Wireless Non-radiative Energy(power) Transfer

  • June 2020
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Wireless

Non-Radiative

Energy Transfer

Motivation

Tesla tower: cca. 1904

WLAN (wireless local area network) concept: radiation

Radiative energy transfer

Omni-directional radiation

Directed radiation

Resonance phenomena 2

2 h − ∇ ψ = Eψ 2m

Schrödinger equation

− c 2∇2 E = ω 2 E Maxwell equation

ε=65.61, Q=9100 Titania (ε ≈ 96, Im{ε}/ε ∼ 10 -3 ) Barium tetratitanate (ε ≈ 37, Im{ε}/ε ∼ 10 -4 ) Lithium tantalite (ε ≈ 40, Im{ε}/ε ∼ 10 -4 )

ε=147.70, Q=1992

Resonant coupling

resonant object (Source)

resonant object (Device)

da S = −i (ωS + iΓS )a S + iκ SD a D dt

daD = −i (ωD + iΓD )aD + iκ DS aD dt

∗ 3 ωS ∫ d rES (r )ED (r )[ε S (r ) − ε 0 ]

∗ 3 d rE ωD ∫ D (r )E S (r )[ε D (r ) − ε 0 ] ≡ 2 2 d 3r E (r ) ε (r )

κ SD ≡

2

∫ d r E (r ) ε (r ) 2

3

κ DS

S

κ ≡ κ SDκ DS



D

Example of resonant coupling Source

Device

START

END

6

8

Distance / Radius

10

One more example of resonant coupling

Coupling with extraneous objects D

e-αx Source

Extraneous object

da S = −i (ωS + iΓS )a S + iκ SE a S dt

ω1 ∫ d r ES (r ) [ε E (r ) − ε 0 ] 2

3

κ SE ≡

2

3 d ∫ r ES (r ) ε (r ) 2

∝ e-2αD

D

e-αx Source

Device ∗ 3 ωS ∫ d rES (r )ED (r )[ε S (r ) − ε 0 ]

da S = −i (ωS + iΓS )a S + iκ SD a D κ SD ≡ 2 dt

∫ d r E (r ) ε (r ) 2

3

S

∝ e-αD

Examples of extraneous coupling ε =2.5

Q = 1992

Q = 1832

Concrete (ε ≈ 4.5, Im{ε}/ε∼10 -2 ) Wood (ε ≈ 1.2-5, Im{ε}/ε∼10 -3 ) Fused quartz (ε ≈ 4.0, Im{ε}/ε∼10

-4

ε =2.5

Q = 873

) QFINAL 1 ≈ QINITIAL 3

ε = 82

Robot & Office: simulation

Source

Device (robot)

Robot & Office: radiative scheme

Robot & Office: non-radiative scheme

Robot & Office: non-radiative scheme

Magnetic resonances B

E Outside: UE~UB

Outside: UE~0 Most materials: µ~µAIR ⇒ no interaction with the field!

Examples of “magnetic technology”

Maglev

Magnetically levitating bed

Robot & Office: magnetic resonances

Q~1000

AC source ~10MHz

1m

3-4m 30cm

Q~1000

Robot & Office: magnetic resonances

Comparison with inductive coupling

D»L Efficiency ≈ ηR/Q2

D L

~ ηR/1,000,000 D

L»D

L

Efficiency ≡ ηR

Some potential applications

Industrial, military, and household robots

Portable personal electronics

Electric vehicles

Other possible applications

• Confidential radio-communication • Optical free-space interconnects for electronic logic circuits • Energy supply for RFIDs and/or nano-robots

Conclusion • mid-range non-radiative energy transfer scheme based on resonances • even very simple designs have promising performance • as a powerful concept, it could enable a wide range of applications

Ok, but how come no one thought of this before?

Collaborators: Aristeidis Karalis (MIT) John Joannopoulos (MIT)

e-mail: [email protected] Pre-print of this work: http://arxiv.org/abs/physics/0611063

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