Wearable Shoe-Mounted Piezoelectric Energy Harvester for a Self-Powered Wireless Communication System

: This study covers a self-powered wireless communication system that is powered using a piezoelectric energy harvester (PEH) in a shoe. The lead-zirconate-titanate (PZT) ceramic of the PEH was coated with UV resin, which (after curing under UV light) allowed it to withstand periodic pressure. The PEH was designed with a simple structure and placed under the sole of a shoe. The durability of the PEH was tested using a pushing tester and its applicability in shoes was examined. With periodic compression of 60 kg, the PEH produced 52 µ W of energy at 280 k Ω . The energy generated by the PEH was used to power a wireless transmitter. A step-down converter with an under-voltage lockout function was used to gather enough energy to operate the wireless transmitter. The transmitter can be operated initially after walking 24 steps. After the transmitter has been activated, it can be operated again after 8 steps. Because a control center receives signals from the transmitter, it is possible to check the status of workers who work outside at night or mostly alone, to detect emergencies.


Introduction
As technology advances, people are more able to address concerns about their safety and health.To meet these needs, various products including wearable devices are being released, and these devices are used to collect and process user information like bio-signals, location, and momentum.The proliferation of wearable devices has made it clear that more electrical energy is required to operate them well.However, due to the limited hours of any battery, users cannot avoid the constant struggle of recharging or replacing batteries.For this reason, low-power circuits have been developed to reduce battery consumption over extended periods of time [1][2][3].Nevertheless, because the capacity of any battery is limited, dead battery conditions cannot be avoided.Therefore, users of electronic devices still have to recharge these batteries or periodically replace them.Battery use comes with many difficulties for product development other than the hours of use, for example, deciding on the appropriate placement of a battery in such devices is often a design challenge.For example, a battery holder should be designed for easy battery replacement by providing ready access to users.Especially for wearable devices, this design problem gets worse because the space available for a battery is very limited.Many of these problems can be solved by replacing a battery with an energy-harvesting device.Energy harvesting involves the conversion of waste energy into renewable electrical energy [4].Many studies have been conducted on different methods of energy harvesting, including piezoelectric [5][6][7][8], electromagnetic [9], triboelectric [10][11][12], and solar energy sources [13][14][15].Among these materials, piezoelectric ones have advantages for applications in wearable devices; for example, piezoelectric materials are not affected by ambient conditions (as is the case with solar panels) because they utilize mechanical energy to generate electricity [16].Moreover, they can be designed to be quite thin [17], which allows easy integration into a system with wireless sensors that need to be powered [18][19][20].
For this reason, there are many studies in which piezoelectric materials have been applied to wearable devices [21].Among these studies, are some that apply PEHs to shoes.Because the entire body load during walking is concentrated on the foot, the piezoelectric device can generate relatively more electricity at that position than with other body parts [22][23][24][25].The large input energy from physical motion can generate substantial power using piezoelectric materials [26].Kuang et al. [27] fabricated a sandwiched piezoelectric transducer placed in a boot.The test was performed on a treadmill and 2.5 mW was generated from the transducer.Yin et al. [28] used two piezoelectric devices and a gear in their design of a frequency-up conversion piezoelectric harvester (impact type).Simulations were carried out according to the different motion states of the piezoelectric device and analysis was conducted on the output power, which varies with the gait frequency.Adsno et al. [29] developed a PEH with a parallel link structure and six multi-layered piezoelectric transducers.The generator and LEDs were installed in a safety shoe and generated the power (1.29 mW) used to power the LEDs.Moro and Benasciutti [23] developed energy harvesting shoes that included a rectangular bimorph with a tip mass and then compared numerical and experimental results.The PEHs designed in these studies have a certain volume due to their mechanical structure that made it essential to deform the shoes to be able to install the PEH inside the shoes.This could cause considerable inconvenience to users.
There are cases in which piezoelectric devices were applied to shoes without an additional mechanical structure to avoid changing the shoe structure and causing inconvenience to the user due to the size of the PEH.Chaudhary and Azad [30] evaluated the power generated by piezoelectric devices embedded inside the shoes according to the types of shoes and sizes of piezoelectric devices.However, when a piezoelectric device is directly applied to a shoe without any mechanical structure, the limited deformation possible with such a simple device limits the power that can be generated.Han et al. [31] developed a motion recognition insole that supplied power by stretching piezoelectric films (PVDF).Two demonstrations were performed to charge a smartwatch and a smart band by scavenging energy from human motion.Because the piezoelectric film is flexible, it is very advantageous to apply it to wearable devices.It has the advantage that it does not cause user discomfort and does not break, unlike hard types of piezoelectric devices [32].
However, because the piezoelectric film has a high internal impedance, when a load with a low impedance is connected, the power delivered to the load is low due to the impedance matching issue.Thus, the energy provided by the piezoelectric film is remarkably low for performance purposes.
Herein, we have overcome the limitation of volume in previous studies by developing a PEH consisting of only one spring.In addition, the durability problem of piezoelectric ceramic (hard type) was solved by applying UV coating to a piezoelectric device so that the performance can be maintained even under the continuous pressure of the user.The PEH makes it very suitable for use in shoes.Through this device, sufficient power can be produced to drive a wireless transmitter using only the user's weight.This wearable device can be applied to protect those who work outside at night or mostly alone and supports a rapid response to sudden accidents by transmitting periodic signal transmissions to a control center (Figure 1).

UV Coating
This piezoelectric device consists of a PZT ceramic over a substrate plate of stainl steel (304SS).Table 1 lists the material properties of the piezoelectric device.The PZT ramic can be broken or cracked under the force of a sudden impact or critical displa ment, as shown in Figure 2a.Consequently, cracks in the PZT ceramic lead to a decre in energy generation.To address this problem, first, the surface of the PZT ceramic w covered with a flexible conductive tape as an assistive electrode layer.This electrode m imizes losses in the harvested energy by connecting the individual pieces if the PZT ramic breaks.Second, UV resin (FA-5, CHEMITECH Industry) was deposited on the ramic to improve its structural durability to allow it to withstand better the pressure plied from the user's weight.The resin was cured with a UV-wavelength lamp (ELC-40 Electro-Lite Inc., Bethel, CT, USA), as shown in Figure 2b.This method is detailed i report by Hong et al. [32].The four layers of the piezoelectric device with UV coating shown in Figure 2c.

Design of a Piezoelectric Energy Harvester for a Shoe 2.1. UV Coating
This piezoelectric device consists of a PZT ceramic over a substrate plate of stainless steel (304SS).Table 1 lists the material properties of the piezoelectric device.The PZT ceramic can be broken or cracked under the force of a sudden impact or critical displacement, as shown in Figure 2a.Consequently, cracks in the PZT ceramic lead to a decrease in energy generation.To address this problem, first, the surface of the PZT ceramic was covered with a flexible conductive tape as an assistive electrode layer.This electrode minimizes losses in the harvested energy by connecting the individual pieces if the PZT ceramic breaks.Second, UV resin (FA-5, CHEMITECH Industry) was deposited on the ceramic to improve its structural durability to allow it to withstand better the pressure applied from the user's weight.The resin was cured with a UV-wavelength lamp (ELC-4001, Electro-Lite Inc., Bethel, CT, USA), as shown in Figure 2b.This method is detailed in a report by Hong et al. [32].The four layers of the piezoelectric device with UV coating are shown in Figure 2c.Energies 2022, 15, 237 5 of 12

Characteristic of PZT Ceramic
The PZT ceramic (of a perovskite unit with Pb 2+ , O 2-, Ti 4+ , or Zr 4+ ) generates electrical potential by converting applied mechanical stress.The piezoelectric ceramic cannot generate electrical potential (Figure 2d(i)) without mechanical stress.Conversely, when a stress is applied from the outside, the piezoelectric ceramic creates an electric potential with a polarity that changes according to whether the ceramic is being compressed (Figure 2d(ii)) or released (Figure 2d(iii)).

Piezoelectric Energy Harvester
Figure 3a,b shows a schematic and real image of the PEH with a unimorph piezoelectric device having UV coating and flexible conductive tape.This piezoelectric device is fixed on a base with rivets on one side, and a spring is inserted between the piezoelectric device and the base.The advantage of this structure is the second generation effect.The first generation effect occurs when the PEH is pushed.During this period, the spring is compressed.Alternatively, the second generation effect occurs during the recovery period of the spring.In addition, the PEH does not cause any inconvenience to the user as it requires little volume in the shoe because of the simple structure of the PEH (compressed height 2 mm, released height 7.5 mm).The PEH is fixed with rivets on the inner bottom of the shoe and is covered by an insole.The PEH is located in the heel, as shown in Figure 3c.The PZT ceramic (of a perovskite unit with Pb 2+ , O 2-, Ti 4+ , or Zr 4+ ) generates electrical potential by converting applied mechanical stress.The piezoelectric ceramic cannot generate electrical potential (Figure 2d(i)) without mechanical stress.Conversely, when a stress is applied from the outside, the piezoelectric ceramic creates an electric potential with a polarity that changes according to whether the ceramic is being compressed (Figure 2d(ii)) or released (Figure 2d(iii)).

Piezoelectric Energy Harvester
Figure 3a,b shows a schematic and real image of the PEH with a unimorph piezoelectric device having UV coating and flexible conductive tape.This piezoelectric device is fixed on a base with rivets on one side, and a spring is inserted between the piezoelectric device and the base.The advantage of this structure is the second generation effect.The first generation effect occurs when the PEH is pushed.During this period, the spring is compressed.Alternatively, the second generation effect occurs during the recovery period of the spring.In addition, the PEH does not cause any inconvenience to the user as it requires little volume in the shoe because of the simple structure of the PEH (compressed height 2 mm, released height 7.5 mm).The PEH is fixed with rivets on the inner bottom of the shoe and is covered by an insole.The PEH is located in the heel, as shown in Figure 3c.

Simulation
To carry out numerical simulation of the voltage output of a piezoelectric device under applied force, COMSOL multi-physics software was used, which is based on finite element modeling.The piezoelectric-solid interaction module of COMSOL was used for this purpose.For a linear piezoelectric material, the electromechanical equations in matrix form can be written as (IEEE Standard on Piezoelectricity, ANSI Standard 176-1987): where s E is the fourth-order strain components at a constant electrical field.The term ε T is the second-order dielectric constant tensor at constant mechanical strain.The third-order tensor of piezoelectric coefficients is expressed by the term d.The term T and S represents a second-order stress tensor and strain tensor respectively, whereas D and E represent the electric displacement vector and electric field components, respectively.The purpose of the simulation was to estimate the open-circuit voltage across the piezoelectric device.This piezoelectric device has an attached cantilever (304SS), which is fixed at one end and free at the other end.In this application, the free end of the cantilever can displace up to a fixed value of displacement (~7.5 mm), as shown in Figure 4a.Due to the displacement strain developed in the piezoelectric device, the voltage shown in Figure 4b is generated.
Energies 2022, 15, x FOR PEER REVIEW 6 of 12 To carry out numerical simulation of the voltage output of a piezoelectric device under applied force, COMSOL multi-physics software was used, which is based on finite element modeling.The piezoelectric-solid interaction module of COMSOL was used for this purpose.For a linear piezoelectric material, the electromechanical equations in matrix form can be written as (IEEE Standard on Piezoelectricity, ANSI Standard 176-1987): where s E is the fourth-order strain components at a constant electrical field.The term ε T is the second-order dielectric constant tensor at constant mechanical strain.The third-order tensor of piezoelectric coefficients is expressed by the term d.The term T and S represents a second-order stress tensor and strain tensor respectively, whereas D and E represent the electric displacement vector and electric field components, respectively.The purpose of the simulation was to estimate the open-circuit voltage across the piezoelectric device.This piezoelectric device has an attached cantilever (304SS), which is fixed at one end and free at the other end.In this application, the free end of the cantilever can displace up to a fixed value of displacement (~7.5 mm), as shown in Figure 4a.Due to the displacement strain developed in the piezoelectric device, the voltage shown in Figure 4b is generated.

Performance Evaluation
A subject weighing 60 kg put on our energy harvesting shoes and walked at normal speed for this experiment.Figure 5a shows the open-circuit voltage generated by the PEH, which shows good agreement with numerical study results shown in Figure 4b.Because the PEH is located inside the shoe, it must be able to withstand the weight of the human body; therefore, the durability of the PEH had to be evaluated.Durability testing was carried out using a pushing tester (Figure 5b) to describe the force exerted when the subject walks in the shoes with the PEH inserted under the insole.The same force was applied repetitively to the PEH using the pushing tester.The waveform of the open-circuit voltage was measured for given numbers of bendings (20 k, 40 k, and 60 k times), as shown in Figure 5c.The initial open-circuit voltage of the PEH was 60 V, which dropped to 57.2 V after 60,000 cycles (full compression and release).Thus, the voltage of the PEH dropped by 0.78% every 10,000 cycles.The resistive matching point of the PEH in the shoe was measured.The highest power was measured while increasing the variable resistance; a value of 52 μW was obtained at 280 kΩ (see graph in Figure 5d,e).

Performance Evaluation
A subject weighing 60 kg put on our energy harvesting shoes and walked at normal speed for this experiment.Figure 5a shows the open-circuit voltage generated by the PEH, which shows good agreement with numerical study results shown in Figure 4b.Because the PEH is located inside the shoe, it must be able to withstand the weight of the human body; therefore, the durability of the PEH had to be evaluated.Durability testing was carried out using a pushing tester (Figure 5b) to describe the force exerted when the subject walks in the shoes with the PEH inserted under the insole.The same force was applied repetitively to the PEH using the pushing tester.The waveform of the open-circuit voltage was measured for given numbers of bendings (20 k, 40 k, and 60 k times), as shown in Figure 5c.The initial open-circuit voltage of the PEH was 60 V, which dropped to 57.2 V after 60,000 cycles (full compression and release).Thus, the voltage of the PEH dropped by 0.78% every 10,000 cycles.The resistive matching point of the PEH in the shoe was measured.The highest power was measured while increasing the variable resistance; a value of 52 µW was obtained at 280 kΩ (see graph in Figure 5d,e).

Performance According to Weight
The difference in voltage generated when subjects weighing 60-90 kg walke mal speed with the energy harvesting shoes was measured.In Figure 6a, as th weight increases, it can be seen that the force applied to the PEH inside the shoe magnitude of the voltage) also increases.The maximum voltage is about 22 V f and 90 kg generates a maximum voltage of 34 V (Figure 6b). Figure 6c,d show the in voltage in a capacitor (47 μF, 94 μF) when the PEH is pressed 10 times acco four weights.As the capacity of the capacitor increases, more force is required charged voltage reaches a specific level.Therefore, the capacitor should be se consideration of the operating voltage of the related electronic device and the am energy required to operate it.

Performance According to Weight
The difference in voltage generated when subjects weighing 60-90 kg walked at normal speed with the energy harvesting shoes was measured.In Figure 6a, as the subject weight increases, it can be seen that the force applied to the PEH inside the shoe (and the magnitude of the voltage) also increases.The maximum voltage is about 22 V for 60 kg, and 90 kg generates a maximum voltage of 34 V (Figure 6b). Figure 6c,d show the changes in voltage in a capacitor (47 µF, 94 µF) when the PEH is pressed 10 times according to four weights.As the capacity of the capacitor increases, more force is required until the charged voltage reaches a specific level.Therefore, the capacitor should be selected in consideration of the operating voltage of the related electronic device and the amount of energy required to operate it.

Step-down Converter with a Wireless Transmitter
The energy generated by the PEH is used to power a wireless transmitter.The amount of energy generated with one cycle (compress-release) by the PEH is insufficient to operate the wireless transmitter.Therefore, a specific circuit is required to store enough energy in a capacitor to operate the wireless transmitter, and then transfer power from the capacitor to the wireless transmitter when enough energy has been gathered to operate it.Figure 7 shows a schematic of the wireless communication system consisting of a rectifier, a step-down converter with under-voltage lockout (UVLO) function, and a wireless transmitter (AK-J027, Shenzhen Century Aoke Electronics Co., Ltd., Shenzhen, China).The voltage generated by the piezoelectric device is rectified through a rectifier and the energy generated is accumulated in the capacitor ( .Initially, the UVLO function turns the device into shutdown mode, and no current flows into the load, and energy is continuously charged to  .When the voltage of  rises and reaches the  _ level, the circuit becomes active and the current charged in  flows to the load.When the voltage of  falls below the  _ level, the circuit returns the device to shutdown mode again.In this way, it is possible to periodically operate the wireless transmitter by serially collecting sufficient power.In this circuit, the voltages  _ and  _ were set to 6 and 4 V, respectively, and the output voltage was 3 V.After 24 steps, the capacitor is charged with enough energy to send a signal to the receiver, as shown in Figure 8, and the transmitter run time is 60 ms (Figure 8b).After starting the device once, it is possible to operate the wireless transmitter again after 8 steps.

Application 4.1. Step-down Converter with a Wireless Transmitter
The energy generated by the PEH is used to power a wireless transmitter.The amount of energy generated with one cycle (compress-release) by the PEH is insufficient to operate the wireless transmitter.Therefore, a specific circuit is required to store enough energy in a capacitor to operate the wireless transmitter, and then transfer power from the capacitor to the wireless transmitter when enough energy has been gathered to operate it.Figure 7 shows a schematic of the wireless communication system consisting of a rectifier, a stepdown converter with under-voltage lockout (UVLO) function, and a wireless transmitter (AK-J027, Shenzhen Century Aoke Electronics Co., Ltd., Shenzhen, China).The voltage generated by the piezoelectric device is rectified through a rectifier and the energy generated is accumulated in the capacitor (C i ).Initially, the UVLO function turns the device into shutdown mode, and no current flows into the load, and energy is continuously charged to C i .When the voltage of C i rises and reaches the V (IN_startup) level, the circuit becomes active and the current charged in C i flows to the load.When the voltage of C i falls below the V (IN_stop) level, the circuit returns the device to shutdown mode again.In this way, it is possible to periodically operate the wireless transmitter by serially collecting sufficient power.In this circuit, the voltages V (IN_startup) and V (IN_stop) were set to 6 and 4 V, respectively, and the output voltage was 3 V.After 24 steps, the capacitor is charged with enough energy to send a signal to the receiver, as shown in Figure 8, and the transmitter run time is 60 ms (Figure 8b).After starting the device once, it is possible to operate the wireless transmitter again after 8 steps.

Emergency Monitoring
The transmitter (Figure 9a) and receiver (Figure 9b) of the wireless communication system were used for emergencies.When the user walks, the transmitter periodically sends a signal to a receiver and this signal is used to reset the timer in the receiver.If the reset signal is received before the time set by an administrator, a stable status will be displayed continuously on the screen (Figure 9d), indicating that the user is moving and working in the workplace.On the other hand, if a certain time passes without receiving

Emergency Monitoring
The transmitter (Figure 9a) and receiver (Figure 9b) of the wireless communication system were used for emergencies.When the user walks, the transmitter periodically sends a signal to a receiver and this signal is used to reset the timer in the receiver.If the reset signal is received before the time set by an administrator, a stable status will be displayed continuously on the screen (Figure 9d), indicating that the user is moving and working in the workplace.On the other hand, if a certain time passes without receiving the reset signal from the transmitter, a warning message is displayed on the screen (Figure

Emergency Monitoring
The transmitter (Figure 9a) and receiver (Figure 9b) of the wireless communication system were used for emergencies.When the user walks, the transmitter periodically sends a signal to a receiver and this signal is used to reset the timer in the receiver.If the reset signal is received before the time set by an administrator, a stable status will be displayed continuously on the screen (Figure 9d), indicating that the user is moving and working in the workplace.On the other hand, if a certain time passes without receiving the reset signal from the transmitter, a warning message is displayed on the screen (Figure 9e) to inform the administrator that user movement has stopped.A diagram of the operating sequence of the system is shown in (Figure 9c).9e) to inform the administrator that user movement has stopped.A diagram of the oper ating sequence of the system is shown in (Figure 9c).

Conclusions
Most of the PEH causes a lot of inconvenience to a user due to its volume, so it was not easy to apply to the actual environment.In this paper, we focused on the developmen of the PEH that can be applied to the actual environment.The structure of the PEH was designed using only one spring, and since the PEH has a height of 2 mm (compressed), i does not cause inconvenience to a user even when it is applied to a shoe.In addition to the volume of the PEH, the durability of PZT has to be strengthened.The PZT can be damaged by strong external shocks because it is brittle material, so conductive tape and UV coating were applied to a piezoelectric device to improve its durability.The PEH was evaluated for durability through a pushing tester and the output was reduced by 0.78% after every 10,000 cycles of testing and generated 52 μW with one step.The energy gen erated by the PEH is used to operate a wireless transmitter.The power generated with eight steps is sufficient to drive it.
The PEH is embedded in the sole of a shoe and generates electricity in response to user movements.The electrical energy accumulated is then used to power a wireless com munication system as a self-powered wearable device.If the user continues to move, the wireless transmitter is driven by power generated from the PEH by transmitting a peri odic signal to the receiver in a control center.Conversely, if the user is in an accident, and there is no user movement, the PEH will not generate power or run the wireless transmit ter.If the receiver does not receive a worker's signal for more than a certain period of time it is judged to be a dangerous situation and informs the administrator of the risk.This is a system that is directly related to the safety of at-risk workers, so the scope of its applica tion is endless.

Conclusions
Most of the PEH causes a lot of inconvenience to a user due to its volume, so it was not easy to apply to the actual environment.In this paper, we focused on the development of the PEH that can be applied to the actual environment.The structure of the PEH was designed using only one spring, and since the PEH has a height of 2 mm (compressed), it does not cause inconvenience to a user even when it is applied to a shoe.In addition to the volume of the PEH, the durability of PZT has to be strengthened.The PZT can be damaged by strong external shocks because it is brittle material, so conductive tape and UV coating were applied to a piezoelectric device to improve its durability.The PEH was evaluated for durability through a pushing tester and the output was reduced by 0.78% after every 10,000 cycles of testing and generated 52 µW with one step.The energy generated by the PEH is used to operate a wireless transmitter.The power generated with eight steps is sufficient to drive it.
The PEH is embedded in the sole of a shoe and generates electricity in response to user movements.The electrical energy accumulated is then used to power a wireless communication system as a self-powered wearable device.If the user continues to move, the wireless transmitter is driven by power generated from the PEH by transmitting a periodic signal to the receiver in a control center.Conversely, if the user is in an accident, and there is no user movement, the PEH will not generate power or run the wireless transmitter.If the receiver does not receive a worker's signal for more than a certain period of time, it is judged to be a dangerous situation and informs the administrator of the risk.This is a system that is directly related to the safety of at-risk workers, so the scope of its application is endless.

Figure 1 .
Figure 1.Wireless communication system between worker and control center.

Figure 1 .
Figure 1.Wireless communication system between worker and control center.

Figure 2 .
Figure 2. (a) Piezoelectric device with a crack, (b) Piezoelectric device with conductive tape and ultraviolet coating, (c) Layers constituting a piezoelectric device and a perovskite PZT unit cell, (d) Direction (polarity) of the voltage formed by default state (i), compression (ii) and release (iii).

Figure 2 .
Figure 2. (a) Piezoelectric device with a crack, (b) Piezoelectric device with conductive tape and ultraviolet coating, (c) Layers constituting a piezoelectric device and a perovskite PZT unit cell, (d) Direction (polarity) of the voltage formed by default state (i), compression (ii) and release (iii).

Figure 3 .
Figure 3. (a) Schematic and (b) Real image of the PEH, (c) Energy harvesting shoe with PEH.

Figure 3 .
Figure 3. (a) Schematic and (b) Real image of the PEH, (c) Energy harvesting shoe with PEH.

Figure 4 .
Figure 4. (a) Total displacement of the piezoelectric device in millimeters, (b) Open-circuit voltage across the piezoelectric device.

Figure 4 .
Figure 4. (a) Total displacement of the piezoelectric device in millimeters, (b) Open-circuit voltage across the piezoelectric device.

Figure 5 .
Figure 5. (a) Open-circuit voltage, (b) Number of cycles with the pushing tester, (c) Exp setup, (d) block diagram of measurement system, (e) Graph of voltage, current, and pow ing to the load resistance.

Figure 5 .
Figure 5. (a) Open-circuit voltage, (b) Number of cycles with the pushing tester, (c) Experimental setup, (d) block diagram of measurement system, (e) Graph of voltage, current, and power according to the load resistance.

Figure 6 .
Figure 6.(a) Open-circuit voltage waveform and (b) Maximum voltage according to the weight of the object, (c) Charged voltage with a capacitor with 47 μF and (d) With 94 μF.

Figure 6 .
Figure 6.(a) Open-circuit voltage waveform and (b) Maximum voltage according to the weight of the object, (c) Charged voltage with a capacitor with 47 µF and (d) With 94 µF.

Figure 7 .
Figure 7. Schematic of the wireless communication circuit with a step-down converter.

Figure 8 .
Figure 8.(a) Charged voltage in the capacitor and output voltage, (b) Time needed to transfer a signal.

Figure 7 . 12 Figure 7 .
Figure 7. Schematic of the wireless communication circuit with a step-down converter.

Figure 8 .
Figure 8.(a) Charged voltage in the capacitor and output voltage, (b) Time needed to transfer a signal.

Figure 8 .
Figure 8.(a) Charged voltage in the capacitor and output voltage, (b) Time needed to transfer a signal.

Figure 9 .
Figure 9. (a) Transmitter, (b) Receiver of the wireless communication system, (c) Diagram of the operating algorithm of the wireless communication system.LCD screen with (d) Stable and (e Warning conditions.

Figure 9 .
Figure 9. (a) Transmitter, (b) Receiver of the wireless communication system, (c) Diagram of the operating algorithm of the wireless communication system.LCD screen with (d) Stable and (e) Warning conditions.

Table 1 .
Material and component properties.

Table 1 .
Material and component properties.