedance of the primary and secondary coils. The skin effect increases proportionally to the square root of the operation frequency, increasing the impedance of the coil.

5.3. EM Field Distribution

Figure 7 shows the magnetic field distribution surrounding the coils at 6 MHz. The field lines are normal to the XY plane. The coupling coefficient is dependent on how much of the magnetic field flux is encircled by the secondary coil, being higher if a high density of lines is projected through the secondary coil. The amount of magnetic field lines diverging from the secondary coil can be seen as a field leakage, reducing the coupling between the two coils.

Magnetic field distribution surrounding the coils, in YZ plane.

As the two coils are separated apart in the Z direction, more field leakage is observed as the concentration of field lines reaching the secondary coil becomes lower.

5.4. Measurements

The limitation of (14) was also tested through experiments. We measured the coupling coefficient of two identical coils with dimensions given in Table 2. The setup for the measurement is shown in Figure 8. The primary coil was connected to a port of a vector network analyzer and the S parameters were measured. The Z matrix was calculated, yielding the input impedance and, therefore, the inductance seen at the primary coil when the secondary coil is shorted (Ls in (22)).

Dimensions of coils used for measurements (in mm).

a h w s n
23.5 0.035 0.5 0.5 18

Setup for measurement of coupling coefficient.

The measured and calculated results are depicted in Figure 9. The measurements were performed at an operation frequency of 1 MHz. For distances above 10 mm, the calculated results are reasonable close to the experimental ones. Since the radii of both coils are the same, (11) can be written as (23)d2=0 which means that for distances close to 0, (14) is no longer valid and good accuracy is no longer obtained, as shown in Figure 9 for small distances (d<10 mm).

Measured coupling coefficient at 1 MHz.

As previously mentioned, as the distance becomes closer to the condition given by (23), the second term of the approximation of the elliptic integral of the first kind (8) asymptotically tends to infinity, resulting in high values of the coupling coefficient.

6. Conclusions

In this paper, the coupling coefficient between two coplanar and coaxial coils was analyzed as a function of the separation distance. We derived an equation for the mutual inductance from Neumann’s equation which can be used to estimate the coupling coefficient between the coils. In order to derive the equation, we used a power series approximation for the solution of the elliptic integrals, which is usually calculated by numerical integration. The derived equation presented good accuracy when compared to simulation results. The experimental results demonstrated the limitation of the presented equation, as it can only be used for coil geometries and properties that do not lead the solution of the elliptic integral of the first kind to infinity.

The analysis presented here is useful for inductive link systems where the distance between the coils is not constant. By predicting the behavior of the coupling coefficient as a function of the variable distance, it is possible to devise a simple mechanism capable of locking the system efficiency at a desired level despite variations in the relative position of the source and load.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

The authors would like to thank the Brazilian National Council for Scientific and Technological Development (CNPq) for funding the studies of the first author in Australia. Also, they would like to thank NICTA, Australia’s Information and Communications Technology (ICT) Research Centre of Excellence.

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