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Wireless electricity for Implants in Body Sensor Networks CHAPTER 1 INTRODUCTION In recent years, wireless body sensor network (wBSN) has gained tremendous interest in research community [1].Using this network, wireless sensors can be affixed to the skin or the underside of clothes to perform a variety of important tasks, such as monitoring vital signs, evaluating motor functions, and measuring physical activity .Micro sensors may albe implanted within the body by either surgery or injection to perform additional functions, such as restoring lost vision, hearing, and motor functions, releasing drugs, and monitoring cancer or cardiovascular diseases. In the military fields, a wBSN embedded within the clothes is highly desirable since it can potentially produce warning signals of imminent attacks, detect the presence of people or objects of interest, monitor chemicals in the air, evaluate wounds, and communicate with a central station or an assistive device such as a rescue robot. With the development of innovative wearable and implantable biosensors, the applications of wBSN have been extended from physiological monitoring to everyday healthcare, as well as fitness, sports and security. Despite the recent developments in low power sensing devices and interface circuitry, system integration, Department of CSE, TOCE Page 1

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Wireless electricity for Implants in Body Sensor Networks

CHAPTER 1

INTRODUCTION

In recent years, wireless body sensor network (wBSN) has gained tremendous

interest in research community [1].Using this network, wireless sensors can be affixed to

the skin or the underside of clothes to perform a variety of important tasks, such as

monitoring vital signs, evaluating motor functions, and measuring physical

activity .Micro sensors may albe implanted within the body by either surgery or injection

to perform additional functions, such as restoring lost vision, hearing, and motor

functions, releasing drugs, and monitoring cancer or cardiovascular diseases.

In the military fields, a wBSN embedded within the clothes is highly

desirable since it can potentially produce warning signals of imminent attacks, detect the

presence of people or objects of interest, monitor chemicals in the air, evaluate wounds,

and communicate with a central station or an assistive device such as a rescue robot. With

the development of innovative wearable and implantable biosensors, the applications of

wBSN have been extended from physiological monitoring to everyday healthcare, as well

as fitness, sports and security. Despite the recent developments in low power sensing

devices and interface circuitry, system integration, sensor miniaturization, wireless

network communication and signal processing, the critical energy problem in wBSN has

not yet been solved.

It is a challenge to power a highly distributed network of electronic devices

without wired connections and batteries. Currently, many wBSNs use a separate battery

for each sensor node, which is obviously inconvenient, costly, and difficult to maintain.

In the case of implantable sensors, these problems become even more serious. It is highly

desirable that the implants are able to receive energy outside of the body wirelessly to

avoid the use of transcutaneous wires or the battery replacement by surgery. In 2007, a

new wireless energy transfer technology was reported in Science [2]. This technology is

often called witricitry (a short form of “wireless electricity”) which has been used to

transmit a considerably large amount of power [2-6]. For example, the original paper [2]

reported a wireless power of 60-walt which fully illuminated a light bulb approximately

two meters away from a power source with an efficiency of approximately 40%.

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This initial experiment demonstrated the feasibility of witricity in wireless

power transfer over a “midrange”, defined as a distance equal to several times of the

resonator size. This experiment also showed that, when compared to the existing

methods, the power transfer by witricity was much less affected by the adjacent non-

resonant objects including biological tissues. Despite these advantages, the system

utilized two large coil resonators of 60 cm in diameter which were excessively large and

structurally unsuitable in practical applications,

1.1 Main Challenges For Wireless Electricity

Induction methods: The electrodynamic induction wireless transmission

technique is near field over distances up to about one-sixth of the wavelength used.

Near field energy itself is non-radiative but some radiative losses do occur. In

addition there are usually resistive losses. With electrodynamic induction, electric

current flowing through a primary coil creates a magnetic field that acts on a

secondary coil producing a current within it. Coupling must be tight in order to

achieve high efficiency. As the distance from the primary is increased, more and

more of the magnetic field misses the secondary. Even over a relatively short range

the inductive coupling is grossly inefficient, wasting much of the transmitted energy.

Directed radio waves: Power transmission via radio waves can be made more

directional, allowing longer distance power beaming, with shorter wavelengths of

electromagnetic radiation, typically in the microwave range. A rectenna may be used

to convert the microwave energy back into electricity. Rectenna conversion

efficiencies exceeding 95% have been realized. Power beaming using microwaves

has been proposed for the transmission of energy from orbiting solar power

satellites to Earth and the beaming of power to spacecraft leaving orbit has been

considered

Microwave methods: In the case of electromagnetic radiation closer to visible

region of spectrum (10s of microns (um) to 10s of nm), power can be transmitted by

converting electricity into a laser beam that is then pointed at a solar cell receiver.

This mechanism is generally known as "powerbeaming" because the power is beamed

at a receiver that can convert it to usable electrical energy.

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1.2 Existing Wireless Electicity System First Experiment Of Witricity

The first experiment of historicity, the concept of wireless electricity, was conducted in

the year 2006, by researchers from Massachusetts Institute of Technology. The Assistant

Professor of this team of researchers was Marin Soljacic.

This experiment was done using two copper coils of diameter two feet, a transmitter

that was attached to a power source and a receiver that was placed about seven feet

from the transmitter. This receiver was attached to a light bulb and once power was

switched on at the transmitter, the bulb lit up despite there being no physical

connection between the transmitter and receiver.

The MIT researchers have been able to power a 60 watt light bulb from a power source

that is located about seven feet away, while providing forty percent efficiency. This was

made possible using two copper coils that were twenty inches in diameter which were

designed so that they resonated together in the MHz range. One of these coils were

connected to a power source while the other, to a bulb. With this witricity setup, the bulb

got powered even when the coils were not in sight.

Data collected through measurements showed that there was transference of 40% of

electricity through witricity. The interesting part of the electricity was that the bulb

glowed despite the fact that wood, metal and other devices were placed in between the

two coils.

This concept of witricity was made possible using resonance where an object vibrates

with the application of a certain frequency of energy. So two objects having similar

resonance tend to exchange energy without causing any effects on the surrounding

objects. Just like in acoustic resonance, where there is a chance of a glass breaking if you

strike the right tone, witricity is made possible with the resonance of low frequency

electromagnetic waves.

In this experiment, the coils were resonated at 10 MHz where the cols coupled and energy

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made to flow between them. With each cycle, more pressure and voltage built up in the

coil till the accumulation of voltage provided enough pressure and energy to flow to the

light bulb. These low frequency electromagnetic waves are rather safe as though the body

responds strongly to electric fields; it has almost zero response to absorbing power from a

magnetic field.

Fig: power a 60 watt light bulb from a power source

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The main objective of this research is to achieve resilience by adding two new,

real time data mining-based layers to complement the two existing non-data mining

layers. These new layers will improve detection of fraudulent applications because the

detection system can detect more types of attacks, better account for changing legal

behaviour, and remove the redundant attributes.

These new layers are not human resource intensive. They represent patterns in a

score where the higher the score for an application, the higher the suspicion of fraud (or

anomaly). In this way, only the highest scores require human intervention. These two new

layers do not use external databases, but only the credit application database. And

crucially, these two layers are unsupervised algorithms which are not completely

dependent on known frauds but use them only for evaluation.

The main contribution of this paper is the demonstration of resilience, with

adaptivity and quality data in real-time data mining-based detection algorithms. The

second contribution is the significant extension of knowledge in credit application fraud

detection because publications in this area are rare. In addition, this research uses the key

ideas from other related domains to design the credit application fraud detection

algorithms. Finally, the last contribution is the recommendation of credit application

fraud detection as one of the many solutions to identity crime. Being at the first stage of

the credit life cycle, credit application fraud detection also prevents some credit

transactional fraud.

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CHAPTER 2

RELATED WORK

2.1 Developments Made So Far

As witricity is in the developmental stage, lots of work is still to be done in improving

it as it is disclosed that witricity power applications operate at only 40% efficiency.

However, Intel reproduced the MIT group's experiment by wirelessly powering a

light bulb with 75% efficiency at a shorter distance.

Just as beneficial witricity may be, there are some contraindications to the concept,

with debates if it is risky living next to power lines and having a low power witricity

network running in the home. They wonder what happens if a glass of water is spilt in

a witricity room. This has also been achieved.It is realized that instead of irradiating

the environment with electromagnetic waves, a power transmitter could fill the space

around it with a "non-radiative" electromagnetic field. Essentially, energy would only

be picked up by gadgets specified to "resonate" with the frequency.

However despite these contraindications, witricity has a bright future with the many

advantages it provides in terms of weight, convenience and portability of electrical

appliances

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CHAPTER 3

PROPOSED METHODS

3.1 Understanding Witricity Based On Coupled Mode Theory

Fig:3.1 Basic components of Witricity system

As shown in Fig. 1, the witricity system consists of

tworesonators (labeled as “Source” and “Device”), a driving loop, and an output loop.

The source resonator is coupled inductively with the driving loop which is linked to an

oscillator to obtain the energy for the system. Similarly, the device resonator is coupled

inductively with the output loop to supply power to an external load.As discussed in over

a greater distance, the conventional non-resonant magnetic induction method (such as

those used in transformers) is inefficient to transmit energy because of the rapid decrease

in magnetic coupling between the primary and secondary coils.

In the witricity design, strongly coupled magnetic resonance is

utilized, which increases the transfer efficiency dramatically by "tunneling" the magnetic

fields from the source resonator to the device resonator, provided that both resonators

have the same resonant frequency. Due to this tunneling effect, the distance of

transmission can be extended significantly The physical principle of operation is that, if

two resonators are in the midrange as defined previously, their near fields (evanescent

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waves) will strongly couple each other, allowing the total energy to concentrate on a

specific resonant frequency.

This “tuned” form of energy travels between the two resonators in

an oscillatory fashion, rather than mono directional as observed in traditional systems.

The respond time of the oscillatory energy transfer is designed to be much shorter than

the time constant of system losses. Since the resonant wavelength is much larger than the

diameter of the resonators, the coupling magnetic fields can effectively circumvent

extraneous non-resonant objects in the path of energy transfer. Therefore, this midrange

energy-transfer scheme does not impose the “lineof- sight” condition, which is highly

desirable in many practical applications. Under the same energy transmitted from a

distance, the witricity system can be more safely implemented than electromagnetic

energy transfer systems because the witricity system can be designed to use the magnetic

field in energy transfer and this type of field interacts weakly with living organisms.

3.2 Evanescent Wave Coupling (EWC) Or non-radiative energy transfer, introduces a concept called “resonance” to the wireless energy equation. Similar to mutual induction, wherein electricity traveling along an electromagnetic wave moves between coils on the same frequency, EWC functions on the concept that if you make both coils resonate at the same frequency, electricity can be passed between them at farther distances and without health dangers. According to this theory, one can even send electricity to multiple devices at once, as long as they all share the same resonance frequency. While this technology is yet to come to market, in 2007, researchers at MIT published a detailed report describing a working prototype they had built which powered a light bulb from two metres away.

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Fig:3.2 A depiction of how Evanescent Wave Coupling would work.

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CHAPTER 4

EXPERIMENTAL RESULTS

4.1 Resonators Energy Calculation:

The simple formalism for the temporal dynamic of a resonant mode is particularly well

suited for the description of coupling between two witricity resonators. Considering the

equations of motion of the amplitudes a1( t) anda2 ( t) of two coupled lossless resonators

with natural frequencies

Where 12 k and 21 k are the coupling coefficients between two modes and can be treated

as complex numbers rather than operators. According to the law of energy conservation,

a restriction on 12 k and 21 k should be imposed. In then extreme case where no energy

loss is assumed, the time rate of energy change must vanish, given by

Since a1(t) and a2(t) can have arbitrary initial amplitudes and phases, the coupling

coefficients satisfy

Solving for the natural frequencies of the coupled systems, we can obtain two

homogeneous equations in the amplitudes and a1(t) and a2(t) from (1) and (2).

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Equation (7) indicates that the two frequencies of the coupled system are separated by

In particular, when , the difference between the two natural

frequencies of the coupled modes is

Suppose, initially, that at a1(t) and a2(t) are specified. Then, the two solutions of

equations (1) and (2) are expressed.

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:

Fig 4.1 Energies for (a) symmetric resonant case (b) general case.

Considering, without loss of generality, the case where the

total system energy equals unity, a1(0)=1 and a2(0)=0 and

, we have

4.2 Design Of Witricity Resonator

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For the wBSN application, a thin-film belt-shaped

resonator is highly desirable. This type of resonator can be imprinted or embedded on the

exterior or interior cover of the parent device to which the electric power will be

transferred without taking its interior space. This thin-film design not only utilizes the

maximum dimensions of the parent device to capture magnetic flux, but also provides the

maximum space for the parent device itself. In addition, it facilitates heat dispersion. Our

cylindrical resonator design consists of three layers of films as shown in Fig. 3a: two

layers of copper (red) and one layer of insulator (blue). The top and middle panels in Fig.

3a show, respectively, the top and side views of the resonator. The horizontal narrow

copper strips (red) in the middle panel represent a helical inductor. The yellow lines

represent the spaces between the copper strips. The bottom panel shows the side view

from the interior. Several vertical copper strips (red) are affixed to the insulator film

(blue). These vertical strips form physical capacitors with the coil conductors in the

exterior layer. Clearly, this thin-film design represents a compact LC tank circuit.

In our design, energy transfer is primarily provided

by the magnetic field, while the electric field is mostly confined within the physical

capacitors. This feature effectively prevents the leakage of the electrical field and helps

reduce health concerns since the biological tissue (and other electrically conductive

objects) interacts much more strongly with electric fields than with magnetic fields.

Another motivation of our design is to obtain a compact size. By increasing the

capacitance using the strips while keeping the same inductance in the LC tank resonator,

the operating frequency of the witricity system can be reduced, which is desirable in

many practical applications where the size of the parent device is small. In practical

applications, the size and shape of the source resonator have fewer restrictions and can be

larger than that of the device resonator.

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Fig 4.3: Thin-film belt shaped resonator: (a) cylindrical structure

4.3 Design of RF Power Source

A larger source resonator can produce stronger magnetic

fields for a longer transmission range. Conversely, the size of the device resonator,though

preferred to be as large as possible, is usually limited by the size of the parent device. As

shown in Fig.3b, in our experiments, we made a larger transmitter resonator in the form

of Fig. 3a. It was a large flexible ring with diameter 350 mm, thickness 0.35 mm, and

width 29 mm. The insulator had a dielectric constant of 3.74. The exterior copper tape

(width 0.635 cm) formed a 4- turn coil. Eight copper strips with 2.54-cm widths were

affixed to the insulator film on the internal side. The resonator was incorporated into the

waist belt, and the one oneturn driving coil (a loop) linked to the RF power source can

was attached on the belt to make the system wearable.

Using vector network analyzer (8753ES), we set its resonant

frequency to be 7 MHz and Q value was measured to be51.62, which was likely lower

than its true value because aprecise Q measurement was difficult without expensive

equipment and the error was expected to be large. Likewise, based on the design in Fig.

3a, a smaller receiver resonator was made as shown in Fig. 3c. The exterior copper strip

with 0.635-cm width formed a 6-turn coil, and six copper strips with 2.54-cm widths were

affixed to the insulator film on the internal side. The radius and height of the cell were

about 8.1 cm and 5 cm, respectively. Similarly, we also designed much smaller resonator

for other body part such as arm. A seven-turn coil was used as the output coil to connect

and power the load. We also set its resonant frequency to be 7 MHz and measured its Q

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value as 56.38. For the purpose of observation, an LED was first used as the load,

simulating the load effect of electronics devices and allowing visual examination.

This LED was then replaced by a resister from which

quantitative measurements was performed. In order to satisfy the requirement of

commonly usedn electronics devices, we also believe the planar structure will be

desirable since it will be easily implemented by printing this resonator on the internal or

external cover, or embedded in the clothes. Similarly with above cylindrical structures, as

shown in Fig.3d and 3e, a planar thin-film receiver resonator

is also designed. It includes three layers: the top metal layer formed a planar spiral

rectangular coil by attaching the metal strip on an insulated thin film (middle layer,

transparent), underneath which there are several separated vertical metal strips. The top

metal strip and bottom metal strips can form capacitors, resulting in a compact LC tank

resonator. Due to page limitation, we will focus on the cylindrical structure.

Fig 4.3: Thin-film belt shaped resonator: (b)transmitter resonator; (c) receiver resonator;

(d) and (e) planar resonator

4.4 Experimental Results

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Fig. 4.3 shows an experimental 7 MHz witricity system on a workbench.

Wireless energy fully illuminated the LED. When we misaligned the axes of

source and device resonators, the power was still be transmitted efficiently as

shown in Fig.4b. This phenomenon differs from that of the conventional

magnetic induction methods. In order to evaluate system performance

quantitatively, we replaced the LED with a resistor whose resistance

approximates the impedance of the output terminals at resonance. Utilizing a

diode-based RF detector, we measured the RF energy at the input terminals

of the driving loop and the energy at the loadterminals of the output loop.

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Fig 4.3(a) Measured transmission efficiency vs. distances of separation

Then the power transfer efficiencies with and

without misalignment are measured and plotted in Fig.5. It can be seen that,

the efficiency without misalignment can reach approximately 80 % at a 15-

cm separation between the transmitter and receiver. It can also be seen that

certain misalignments (e.g. 5 cm) between transmitter and receiver cause

only a slight drop in efficiency. This tolerance in misalignment is highly

desirable in practical applications since, for example, it allows energy to be

transmitted to a moving target or multiple locations as in the case of wBSN.

As [2, 3], we also arrived at the same conclusion that the uninterruptible line

of- sight between the transmitter and receiver is unnecessary in the witricity

system. Also in [9], we reported a relay effect of witricity, which allows a

much longer effective transmission distance with one or more relay resonator

between source and device resonators. Obviously, this physical mechanism

will further enhance the robustness of

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CHAPTER 5

CONCLUSION

As a new method of wireless energy transfer, witricity has a high potential in medical

applications. In this paper, we investigate the feasibility of witricity in providing wireless

power to body sensor networks. A theoretical analysis has been presented to understand

the oscillatory behavior in system operation. A novel type of thin film belt-shaped

resonators has been designed, fabricated and measured. A witricity prototype system was

built and evaluated. Our experimental results have indicated that the witricity technology

provides a powerful solution to power multiple sensors in wireless body sensor networks

REFERENCES

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Wireless electricity for Implants in Body Sensor Networks

[1] G.Z. Yang, “Body sensor networks”, Birkhauser, 2006, ISBN: 978-1- 84628-272-0

[2] A. Kurs, A. Karalis, R. Moffatt, J. D. Joannopoulos, P. Fisher, and M. Soljacic,

“Wireless Power Transfer via Strongly Coupled Magnetic Resonances”, Science, Vol.

317, pp. 83-86, Jul. 2007.

[3] A. Karalis, J.D. Joannopoulos, and M. Soljacic, “Efficient Wireless Non-radiative

Mid-range Energy Transfer”, Annals of Physics, Vol. 323, pp. 34-48, Jan. 2008.

[4] V. Chrisianto and F. Smarandache, “A note on Computer Solution of Wireless

Energy Transmit via Magnetic Resonance”, Process in Physics, Vol. 1, pp.81 83, Jan.

2008.

[5] Y. Hori, “Motion Control of Electric Vehicles and Prospects of supercapacitors”,

IEEJ Transactions on Electrical and Electronic Engineering, Vol.4, pp.231-239, Feb.

2009.

[6] A. Kurs, R. Moffatt, and M. Soljacic, “Simultaneous mid-range power transfer to

multiple devices”, Applied Physics Letters, Vol.96, pp.044102, Jan. 2010

[7] F. Zhang, S. A. Hackworth, X. Liu, H. Chen, R. J. Sclabassi, and M. Sun, “Wireless

Energy Transfer Platform for Medical Sensors and Implantable Devices”, IEEE

International Conf. of EMBS, Minneapolis, Minnesota, USA, Sep. 2-6, 2009.

[8] F. Zhang, X. Liu, S. A. Hackworth, R. J. Sclabassi, and M. Sun, “In Vitro and In

Vivo Studies on Wireless Powering of Medical Sensors and Implantable Devices,” Fourth

annual IEEE-NIH Life Science Systems and Application, Bethesda, Maryland, USA, Apr

9-10, 2009.

[9] F. Zhang, S. A. Hackworth, W. Fu and M. Sun, “The Relay Effect on Wireless Power

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Computation, Chicago Illinois, USA, May 9-12, 2010.

[10] H. Haus, Waves and Fields in Optoelectronics, Chapter 7, Prenticehall, Englewood

Cliffs, NJ,1984

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