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01/22/2013 Energy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays Qian Zhang and Eun Sok Kim Department of Electrical Engineering-Electrophysics University of Southern California Los Angeles, CA 90089-0271 IEEE MEMS 2013

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Page 1: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

01/22/2013

Energy Harvesters with High Electromagnetic Conversion Efficiency

through Magnet and Coil Arrays

Qian Zhang and Eun Sok Kim

Department of Electrical Engineering-Electrophysics University of Southern California

Los Angeles, CA 90089-0271

IEEE MEMS 2013

Page 2: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

USCMEMS

Outline

Introduction Electromagnetic energy harvesting Power levels in recent harvesters

Energy harvesters with magnet and coil arrays Working principle Microfabricated energy harvester

MEMS fabrication, experimental testing setup and results Macroscale energy harvester

Experimental results and video

Summary

Page 3: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

Ocean-wave energyHydropower energyWind energy

Renewable Energy Sources

USCMEMS

From nature resourcesWind energyWater energyWave energy …

Kinetic energy

Electrical energy

Electromagnetic transductionFaraday’s lawLow working frequencyLow output impedance

Page 4: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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T.V. Galchev et al., JMM, 2011.

Frequency-increased generator Volume: 68cc Vibration: 4mm at 2Hz (55mg )Harvested power: 57μW

Optimizing arrangement of magnets Volume: 9.3cc Vibration: 85μm at 102Hz (3.6g )Harvested power: 290μW

E. Sardini et al., Sensors and Actuators A, 2011.

Recent Electromagnetic Energy Harvesters

Power ?

Page 5: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

Model of Vibration-Driven Power Generator

( )" ( ) ' ( ) 0smx t dz t k z t

( ) ( ) ( )z t x t y t

2

0 0 22 2

1 2

n

n n

Z Y

2

2

0 0 02 22 2 2 2

1 2 1 2

n n

n n n n

d dB dz dB dB dBN NS NS Z NS Y NSAdt dz dt dz dz dz

Faraday’s law

USCMEMS

20 0A Y( )

Equation of motion

10ωnωn0.1ωn

20

-20

Mag

nitu

de(d

B)

0Decreased

Page 6: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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At resonant frequency (ω=ωn) 01

2ndBNS Ydz

To increase power output, increase N and S increase ωn and Y0

larger volume and weightmore vibration energy

dBdz ?

2

0 22 2

1 2

n

n n

dBNSAdz

ωn0.1ωn 10ωn

-20

-30

-40

-50

Mag

nitu

de(d

B)

Decreased

Increasing Power Output

Page 7: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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-1 0 1 2 3 4 5

0.04

0.08

0.12

0.16

0.20 |dBz/dz|

|dB

z/dz

| (T/

mm

)Z position (mm)

0 1 2 3 4 50.00

0.04

0.08

0.12

0.16 Bz

Bz

(T)

Z position (mm)

Y

Z

N

Z

0Y

Z

X

When magnetic field is provided by a single magnet,magnetic flux change is caused by a distance change.

Magnetic flux density (Bz) and its gradient (dBz/dz)Magnetic field lines

Magnetic Flux Change – One Magnet

Page 8: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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NS

Y0

-3 -2 -1 0 1 2 3

0

2

4

d=100m d=200m d=400m

d=100m d=200m d=400m

|dB

z/dy

| (T/

mm

)

Y position (mm)

-3 -2 -1 0 1 2 3

-0.4-0.20.00.20.4

Bz

(T)

Y position (mm)

d

Y

Z

YZ

X

When magnetic field is provided by two magnets through alternating north- and south-orientation on a planar surface,magnetic flux changes in the direction parallel to the planar surfacepeaking at the boundary between two magnets increasing as the distance (d) from the magnet surface is decreased

Magnetic Flux Change – Two Magnets

Magnetic field lines Magnetic flux density (Bz) and its gradient (dBz/dy)

Page 9: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Energy Harvester with Magnet and Coil Arrays

Magnet arrayCoil array

Spring system

Magnet array with alternating north- and south-orientation on a planar surface

Coil array over the boundaries between the magnets

Vibration direction parallel to the planar surface Gap between magnet array and coil array as

close as possible

Page 10: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Fabrication Steps Microfabricated Energy Harvester

(a) KOH etching

(b) Electroplating copper

(c) Si etching by DRIE

(d) Assembling magnets

Narrow gap between the magnet array and coil array Microdiaphragm-based front-to-backside alignment technique

Page 11: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

20mm

5mm

USCMEMS

Microfabricated Electromagnetic Energy Harvester

Total volume (mm3)20×5×0.9(0.09cc)

Weight (gram) 0.5Magnet size (mm3) 4.8×4.8×0.8Coil thickness (μm) 22

Coil turns 20Coil resistance (Ω) 3.6

Coil number 3

Top-view and bottom-view

Detailed parameters

200μm wide two-fold spring

20-turn spiral coil

Page 12: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Testing Setup

Function generator

Power amplifier Shaker table

LDDM

Oscilloscope

Pre-amplifier

Page 13: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Measured Electromotive Force (EMF) vs Vibration Frequency

Three coils are connected in series At a fixed acceleration, the EMFs

peak at the resonant frequency 30mVp-p from 3.75g at 290Hz

240 260 280 300 320 3400

10

20

30

V p-p

(mV)

Frequency (Hz)

0.75g 1.5g 2.25g 3g 3.75g

Page 14: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Power Output Delivered to Loads

0.0

0.5

1.0

1.5

2.0

2.5

3.0

0.0 0.2 0.4 0.6 0.8 1.00

10

20

30

V p-p

(mV)

Current (mA)

Vp-p vs. Current Power vs. Current

Pow

er (

W)

Output voltage and power across a load for different resistanceswith the largest power

delivered to a matched load

1 2 3 40

1

2

3

Pow

er (

W)

Acceleration (g)

Power vs. Acceleration

290Hz, 11μm

Power output vs input acceleration into 10.8Ω load at the resonant frequency 2.6μW is delivered from 3.75g

acceleration at 290Hz (vibration amplitude = 11μm)

Page 15: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Total volume (mm3) 20×5×0.9 (0.09cc)Weight (gram) 0.5

Resonant frequency (Hz) 290Vibration amplitude (μm) 11

Input acceleration (g) 3.75Open circuit voltage (mVp-p) 30

Load resistance (Ω) 10.8Power output (μW) 2.6

Summary of Microfabricated Energy Harvester

Resonant frequency can be adjusted by design of silicon cantilever Coil resistance can be reduced by electroplating thick copper Number of array can be increased easily for mass production

Page 16: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Total volume (mm3)51×51×10

(26cc)Weight (gram) 90

Magnet size (mm3) 12.7×12.7×3.2Coil turns 200

Coil resistance (Ω) 8Coil number 12

Scaled up to 16 magnets and 12 coils 12 coils are connected in series Vp-p=22V at a resonant frequency of 82Hz with vibration amplitude of 414μm

Macroscale Energy Harvester

Detailed parameters Measured EMF

Page 17: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Power Output Delivered to Load

3 6 9 120

40

80

120

160

Pow

er (m

W)

Acceleration (g)

Power vs. Acceleration

82Hz, 414μm

Power output vs. input acceleration into 96Ω load 158mW is delivered from 11.2g

acceleration at 82Hz (vibration amplitude of 414μm)

Demo of the energy harvester 120mW incandescent light bulbDirectly connectedClose to the bulb’s full capacity

Page 18: Energy Harvesters with High Electromagnetic …mems.usc.edu/MEMS2013_EnergyHarvesters.pdfEnergy Harvesters with High Electromagnetic Conversion Efficiency through Magnet and Coil Arrays

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Summary

A new electromagnetic-transduction idea to increase the mechanical-to-electrical conversion efficiency array of magnets is used to provide a rapidly changing

magnetic field

The microfabricated energy harvester, occupying a volume of 0.09cc weighing 0.5 gram, produces 2.6μW at 290Hz (vibration amplitude of 11μm)

The macroscale version, that is scaled up to 26cc weighing 90 gram, generates 158mW at 82Hz (vibration amplitude of 414μm), and lights an incandescent light bulb