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SAR Calculation in a Simulant Human Body which is between the Transmitter and Receiver of the Wireless Power Transmission System Young-Jun Ju 1 , Yu-Ri Lee 1 , Dong-Yeol Lee 1 , # Yoon-Myoung Gimm 1 1 Department of Electronics and Electrical Engineering, Graduate School, Dankook University 126, Jukjeon-Dong, Suji-Gu, Yongin-Si, Gyeonggi-Do, South Korea, [email protected], [email protected], [email protected], [email protected] Abstract Self-resonance wireless power delivery systems operating at 128 kHz and 13.56 MHz were designed. SAR (Specific Absorption Rate) of homogeneous human body between the transmitter and the receiver and resonance frequency of the wireless system were calculated. Keywords : SAR Calculation Simulant Human Body Wireless Transmitter System 1. Introduction Although wireless power transfer technology was suggested by Nikola Tesla, it has not been deeply studied until self-resonance technique was announced by Marin Soljačić in 2007[1]. Usually wireless power transfer is performed by applying magnetic field and its facilities are installed where people resides, so evaluation of human body effect by the magnetic field became very important. Self-resonance wireless power transfer system was designed at 128 kHz and 13.56 MHz, and homogenous numerical human body was installed between the transmitter and the receiver. The reasons of 128 kHz and 13.56 MHz for wireless power transfer system are that 128 kHz is used for MFAN(Magnetic Field Area Network)[2] and 13.56 MHz is in a ISM band which has variables usage including RFID and NFC(Near Field Communication). 2. Self-Resonant Wireless Transmitter System Fig. 1 shows schematic diagram of self-resonance wireless power transfer system[1]. This system is more efficient than the other systems at near distance applying the resonating auxiliary coils. Figure 1: Self-resonance wireless power transfer system using the resonance coils. 3. Reference Values of Human Body Protection of Electromagnetic Fields Because of the possibility that electromagnetic fields can affect human health, many national and international EMF protection guidelines were provided. Table 1 shows basic restrictions of SAR values for frequencies up to 10 GHz[3]. Point SAR value is defined as absorption power per unit mass of the human body at a point. SARሺx, y, zሻ ൌ σሺx, y, zሻ|E ሺx, y, zሻ| /2ρሺx, y, zሻ (1) σሺx, y, zሻ ൌ Conductivity of the medium at ሺx, y, zሻ including dielectric loss ሺωԖ Ԗ ′′ ). E ሺx, y, zሻ = Vector phasor of E-field at (x, y, z). ρሺx, y, zሻ = Mass density of the material where SAR value is to be evaluated.

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Page 1: SAR Calculation in a Simulant Human Body which is between ...WeB2-1] SE02_1004.pdf · SAR Calculation in a Simulant Human Body which is between the Transmitter and Receiver of the

SAR Calculation in a Simulant Human Body which is between the Transmitter and Receiver of the

Wireless Power Transmission System Young-Jun Ju 1, Yu-Ri Lee 1, Dong-Yeol Lee 1, #Yoon-Myoung Gimm 1

1 Department of Electronics and Electrical Engineering, Graduate School, Dankook University 126, Jukjeon-Dong, Suji-Gu, Yongin-Si, Gyeonggi-Do, South Korea,

[email protected], [email protected], [email protected], [email protected]

Abstract Self-resonance wireless power delivery systems operating at 128 kHz and 13.56 MHz were

designed. SAR (Specific Absorption Rate) of homogeneous human body between the transmitter and the receiver and resonance frequency of the wireless system were calculated. Keywords : SAR Calculation Simulant Human Body Wireless Transmitter System 1. Introduction

Although wireless power transfer technology was suggested by Nikola Tesla, it has not been

deeply studied until self-resonance technique was announced by Marin Soljačić in 2007[1]. Usually wireless power transfer is performed by applying magnetic field and its facilities are installed where people resides, so evaluation of human body effect by the magnetic field became very important.

Self-resonance wireless power transfer system was designed at 128 kHz and 13.56 MHz, and homogenous numerical human body was installed between the transmitter and the receiver.

The reasons of 128 kHz and 13.56 MHz for wireless power transfer system are that 128 kHz is used for MFAN(Magnetic Field Area Network)[2] and 13.56 MHz is in a ISM band which has variables usage including RFID and NFC(Near Field Communication).

2. Self-Resonant Wireless Transmitter System

Fig. 1 shows schematic diagram of self-resonance wireless power transfer system[1]. This system is more efficient than the other systems at near distance applying the resonating auxiliary coils.

Figure 1: Self-resonance wireless power transfer system using the resonance coils.

3. Reference Values of Human Body Protection of Electromagnetic Fields

Because of the possibility that electromagnetic fields can affect human health, many national and international EMF protection guidelines were provided. Table 1 shows basic restrictions of SAR values for frequencies up to 10 GHz[3].

Point SAR value is defined as absorption power per unit mass of the human body at a point.

SAR x, y, z σ x, y, z |E x, y, z | /2ρ x, y, z (1) σ x, y, z Conductivity of the medium at x, y, z including dielectric loss ω ′′). E x, y, z = Vector phasor of E-field at (x, y, z). ρ x, y, z = Mass density of the material where SAR value is to be evaluated.

Page 2: SAR Calculation in a Simulant Human Body which is between ...WeB2-1] SE02_1004.pdf · SAR Calculation in a Simulant Human Body which is between the Transmitter and Receiver of the

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120.00Freq [kHz]

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Conductiv(S/m)( ωε

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Page 3: SAR Calculation in a Simulant Human Body which is between ...WeB2-1] SE02_1004.pdf · SAR Calculation in a Simulant Human Body which is between the Transmitter and Receiver of the

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Page 4: SAR Calculation in a Simulant Human Body which is between ...WeB2-1] SE02_1004.pdf · SAR Calculation in a Simulant Human Body which is between the Transmitter and Receiver of the

Table system

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tial peak E-fiin the body

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erences

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hysical Layerternational CCNIRP, “GectromagnetiEI/IEC62233milar Apparatp://niremf.if

CNIRP, “Guiz - 100 kHz),

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work was sBand Multi-

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Fre

ield 1213.5

AR on x-z pl

ns

wireless poAR calculatio

formed. Resthey varied in

Aristeidis Keless Power pp. 83-86, Ju, YunJae Wr for Magne

Conference onGuidelines fo

ic Fields (up3, Measurematus with Regfac.cnr.it/docidelines for L,” Health Phy

ments

supported byMode Intera

elds in the

equency

8 kHz

56 MHz

lane of Fig. 1

ower transferons in homoonance frequn 13.56 MHz

Karalis, RobTransfer via

uly 2007. Won, YongSeetic Field Arn Wireless Por Limiting

p to 300 GHzment Methods

gard to Humcs/DIELECTLimiting Exysics, vol. 99

y the IT R&Dactive Wirele

human body

Basic Restri[V/m

1,8

10. Fig

r systems oogeneous huuency and inz system with

bert Moffatta Strongly C

eok Lim, Krea Network

Pervasive ComExposure

z),” Health Phs for Electrom

man ExposureTRIC/home.hxposure to Ti9, no. 6, pp. 8

D program oess Charging

y of self-res

ction Valuesm]rms 17.3

830

gure 13: 10 g

operating at uman body bnsertion loss h regard to th

tm J.D. JoaCoupled Mag

KyeungHak Sk,” ISWPC'1mputing, pp.to Time-V

hysics, vol. 7magnetic Fiee, 2005. html. ime-Varying818-836, 201

of MKE/KEISystem for P

sonance wir

s Calculat

SAR on y-z

128 kHz anbetween theat resonanc

he human bo

annopoulos, gnetic Reson

Seo, SeungO10, Proceedin. 256-260, 20arying Elec74, no. 4, ppelds of House

g Electric an10.

IT. [1003525Portable Dev

reless power

ted E-field M[V/m]peak

0.378 7.04

z plane of Fig

nd 13.56 Me transmitterce of 128 kHody insertion

Peter Fishenances,” Scie

Ok Lim, “Dngs of the 5010. ctric, Magne. 494-522, 19ehold Applia

d Magnetic

55, Developmvice.]

r transfer

Maximum

g. 10.

MHz were r and the

Hz system n.

er, Marin ence, vol.

Design of 5th IEEE

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