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Wireless Power Transmission
Inductive coupling
• Primary and secondary coils are not
connected with wires.
• Energy transfer is due to Mutual Induction
2
CIRCUIT SCHEMATICS
working
5
Resonant inductive coupling
Resonant inductive coupling is a form of inductive coupling in
which power is transferred by magnetic field between
two resonant circuits , one in the transmitter and one in the
receiver .
The two are tuned to resonate at the same resonant frequency.
• In 2007 a team led by Marin Soljačić at MIT used two coupled tuned
circuits each made of a 25 cm self-resonant coil of wire at 10 MHz to
achieve the transmission of 60 W of power over a distance of 2 meters
(6.6 ft) (8 times the coil diameter) at around 40% efficiency.
• The two are tuned to resonate at the same resonant frequency.
• Resonant inductive coupling can achieve high efficiency at ranges of 4 to
10 times the coil diameter .
• An environmental and economic benefit of wirelessly powering small
devices such as clocks, radios, music players and remote controls is that it
could drastically reduce the 6 billion batteries disposed of each year, a
large source of toxic waste and groundwater contamination
RIC vs Inductive coupling
• RIC is highly efficient.
• RIC has much greater range than inductive
coupling.
• RIC is directional when compared to inductive
coupling.
• Devices using RIC technique are highly
portable.
Simulation of the RIC
clc
clear all
% input data for the wireless power transfer through concert.
v=input('input voltage in volts V=');
f=input(' frequency in HZ F =');
x1=input('reactance of pri.winding in ohms X1 =');
x2=input('reactance of sec.winding in ohms X2 =');
xL=input('reactance of magnatic circuit in ohms XL =');
xc1=input('capacitance reactance of pri.winding side in ohms
XC1=');
%xc2=input('capacitance reactance of sec.winding side in
ohms
XC2=');
r1=input('resistance of pri.winding in ohms r1 =');
r2=input('resistance of sec.winding in ohms r2 =');
rc=input('resistance of magnatic circuit in ohms rc =');
RL=input('load resistance of in ohms RL =');
xc2=(xL+x2);
w0=2*pi*f;
c2=(1/(w0*xc2));
c1=(1/(w0*xc1));
B=0;
if c1==B
z=((xL/(xL+x2))^2*RL)+j*((xL*x1+x1*x2+x2*xL)/(xL+x2));
fprintf('nthe value of z when C1=0 is
=%f%+fiohms',real(z),imag(z));
End
if c1~=B
z=(((xL/(xL+x2))^2*RL)^2)/((xL*x1+x1*x2+x2*xL)/(xL+x2))+((
xL*x1+x1*x2+x2*xL)/(xL+x2));
fprintf('n the value of z when C1~=0 is =%f%ohms',real(z));
end
turnsratio=1;
% to find effeiency of he system.
k=input('n Turns Ratio=');
if k==turnsratioalpha=(xL+x2)/xL;
IL=v/RL;
I1=alpha*IL;
I2=IL*(sqrt(1+(RL/xc2)^2));
I0=I1-I2;
pf=xc2/(RL^2+xc2^2);
%I0^2=IL^2*(alpha^2+(1+(RL/xc2)^2)-
2*alpha*sqrt(1+(RL/xc2)^2*pf);
eff=RL/((RL+r1*alpha^2+r2*(1+(RL/xc2)^2))+rc*(alpha^2+1+(R
L/xc2)^2-2*alpha*sqrt(1+(RL/xc2)^2*pf)));
eff1=eff*100;
fprintf('n the efficiency of the system =%f%',eff1);
end
References:
• S. Sheik Mohammed, K. Ramasamy, T. Shanmuganantham,” Wireless
power transmission – a next generation power transmission system”,
International Journal of Computer Applications (0975 – 8887) (Volume 1 –
No. 13)
• Peter Vaessen,” Wireless Power Transmission”, Leonardo Energy,
September 2009
• C.C. Leung, T.P. Chan, K.C. Lit, K.W. Tam and Lee Yi Chow, “Wireless Power
Transmission and Charging Pad”
• David Schneider, “Electrons unplugged”, IEEE Spectrum, May 2010
• Shahrzad Jalali Mazlouman, Alireza Mahanfar, Bozena Kaminska, “Mid-
range Wireless Energy Transfer Using Inductive Resonance for Wireless
Sensors”
• Chunbo Zhu, Kai Liu, Chunlai Yu, Rui Ma, Hexiao Cheng, “Simulation and
Experimental Analysis on Wireless Energy Transfer Based on Magnetic
Resonances”, IEEE Vehicle Power and Propulsion Conference (VPPC),
September 3-5, 2008
Wireless power transmission

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Wireless power transmission

  • 2. Inductive coupling • Primary and secondary coils are not connected with wires. • Energy transfer is due to Mutual Induction 2
  • 5. 5
  • 6. Resonant inductive coupling Resonant inductive coupling is a form of inductive coupling in which power is transferred by magnetic field between two resonant circuits , one in the transmitter and one in the receiver . The two are tuned to resonate at the same resonant frequency.
  • 7. • In 2007 a team led by Marin Soljačić at MIT used two coupled tuned circuits each made of a 25 cm self-resonant coil of wire at 10 MHz to achieve the transmission of 60 W of power over a distance of 2 meters (6.6 ft) (8 times the coil diameter) at around 40% efficiency. • The two are tuned to resonate at the same resonant frequency. • Resonant inductive coupling can achieve high efficiency at ranges of 4 to 10 times the coil diameter . • An environmental and economic benefit of wirelessly powering small devices such as clocks, radios, music players and remote controls is that it could drastically reduce the 6 billion batteries disposed of each year, a large source of toxic waste and groundwater contamination
  • 8. RIC vs Inductive coupling • RIC is highly efficient. • RIC has much greater range than inductive coupling. • RIC is directional when compared to inductive coupling. • Devices using RIC technique are highly portable.
  • 9. Simulation of the RIC clc clear all % input data for the wireless power transfer through concert. v=input('input voltage in volts V='); f=input(' frequency in HZ F ='); x1=input('reactance of pri.winding in ohms X1 ='); x2=input('reactance of sec.winding in ohms X2 ='); xL=input('reactance of magnatic circuit in ohms XL ='); xc1=input('capacitance reactance of pri.winding side in ohms XC1='); %xc2=input('capacitance reactance of sec.winding side in ohms XC2=');
  • 10. r1=input('resistance of pri.winding in ohms r1 ='); r2=input('resistance of sec.winding in ohms r2 ='); rc=input('resistance of magnatic circuit in ohms rc ='); RL=input('load resistance of in ohms RL ='); xc2=(xL+x2); w0=2*pi*f; c2=(1/(w0*xc2)); c1=(1/(w0*xc1)); B=0; if c1==B z=((xL/(xL+x2))^2*RL)+j*((xL*x1+x1*x2+x2*xL)/(xL+x2)); fprintf('nthe value of z when C1=0 is =%f%+fiohms',real(z),imag(z));
  • 11. End if c1~=B z=(((xL/(xL+x2))^2*RL)^2)/((xL*x1+x1*x2+x2*xL)/(xL+x2))+(( xL*x1+x1*x2+x2*xL)/(xL+x2)); fprintf('n the value of z when C1~=0 is =%f%ohms',real(z)); end turnsratio=1; % to find effeiency of he system. k=input('n Turns Ratio='); if k==turnsratioalpha=(xL+x2)/xL; IL=v/RL; I1=alpha*IL; I2=IL*(sqrt(1+(RL/xc2)^2)); I0=I1-I2; pf=xc2/(RL^2+xc2^2); %I0^2=IL^2*(alpha^2+(1+(RL/xc2)^2)- 2*alpha*sqrt(1+(RL/xc2)^2*pf); eff=RL/((RL+r1*alpha^2+r2*(1+(RL/xc2)^2))+rc*(alpha^2+1+(R L/xc2)^2-2*alpha*sqrt(1+(RL/xc2)^2*pf))); eff1=eff*100; fprintf('n the efficiency of the system =%f%',eff1); end
  • 12. References: • S. Sheik Mohammed, K. Ramasamy, T. Shanmuganantham,” Wireless power transmission – a next generation power transmission system”, International Journal of Computer Applications (0975 – 8887) (Volume 1 – No. 13) • Peter Vaessen,” Wireless Power Transmission”, Leonardo Energy, September 2009 • C.C. Leung, T.P. Chan, K.C. Lit, K.W. Tam and Lee Yi Chow, “Wireless Power Transmission and Charging Pad” • David Schneider, “Electrons unplugged”, IEEE Spectrum, May 2010 • Shahrzad Jalali Mazlouman, Alireza Mahanfar, Bozena Kaminska, “Mid- range Wireless Energy Transfer Using Inductive Resonance for Wireless Sensors” • Chunbo Zhu, Kai Liu, Chunlai Yu, Rui Ma, Hexiao Cheng, “Simulation and Experimental Analysis on Wireless Energy Transfer Based on Magnetic Resonances”, IEEE Vehicle Power and Propulsion Conference (VPPC), September 3-5, 2008