# Modeling Resonant Coupled Wireless Power Transfer System

This example shows how to create and analyze a resonant coupling type wireless power transfer(WPT) system with emphasis on concepts such as resonant mode, coupling effect, and magnetic field pattern. The analysis is based on a 2-element system of spiral resonators.

This example requires the following product:

- Partial Differential Equation Toolbox™

## Contents

## Design Frequency and System Parameters

Choose the design frequency to be 30MHz. This is a popular frequency for compact WPT system design. Also specify the frequency for broadband analysis, and the points in space to plot near fields.

fc=30e6; fcmin = 28e6; fcmax = 31e6; fband1 = 27e6:1e6:fcmin; fband2 = fcmin:0.25e6:fcmax; fband3 = fcmax:1e6:32e6; freq = unique([fband1 fband2 fband3]); pt=linspace(-0.3,0.3,61); [X,Y,Z]=meshgrid(pt,0,pt); field_p=[X(:)';Y(:)';Z(:)'];

## The Spiral Resonator

The spiral is a very popular geometry in a resonant coupling type wireless power transfer system for its compact size and highly confined magnetic field. We will use such a spiral as the fundamental element in this example.

**Create Spiral Geometry** The spiral is defined by its inner and outer radius, and number of turns. Express the geometry by its boundary points, then import its boundary points into pdetool. The mesh is generated in pdetool and exported. The mesh is described by points and triangles.

Rin=0.05; Rout=0.15; N=6.25; [p,t]=createSpiral(Rin,Rout,N);

**Create custom antenna** Use customAntennaMesh to import the mesh. The feed is created at the inner circle of the spiral mesh. This structure is now ready for analysis.

```
spiralobj=customAntennaMesh(p,t);
spiralobj.Tilt=90;
spiralobj.TiltAxis='Y';
createFeed(spiralobj,[0.0525 0.0025],[0.0675 0.0025]);
```

## Resonance Frequency and Mode

It is important to find the resonant frequency of the designed spiral geometry. A good way to find the resonant frequency is to study the impedance of the spiral resonator. Since the spiral is a magnetic resonator, a lorentz shaped reactance is expected and observed in the calculated impedance result.

figure; impedance(spiralobj,freq);

Since the spiral is a magnetic resonator, the dominant field component of this resonance is the magnetic field. A strongly localized magnetic field is observed when the near field is plotted.

figure; EHfields(spiralobj,fc,field_p,'ViewField','H','ScaleFields',[0 5]);

## Create Spiral to Spiral Power Transfer System

The complete wireless power transfer system is composed of two parts: the transmitter(Tx) and receiver(Rx). Choose identical resonators for both transmitter and receiver to maximize the transfer efficiency. Here, the wireless power transfer system is modeled as a linear array.

```
wptsys=linearArray('Element',[spiralobj spiralobj]);
wptsys.ElementSpacing=Rout*2;
figure;
show(wptsys);
```

## Variation of System Efficiency with Transfer Distance

One way to evaluate the efficiency of the system is by studying the S21 parameter. As presented in [1], the system efficiency changes rapidly with operating frequency and the coupling strength between the transmitter and receiver resonator. Peak efficiency occurs when the system is operating at its resonant frequency, and the two resonators are strongly coupled. The results for s-parameter analysis has been precomputed and stored in a MAT-file.

load arraysparam figure; rfplot(sparam,2,1,'abs');

**Critical Coupled Point** The coupling between two spirals increases with decreasing distance between two resonators. This trend is approximately proportional to . Therefore, the system efficiency increases with shorter transfer distance until it reaches the critical coupled regime [1]. When the two spirals are over coupled, exceeding the critical coupled threshold, system efficiency remains at its peak, as shown in Fig.3 in[1]. We observe this critical coupling point and over coupling effect during modeling of the system. Perform a parametric study of the system s-parameters as a function of the transfer distance. The transfer distance is varied by changing the ElementSpacing. It is varied from half of the spiral dimension to one and half times of the spiral dimension, which is twice of the spiral's outer radius. The frequency range is expanded and set from 25 MHz to 36 MHz.

freq=(25:0.1:36)*1e6; dist=Rout*2*(0.5:0.1:1.5); load('wptData.mat'); s21_dist=zeros(length(dist),length(freq)); for i=1:length(dist) s21_dist(i,:)=rfparam(sparam_dist(i),2,1); end figure; [X,Y]=meshgrid(freq/1e6,dist); surf(X,Y,abs(s21_dist),'EdgeColor','none'); view(150,20); shading(gca,'interp'); axis tight; xlabel('Frequency [MHz]'); ylabel('Distance [m]'); zlabel('S_{21} Magnitude');

## Coupling Mode between Two Spiral Resonator

The dominant energy exchange mechanism between the two spiral resonators is through the magnetic field. Strong magnetic fields are present between the two spirals at the resonant frequency.

wptsys.ElementSpacing=Rout*2; figure; EHfields(wptsys,fc,field_p,'ViewField','H','ScaleFields',[0 5]); view(0,0);

## Conclusion

The results obtained for the wireless power transfer system match well with the results published in [1].

## References

[1] A. P. Sample, D. T. Meyer, and J. R. Smith, "Analysis, Experimental Results, and Range Adaptation of Magnetically Coupled Resonators for Wireless Power Transfer", IEEE Transactions on Industrial Electronics, pp.544-554, 58, 2, 2011.