Self-Oscillating Boost Converter of Wiegand Pulse Voltage for Self-Powered Modules

This paper introduces a new method of electricity generation using a Wiegand sensor. The Wiegand sensor consists of a magnetic wire and a pickup coil wound around it. This sensor generates a pulse voltage of approximately 5 V and 20 µs width as an induced voltage in the pickup coil. The aim of this study is to generate a DC voltage of 5 V from the sensor, which is expected to be used as a power source in self-powered devices and battery-less modules. We report on the design and verification of a self-oscillating boost converter circuit in this paper. A DC voltage obtained by rectifying and smoothing the pulse voltage generated from the Wiegand sensor was boosted by the circuit. A stable DC output voltage in the order of 5 V for use as a power supply in electronics modules was successfully obtained. A quantitative analysis of the power generated by the Wiegand sensor revealed a suitable voltage-current range for application in self-powered devices and battery-less modules.


Introduction
In the Internet of Things (IoT) society, electronic devices and modules can be connected to the internet and exchange information through various sensors [1]. These are generally called IoT devices. The number of IoT devices is increasing rapidly and is expected to reach 80-120 billion by 2025 [2]. A significant number of batteries that need expensive and time-consuming maintenance are required for these devices, which also cause environmental pollution. Energy harvesting, such as collecting small amounts of energy from the surroundings and converting them into electrical energy, is expected to solve this problem [3,4]. Energy from the surrounding environment, if available, can continuously supply electrical power, and thus, be used as an independent power source for long periods of time, without replacing the power harness and battery. With developments in miniaturization and energy-saving approaches, low-power power supplies can gradually satisfy the many requirements of IoT devices [5]. This research introduces the use of a self-oscillating boost converter circuit for electricity generation using a Wiegand sensor [6,7] as an energy-harvesting element.
The Wiegand sensor generates pulse voltages that do not depend on the frequency of the external magnetic field [8]. These pulse voltages are generated with a constant intensity, even under ultra-slow changes in the magnetic field. Therefore, the Wiegand sensor has attracted significant attention as a power supply for the battery-less operation of electronic devices and for energy harvesting [9]. The contribution of this research involves the development of a DC power supply for electronic devices and modules using the Wiegand sensor. It is essential to build a DC power supply of 5 V because it can be used for multiple IoT devices. The power generated by the Wiegand sensor is in the order of 1 mW, even when the frequency of the applied magnetic field is as low as 1 kHz [8]. In this study, we designed and verified a self-oscillating boost converter circuit [10][11][12] connected to the Wiegand sensor as a power generator. DC power generation of 5 V was realized using the Wiegand sensor; this may not be achievable using other methods under an excitation frequency of 1 kHz.
The remainder of this paper is organized as follows: Following the introduction of the Wiegand sensor and its pulse generation in Section 2, the circuits for DC conversion of the pulse voltage and the self-oscillating boost converter are presented in Section 3. In Section 4, we present the circuit properties of the self-oscillating boost converter connected to the Wiegand sensor, derived both experimentally and through simulations. Finally, the conclusions of this study are presented in Section 5.

Measurement of Pulse Voltage from the Wiegand Sensor
We used a magnet wire composed of iron-cobalt-vanadium (FeCoV) with a diameter of 0.25 mm and a length of 11 mm. The Wiegand sensor used in this study consisted of a wire and a pickup coil with 3000 turns wound around it. The magnetic properties of this wire are essentially the same as those we have previously reported in detail [13]. Its magnetic structure is shown in Figure 1. The outer layer and inner core exhibit soft and hard magnetic properties with lower (1.6 kA/m) and higher (6.4 kA/m) coercive forces, respectively. The direction of magnetization of these layers can be either in parallel or antiparallel configurations, as shown in Figure 1-a specific feature of the Wiegand wire.
Energies 2021, 14, 5373 2 of 1 multiple IoT devices. The power generated by the Wiegand sensor is in the order of 1 mW even when the frequency of the applied magnetic field is as low as 1 kHz [8]. In this study we designed and verified a self-oscillating boost converter circuit [10][11][12] connected to th Wiegand sensor as a power generator. DC power generation of 5 V was realized using th Wiegand sensor; this may not be achievable using other methods under an excitation fre quency of 1 kHz. The remainder of this paper is organized as follows: Following the introduction o the Wiegand sensor and its pulse generation in Section 2, the circuits for DC conversion of the pulse voltage and the self-oscillating boost converter are presented in Section 3. In Section 4, we present the circuit properties of the self-oscillating boost converter connected to the Wiegand sensor, derived both experimentally and through simulations. Finally, th conclusions of this study are presented in Section 5.

Measurement of Pulse Voltage from the Wiegand Sensor
We used a magnet wire composed of iron-cobalt-vanadium (FeCoV) with a diamete of 0.25 mm and a length of 11 mm. The Wiegand sensor used in this study consisted of wire and a pickup coil with 3000 turns wound around it. The magnetic properties of thi wire are essentially the same as those we have previously reported in detail [13]. Its mag netic structure is shown in Figure 1. The outer layer and inner core exhibit soft and hard magnetic properties with lower (1.6 kA/m) and higher (6.4 kA/m) coercive forces, respec tively. The direction of magnetization of these layers can be either in parallel or antiparal lel configurations, as shown in Figure 1-a specific feature of the Wiegand wire. When a magnetic field exceeds the coercive force of the soft layer, the latter exhibit a fast magnetization reversal, which is called the Wiegand effect [6]. A pulse voltage i induced in the pickup coil wound around the wire [8,14]. The Wiegand sensor consists o a Wiegand wire and a pickup coil. As fast magnetization reversal is initiated inde pendently from the changing ratio of the applied magnetic field, the intensity and width of the pulse are constant [15]. Figure 2 shows the measured waveform of the pulse voltag generated from the Wiegand sensor. We measured the waveform of the open-circuit volt age across both ends of the pickup coil using an oscilloscope [8,9]. The intensity and fre quency of the alternating applied magnetic field were 3.2 kA/m and 1 kHz, respectively An excitation coil with 25 mm length, 22 mm diameter, and 90 turns was used. An When a magnetic field exceeds the coercive force of the soft layer, the latter exhibits a fast magnetization reversal, which is called the Wiegand effect [6]. A pulse voltage is induced in the pickup coil wound around the wire [8,14]. The Wiegand sensor consists of a Wiegand wire and a pickup coil. As fast magnetization reversal is initiated independently from the changing ratio of the applied magnetic field, the intensity and width of the pulse are constant [15]. Figure 2 shows the measured waveform of the pulse voltage generated from the Wiegand sensor. We measured the waveform of the open-circuit voltage across both ends of the pickup coil using an oscilloscope [8,9]. The intensity and frequency of the alternating applied magnetic field were 3.2 kA/m and 1 kHz, respectively. An excitation coil with 25 mm length, 22 mm diameter, and 90 turns was used. An alternating magnetic field was applied to the Wiegand sensor by using the excitation coil, a signal generator, and a bipolar amplifier. Positive and negative pulses with widths of 20 µs were alternatingly induced in the pickup within 1 ms. These were attributed to electromagnetic induction caused by the change in magnetic flux corresponding to the alternating magnetization reversal of the soft layer. ergies 2021, 14,5373 alternating magnetic field was applied to the Wiegand sensor by usin a signal generator, and a bipolar amplifier. Positive and negative puls µs were alternatingly induced in the pickup within 1 ms. These wer tromagnetic induction caused by the change in magnetic flux corresp nating magnetization reversal of the soft layer.

Pulse Voltage from the Wiegand Sensor Used as a Voltage Source in Sim
As previously reported, we can determine the equivalent circui gand sensor [16]. The intrinsic pulse voltage, Vin, of the Wiegand se evaluate the application circuits of the Wiegand sensor through M simulations. Figure 3 shows the waveform of the intrinsic pulse vo from the Wiegand sensor. The performances of the simulated and e were in agreement when employing the equivalent circuit model of t which consisted of Vin as a voltage source, an internal resistance of 18 ance of 17 mH [16].

Pulse Voltage from the Wiegand Sensor Used as a Voltage Source in Simulation
As previously reported, we can determine the equivalent circuit model of the Wiegand sensor [16]. The intrinsic pulse voltage, V in , of the Wiegand sensor was defined to evaluate the application circuits of the Wiegand sensor through MATLAB ® /Simulink ® simulations. Figure 3 shows the waveform of the intrinsic pulse voltage, V in , generated from the Wiegand sensor. The performances of the simulated and experimental circuits were in agreement when employing the equivalent circuit model of the Wiegand sensor, which consisted of V in as a voltage source, an internal resistance of 180 Ω, and an inductance of 17 mH [16]. a signal generator, and a bipolar amplifier. Positive and negative puls µs were alternatingly induced in the pickup within 1 ms. These wer tromagnetic induction caused by the change in magnetic flux corresp nating magnetization reversal of the soft layer.

Pulse Voltage from the Wiegand Sensor Used as a Voltage Source in Si
As previously reported, we can determine the equivalent circu gand sensor [16]. The intrinsic pulse voltage, Vin, of the Wiegand se evaluate the application circuits of the Wiegand sensor through M simulations. Figure 3 shows the waveform of the intrinsic pulse vo from the Wiegand sensor. The performances of the simulated and e were in agreement when employing the equivalent circuit model of which consisted of Vin as a voltage source, an internal resistance of 18 ance of 17 mH [16].

DC Conversion of Wiegand Pulse Voltage
AC-DC conversion is used to obtain a DC voltage from the Wiegand pulse voltage, as shown in Figure 4. The alternatingly positive and negative pulse voltages are rectified by the rectifier circuit using diodes. A smoothing filter circuit using a capacitor converts the pulse voltages to DC. Figure 5 shows the DC conversion circuit, diode parameters, capacitor, and resistor used in our experiments and simulations. D 1 -D 4 , indicated in Figure 5, represent the diodes (RBR3MM30A) for rectification. R Load is a 5.5 MΩ load resister. C 1 was used as a smoothing capacitor in the range of 1-220 nF to analyze a processed and constant DC voltage. C 1 = 1, 10, 20, 50, 100, or 220 nF was connected to the full-wave bridge rectifier, and waveforms of the output voltage, V out , were measured. Figure 6a shows that V out saturates at 2.77 V, regardless of the capacitance of C 1 . The relaxation time of the saturation is longer for a smaller C 1 . Figure 6b shows the simulated waveforms of the output voltage, which agree with the experimental results. LTspice ® was used for the circuit simulation [16]. waveforms of the output voltage, Vout, were measured. Figure 6a shows that Vout saturates at 2.77 V, regardless of the capacitance of C1. The relaxation time of the saturation is longer for a smaller C1. Figure 6b shows the simulated waveforms of the output voltage, which agree with the experimental results. LTspice ® was used for the circuit simulation [16].  The frequency of the ripple was 2 kHz, i.e., twice the excitation frequency, because of the full-wave rectifier. The output voltage ripple is high for C1 ≤ 20 nF, and it is very low for C1 > 20 nF. The ripple rate, Ripple, was calculated using the following equation:

%
(1)  waveforms of the output voltage, Vout, were measured. Figure 6a shows that Vout saturates at 2.77 V, regardless of the capacitance of C1. The relaxation time of the saturation is longer for a smaller C1. Figure 6b shows the simulated waveforms of the output voltage, which agree with the experimental results. LTspice ® was used for the circuit simulation [16].  The frequency of the ripple was 2 kHz, i.e., twice the excitation frequency, because of the full-wave rectifier. The output voltage ripple is high for C1 ≤ 20 nF, and it is very low for C1 > 20 nF. The ripple rate, Ripple, was calculated using the following equation:

%
(1) waveforms of the output voltage, Vout, were measured. Figure 6a shows that Vout saturates at 2.77 V, regardless of the capacitance of C1. The relaxation time of the saturation is longer for a smaller C1. Figure 6b shows the simulated waveforms of the output voltage, which agree with the experimental results. LTspice ® was used for the circuit simulation [16].  The frequency of the ripple was 2 kHz, i.e., twice the excitation frequency, because of the full-wave rectifier. The output voltage ripple is high for C1 ≤ 20 nF, and it is very low for C1 > 20 nF. The ripple rate, Ripple, was calculated using the following equation: where Vmax, Vmin, and Vaverage are the maximum, minimum, and average voltages, respec- The frequency of the ripple was 2 kHz, i.e., twice the excitation frequency, because of the full-wave rectifier. The output voltage ripple is high for C 1 ≤ 20 nF, and it is very low for C 1 > 20 nF. The ripple rate, Ripple, was calculated using the following equation: where V max , V min , and V average are the maximum, minimum, and average voltages, respectively, applied for 1 ms during one cycle of excitation. The ripple rates calculated from the experimental and simulated output voltages are shown in Figure 7.

Self-Oscillating Boost Converter Circuit
As mentioned in Section 2.2, the maximum voltage obtained at the smoothin itor after DC conversion of the Wiegand pulse voltage is 2.77 V. It is fundamental t a DC voltage of 5 V for operating several electronics modules. In this study, we self-oscillating boost converter circuit for a Wiegand pulse voltage. The featur booster converter is that the energy stored in an inductor increases the output which then exceeds the input voltage. Figure 8 shows the typical circuit of a bo verter. The alternating sequence of storing energy in the inductor and transmittin to the circuit boosts the voltage. The energy is stored in inductor L when M, a fie transistor (FET), is in the ON state, whereas the stored energy is transferred fr capacitor C when M is in the OFF state. As a result, Vout higher than Vin is obtaine erally, the switching ON/OFF of M, controlled by an external signal, is used to ap alternating sequence [10]. As this study aims to develop self-powered electronic m the external signal for an alternating sequence cannot be used. Therefore, a self-os boost converter is employed. Figure 9 shows the self-oscillating boost converte used in this study for a Wiegand pulse voltage. The input voltage, Vin, of a 20pulse used as the power source generates an oscillating voltage at VC1. The frequ these oscillations corresponds to a resonant frequency determined by the inducto capacitors C1 and Cgs [11,12]. This oscillation voltage at VC1 switches the consecu and OFF states of M, as shown in Figure 9.

Self-Oscillating Boost Converter Circuit
As mentioned in Section 2.2, the maximum voltage obtained at the smoothing capacitor after DC conversion of the Wiegand pulse voltage is 2.77 V. It is fundamental to obtain a DC voltage of 5 V for operating several electronics modules. In this study, we apply a selfoscillating boost converter circuit for a Wiegand pulse voltage. The feature of the booster converter is that the energy stored in an inductor increases the output voltage, which then exceeds the input voltage. Figure 8 shows the typical circuit of a boost converter. The alternating sequence of storing energy in the inductor and transmitting it back to the circuit boosts the voltage. The energy is stored in inductor L when M, a field-effect transistor (FET), is in the ON state, whereas the stored energy is transferred from L to capacitor C when M is in the OFF state. As a result, V out higher than V in is obtained. Generally, the switching ON/OFF of M, controlled by an external signal, is used to apply this alternating sequence [10]. As this study aims to develop self-powered electronic modules, the external signal for an alternating sequence cannot be used. Therefore, a self-oscillating boost converter is employed. Figure 9 shows the self-oscillating boost converter circuit used in this study for a Wiegand pulse voltage. The input voltage, V in , of a 20-µs-wide pulse used as the power source generates an oscillating voltage at V C1 . The frequency of these oscillations corresponds to a resonant frequency determined by the inductor L and capacitors C 1 and C gs [11,12]. This oscillation voltage at V C1 switches the consecutive ON and OFF states of M, as shown in Figure 9. When the oscillating pulse voltage at VC1 is below Vth, the FET is tur energy stored in L during the FET is transmitted to the capacitor of t through diode D. D prevents a backflow current to L. By repeating the ON/OFF switchin the FET, a DC output voltage exceeding Vin is obtained.

Design of a Self-Oscillating Boost Converter for Wiegand Pulse
In this study, we designed and fabricated a rectifying and boosting circuit for gand pulse voltage in Figure 10. The circuit consists of a bridge rectifier with dio self-oscillating boost converter components, such as inductors, capacitors, n-chan and diodes, as described in the previous section and in Figures 8 and 9. Details o rameters of the circuit elements are indicated in Figure 10 and Table 1. The input v supplied from a Wiegand sensor. An alternating magnetic field of 3.2 kA/m was ap the wire. The frequency of this field was 1 kHz. The Wiegand sensor is advanta terms of its efficient power generation at low frequency ranges below 1 kHz [8]. D prevents a backflow current to L. By repeating the ON/OFF switching sequence of the FET, a DC output voltage exceeding V in is obtained.

Design of a Self-Oscillating Boost Converter for Wiegand Pulse
In this study, we designed and fabricated a rectifying and boosting circuit for the Wiegand pulse voltage in Figure 10. The circuit consists of a bridge rectifier with diodes and self-oscillating boost converter components, such as inductors, capacitors, n-channel FET, and diodes, as described in the previous section and in Figures 8 and 9. Details of the parameters of the circuit elements are indicated in Figure 10 and Table 1. The input voltage is supplied from a Wiegand sensor. An alternating magnetic field of 3.2 kA/m was applied to the wire. The frequency of this field was 1 kHz. The Wiegand sensor is advantageous in terms of its efficient power generation at low frequency ranges below 1 kHz [8].
In this study, we designed and fabricated a rectifying and boosting circuit for the Wiegand pulse voltage in Figure 10. The circuit consists of a bridge rectifier with diodes and self-oscillating boost converter components, such as inductors, capacitors, n-channel FET, and diodes, as described in the previous section and in Figures 8 and 9. Details of the parameters of the circuit elements are indicated in Figure 10 and Table 1. The input voltage is supplied from a Wiegand sensor. An alternating magnetic field of 3.2 kA/m was applied to the wire. The frequency of this field was 1 kHz. The Wiegand sensor is advantageous in terms of its efficient power generation at low frequency ranges below 1 kHz [8].

Component Value/Type (Model Name)
Capacitance: C 1 20 nF Capacitance: C 2 60 nF Inductance: L 1 4.5 mH Resistance: R 4 800 Ω Diode: D 1 -D 5 low V F , Schottky (RBR3MM30A) MOSFET: M 1 n-channel (RE1C002UN) Resistance: R LOAD 1 kΩ-5 MΩ Figure 11 shows the simulated waveforms of the voltages and currents in the selfoscillating boost converter. The rectified voltage of the Wiegand pulse is oscillated by a resonance of C 1 and L 1 . This oscillated voltage, V C1 , switches the FET ON/OFF. V ds confirms the ON/OFF status of the FET. As a result of the oscillated I L1 and I D5 and the smoothing capacitor C 2 , a constant DC voltage is obtained as the output. V out is 5.1 V, which is higher than the input voltage of V C1 , and a DC voltage of 2.77 V is obtained without the booster circuit, as shown in Figure 6.  Figure 11 shows the simulated waveforms of the voltages and currents in the selfoscillating boost converter. The rectified voltage of the Wiegand pulse is oscillated by a resonance of C1 and L1. This oscillated voltage, VC1, switches the FET ON/OFF. Vds confirms the ON/OFF status of the FET. As a result of the oscillated IL1 and ID5 and the smoothing capacitor C2, a constant DC voltage is obtained as the output. Vout is 5.1 V, which is higher than the input voltage of VC1, and a DC voltage of 2.77 V is obtained without the booster circuit, as shown in Figure 6. Vout depends on the circuit parameters of L1 and C1, as shown in Figure 12. Vout increases as C1 decreases. The combination of L1 = 4.5 mH and C1 = 20 nF is optimum for producing a DC voltage of approximately 5.1 V, thus meeting the aim of this study to generate a DC voltage of 5 V that can be used as a power source for various electronic modules. The dependency of the output voltage ripple on capacitor C2 was also studied. As shown in Figure 13, Vout is not dependent on C2, and is stable with fewer ripples when V out depends on the circuit parameters of L 1 and C 1 , as shown in Figure 12. V out increases as C 1 decreases. The combination of L 1 = 4.5 mH and C 1 = 20 nF is optimum for producing a DC voltage of approximately 5.1 V, thus meeting the aim of this study to generate a DC voltage of 5 V that can be used as a power source for various electronic modules. The dependency of the output voltage ripple on capacitor C 2 was also studied. As shown in Figure 13, V out is not dependent on C 2 , and is stable with fewer ripples when C 2 > 60 nF. Figure 11. Simulated waveforms of voltages and currents in the self-oscillating boost conv Vout depends on the circuit parameters of L1 and C1, as shown in Figure 12 creases as C1 decreases. The combination of L1 = 4.5 mH and C1 = 20 nF is optim producing a DC voltage of approximately 5.1 V, thus meeting the aim of this generate a DC voltage of 5 V that can be used as a power source for various e modules. The dependency of the output voltage ripple on capacitor C2 was also As shown in Figure 13, Vout is not dependent on C2, and is stable with fewer rippl C2 > 60 nF.   Figure 14 shows the experimental and simulated waveforms for the output a voltages of the self-oscillating boost converter circuit presented in Figure 10 and We measured the waveforms of voltages at Vout, Vds, and VC1, as indicated in th diagram in Figure 10, by using an oscilloscope. Since the applied field frequenc kHz, the full-time scale of 0.5 ms in Figure 14 corresponds to one cycle of the ge Wiegand pulse. The observed oscillations of Vds, VC1, and Vout agreed with the corr ing simulated values. Figure 13. Dependence of the output voltage, V out , on parameter C 2 and its ripple rate. Figure 14 shows the experimental and simulated waveforms for the output and other voltages of the self-oscillating boost converter circuit presented in Figure 10 and Table 1. We measured the waveforms of voltages at V out , V ds , and V C1 , as indicated in the circuit diagram in Figure 10, by using an oscilloscope. Since the applied field frequency was 1 kHz, the full-time scale of 0.5 ms in Figure 14 corresponds to one cycle of the generated Wiegand pulse. The observed oscillations of V ds , V C1 , and V out agreed with the corresponding simulated values. We measured the waveforms of voltages at Vout, Vds, and VC1, as indicated in the circuit diagram in Figure 10, by using an oscilloscope. Since the applied field frequency was 1 kHz, the full-time scale of 0.5 ms in Figure 14 corresponds to one cycle of the generated Wiegand pulse. The observed oscillations of Vds, VC1, and Vout agreed with the corresponding simulated values.  Figure 15 shows the time dependency of Vout. The simulated and observed saturated voltages are almost equivalent. We have discussed the experimental and simulated results of the circuit shown in Figure 10. The load resistance RLoad = 5 MΩ was used, corresponding to an almost "open circuit condition" for the output. Figure 16 shows the dependence of Iout and Vout on the load resistance RLoad. Vout decreases as RLoad increases. Figure 12 shows that Vout changes with C1, reaching 5 V on adjusting C1. However, the ripple of Vout degrades at C1 < 10 nF. Figure 14. Waveforms of V out , V ds , and V C1 in the self-oscillating boost converter. Figure 15 shows the time dependency of V out . The simulated and observed saturated voltages are almost equivalent. We have discussed the experimental and simulated results of the circuit shown in Figure 10. The load resistance R Load = 5 MΩ was used, corresponding to an almost "open circuit condition" for the output. Figure 16 shows the dependence of I out and V out on the load resistance R Load . V out decreases as R Load increases. Figure 12 shows that V out changes with C 1 , reaching 5 V on adjusting C 1 . However, the ripple of V out degrades at C 1 < 10 nF.      Figure 17 shows the electric power Pout utilized at RLoad. A maximum power of 63 µW was experimentally obtained at RLoad = 10 kΩ, which does not match with the resistance of the pickup coil, such as 180 Ω for the Wiegand sensor [9]. This mismatch is attributed to the elements and operation of the self-oscillating boost circuit. In fact, we have reported that the  Figure 17 shows the electric power P out utilized at R Load . A maximum power of 63 µW was experimentally obtained at R Load = 10 kΩ, which does not match with the resistance of the pickup coil, such as 180 Ω for the Wiegand sensor [9]. This mismatch is attributed to the elements and operation of the self-oscillating boost circuit. In fact, we have reported that the maximum power was obtained at a load resistance of 2 kΩ, higher than the DC coil resistance for the Wiegand sensor connected with rectifying and smoothing circuits [8]. Figure 16. Dependence of simulated and measured Vout and Iout on load resistance, Figure 17 shows the electric power Pout utilized at RLoad. A maximum po was experimentally obtained at RLoad = 10 kΩ, which does not match with th the pickup coil, such as 180 Ω for the Wiegand sensor [9]. This mismatch is a elements and operation of the self-oscillating boost circuit. In fact, we have re maximum power was obtained at a load resistance of 2 kΩ, higher than t sistance for the Wiegand sensor connected with rectifying and smoothing cir In this study, an alternating magnetic field is externally applied to the sor as excitation energy, leading to the generation of the Wiegand pulse v tractive feature of the Wiegand sensor is that the generated pulse voltage i of the frequency of the applied alternating magnetic field. Figure 18 shows In this study, an alternating magnetic field is externally applied to the Wiegand sensor as excitation energy, leading to the generation of the Wiegand pulse voltage. An attractive feature of the Wiegand sensor is that the generated pulse voltage is independent of the frequency of the applied alternating magnetic field. Figure 18 shows the measured V out and its ripple rate function under an excitation frequency of 1 kHz and lower; V out decreases with the frequency. However, V out of approximately 5 V and a low ripple rate are obtained at a frequency range of up to 0.6 kHz. When the frequency is 0.4 kHz, the output voltage still reaches 3.3 V with a ripple rate lower than 5%. This result indicates that the selfoscillating boost converter can be used in practical applications as a power source for electronic modules. ergies 2021, 14,5373 Vout and its ripple rate function under an excitation frequency of 1 decreases with the frequency. However, Vout of approximately 5 V a are obtained at a frequency range of up to 0.6 kHz. When the frequ output voltage still reaches 3.3 V with a ripple rate lower than 5%. that the self-oscillating boost converter can be used in practical app source for electronic modules.  Figure 19 summarizes the relationship between Vout and Iout, obta gand sensor with a self-oscillating boost converter. It shows the voltag Figure 18. Dependence of measured V out on the frequency and its ripple rate. Figure 19 summarizes the relationship between V out and I out , obtained using the Wiegand sensor with a self-oscillating boost converter. It shows the voltage and current range functions for the load resistance used for practical application as a power source. A stable output of 5 V is maintained for currents up to 1 µA. This voltage/current range is used in low-energy IoT devices [17]. Furthermore, it is compatible with the existing energy-harvesting IC, such as power-storing buck DC-DC converters used for photovoltaic and vibration power generation elements [18]. Typically, a DC-DC converter is used in combination with storage batteries to ensure high efficiency and a maximized current supply in the order of 1 mA [19]. Therefore, the developed circuit system with the Wiegand sensor can be used with a storage battery; it allows for a higher capability of current consumption and can be used as a power supply for IoT devices. Figure 18. Dependence of measured Vout on the frequency and its ripple rate. Figure 19 summarizes the relationship between Vout and Iout, obtained u gand sensor with a self-oscillating boost converter. It shows the voltage and functions for the load resistance used for practical application as a power so output of 5 V is maintained for currents up to 1 µA. This voltage/current ra low-energy IoT devices [17]. Furthermore, it is compatible with the existin vesting IC, such as power-storing buck DC-DC converters used for photov bration power generation elements [18]. Typically, a DC-DC converter is u nation with storage batteries to ensure high efficiency and a maximized cur the order of 1 mA [19]. Therefore, the developed circuit system with the W can be used with a storage battery; it allows for a higher capability of current and can be used as a power supply for IoT devices.

Conclusions
We designed a self-oscillating boost converter circuit connected to the sor. The Wiegand sensor consists of an FeCoV magnetic wire with a diamet length of 11 mm, and pickup coil with 3000 turns wound around the wire. wire, i.e., the Wiegand wire, generates a peak pulse voltage of 4.62 V and during the magnetization reversal of its outer layer under a lower coercive f nating magnetic field of 3.2 kA/m at 1 kHz was applied to the Wiegan

μW
Unstable DC voltage Figure 19. Mapping of V out -I out for practical applications of the Wiegand sensor with a self-oscillating boost converter.

Conclusions
We designed a self-oscillating boost converter circuit connected to the Wiegand sensor. The Wiegand sensor consists of an FeCoV magnetic wire with a diameter of 0.25 mm, length of 11 mm, and pickup coil with 3000 turns wound around the wire. This magnetic wire, i.e., the Wiegand wire, generates a peak pulse voltage of 4.62 V and 20 µs width during the magnetization reversal of its outer layer under a lower coercive field. An alternating magnetic field of 3.2 kA/m at 1 kHz was applied to the Wiegand sensor and alternating positive and negative pulse voltages were induced in the pickup coil. A DC voltage of 2.77 V was obtained by a bridge rectifier and a smoothing capacitor connected to the Wiegand sensor. This DC voltage could be intensified to approximately 5 V through a self-oscillating boost converter circuit. The experimental results of the voltage/current and ripple characteristics agreed with the simulation results. This study represents a significant development pertaining to the use of the Wiegand sensor as a power source for battery-less devices and modules.