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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Research on Vibration Piezoelectric Generator Energy Acquisition Method of</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Yi Cao</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Shuangjie Liu</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Yongping Hao</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Kai Ma</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>School of Equipment Engineering, Shenyang Ligong University</institution>
          ,
          <addr-line>Shenyang, Liaoning</addr-line>
          ,
          <country country="CN">China</country>
        </aff>
      </contrib-group>
      <fpage>79</fpage>
      <lpage>84</lpage>
      <abstract>
        <p>With the modern weapon system to fuze reliability, security, versatility and storage life and other technical requirements are becoming higher and higher, the traditional chemical battery power supply mode can not meet the requirements of modern weapon fuze power supply. In order to meet the power supply needs of modern fuze, based on the analysis of the electrical characteristics of piezoelectric materials, the vibration energy acquisition method of the fuze piezoelectric generator is studied, and the energy acquisition method of the fuze piezoelectric generator is optimized, so as to achieve the purpose of efficiently collecting the output energy of the piezoelectric generator. The research method in this paper provides a theoretical reference for the research of vibration and piezoelectric energy acquisition technology of piezoelectric generator, and provides a reference for the further research and design of vibration energy acquisition technology.</p>
      </abstract>
      <kwd-group>
        <kwd>1 Piezoelectric vibration energy</kwd>
        <kwd>Energy collection</kwd>
        <kwd>Power management</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        Vibration energy is a common energy of natural environment, which is widely used in military
facilities, industrial equipment, human movement and biological activities. Piezoelectric vibration
power generation devices are widely used in vibration energy capture because of their advantages such
as simple structure, flexible shape, high energy density and easy miniaturization[
        <xref ref-type="bibr" rid="ref1 ref2">1-2</xref>
        ].Because of its
advantages of simple structure, flexible shape, high energy density and easy to realize miniaturization,
piezoelectric vibration generator is widely used in vibration energy capture. However, due to the high
capacitive impedance of piezoelectric materials, the output power of the generator has the
characteristics of low current and high voltage, and its output power is related to the load. At the same
time, because of the characteristics of vibration energy, the output of the piezoelectric generator is AC
electric energy, and can not directly charge the battery or power the fuze load equipment. Therefore, a
power collecting circuit must be added between the piezoelectric generator and the fuze load equipment,
whose function is to realize AC - DC conversion and improve the output power of the piezoelectric
generator[
        <xref ref-type="bibr" rid="ref3">3</xref>
        ].
      </p>
    </sec>
    <sec id="sec-2">
      <title>2. DC - AC rectifier circuit</title>
      <p>Due to the characteristics of vibration energy, the output is AC electric energy, which can not directly
charge the battery or power the load. Therefore, AC/DC rectifier circuit should be added between
piezoelectric material and load to collect electric energy.
material is the standard sinusoidal oscillation excitation, defined as</p>
      <p>It is assumed that the electric energy excitation generated by the vibration F of the piezoelectric
In Equation（1），V0 is voltage amplitude and ω is vibration frequency. According to Kirchhoff's
law and the piezoelectric equation, the voltage on the load resistance R0 can be obtained as follows:
 ( ) =  0sin⁡( )
piezoelectric material, R0 is load resistance, RD is rectifier diode loss resistance, CP is internal static
capacitance of piezoelectric material. Then, the average power on the load resistor is:
[( 0 + 2  )   + 2
 2
]</p>
      <p>Because of the simple structure of standard energy collection circuit, its application field is very
wide, but the circuit has the problems of low collection efficiency and high energy loss, and there are</p>
    </sec>
    <sec id="sec-3">
      <title>2.1. Standard energy harvesting circuit</title>
      <p>classical full-bridge rectifier circuit. The entire circuit consists of four diodes, with R0 representing the
load.
many places to be improved.
2.2.</p>
    </sec>
    <sec id="sec-4">
      <title>MOSFET energy collection circuit</title>
      <p>In order to eliminate the problem of high starting voltage and high power consumption caused by a
large diode voltage drop, the power MOSFET is used to replace the rectifier and form an active rectifier
circuit. The voltage drop of MOSFET is close to zero, and it has approximately the circuit characteristics
of ideal diode. Therefore, the power loss and starting voltage of the rectifier circuit can be reduced, and
the energy collection efficiency can be improved.</p>
      <p>MN1 and MP2 are on, and MN2 and MP1 are off.</p>
      <p>
        As shown in Figure 2, the voltage comparator is used to cross-couple NMOS and PMOS[
        <xref ref-type="bibr" rid="ref4">4</xref>
        ], so that
the MOSFET can work in the amplification area, so that it can be completely closed, and improve the
energy collection efficiency. The principle is that when the output voltage of piezoelectric material is
in a positive half period, because⁡ 
−  1 &gt; |
      </p>
      <sec id="sec-4-1">
        <title>1|, At this point, MP1 and MN2 are on, and MP2 and</title>
        <p>MN1 are off. At the end of CP discharge, when V1=V2, all MOSFET cut off. Similarly, when the output
voltage of piezoelectric material is in negative half period, due to  
−  2 &gt; |</p>
      </sec>
      <sec id="sec-4-2">
        <title>2|, At this point,</title>
      </sec>
    </sec>
    <sec id="sec-5">
      <title>3. Passive power factor correction circuit</title>
      <p>
        After the electric energy output by piezoelectric material passes the rectifier circuit, its voltage
waveform is close to the DC circuit, and the current produces distortion and distortion because the
conduction time of the rectifier tube is too short, which becomes a spike pulse and reduces the power
factor. The passive power factor correction method is to make the input current of the circuit close to
sine wave by adding passive components such as capacitance and inductance into the circuit, that is, to
improve the power factor through reactive power compensation, so as to achieve the purpose of
increasing active power[
        <xref ref-type="bibr" rid="ref5">5</xref>
        ]. Compared with other circuits, grain filling circuit needs fewer components
and has better performance. The grain filling circuit is shown in Figure 3.
the capacitor is in parallel, and the voltage at both ends of the capacitor is 1⁄ n of the peak total voltage
(n is the order of the capacitor), which reduces the circuit's recharging inch charging voltage threshold.
      </p>
      <p>When the circuit is charging, D1 in the filling circuit is on, D2 and D3 are off, and the two filter
capacitors are connected in series. The series of capacitors reduces the total capacitance value and
therefore the time constant. When the circuit discharges, D1 in the filling circuit shuts off, D2 and D3
are on, and the two filter capacitors are connected in parallel. The voltage at both ends of each capacitor
is 1⁄2 peak voltage, which reduces the charging threshold when the circuit is recharged.
Output power of grain filling circuit is:
 =
=</p>
      <p>4 02  2 2
(2</p>
      <p>+  )2</p>
      <p>= 0, it can be known that the maximum output power and optimal load resistance of
piezoelectric material are:</p>
      <p>Valley filling circuit can greatly increase the conduction Angle of rectifier tube, by filling the valley
point, the input current from the peak pulse to the waveform close to the sine wave, reduce harmonic
content, improve the power factor, significantly reduce waveform distortion.</p>
    </sec>
    <sec id="sec-6">
      <title>4. BUCK - BOOST circuit</title>
      <p>The waveform of the circuit corrected by the filling circuit is similar to that of the DC power supply.
At this time, the output voltage can be adjusted by the buck-Boost circuit to make the output voltage
meet the requirements of the load. The circuit is shown in Figure 4.</p>
      <p>=</p>
      <p>1 −</p>
      <p>(8)
(9)
(10)
(11)
state, so the input capacitor C1 is the main power supply during this process. At the output end, C2
provides energy for R0 by its own discharge. When switch S is off, power supply V charges the input
capacitor. Since the current of the inductor cannot be mutated, the inductor L1 supplies power to the
output capacitor C2 and the load R0 through the continuation tube D1. After stable operation, the
inductance is conserved in volts second. When the switch S is on, the inductance voltage is equal to the
input power voltage VIN; When switch S is off, the inductance voltage is equal to the output voltage
VOUT. Let T be the cycle, TON be the on-time, TOFF be the off time, D be the duty cycle.</p>
      <p>When duty cycle is less than 0.5, output step-down; When duty cycle is greater than 0.5, output
boost.</p>
    </sec>
    <sec id="sec-7">
      <title>5. Simulation</title>
      <p>The circuit is shown in Figure 5, figure 6 is the simulation of traditional energy collection circuit,
and Figure 7 is the simulation of induced piezoelectric energy collection circuit.</p>
    </sec>
    <sec id="sec-8">
      <title>6. Conclusion</title>
      <p>Comparing the output voltage of the traditional energy collection circuit with that of the induced
piezoelectric energy collection circuit, the peak voltage is increased by 1.455 V, the valley value is
increased by 0.703 V, the average output voltage is increased by 29.4%, and the energy collection
efficiency is improved to a certain extent.</p>
      <p>In this paper, a piezoelectric energy collection circuit with low power consumption and high
acquisition efficiency is designed, which uses active diode instead of traditional diode to reduce the
voltage loss and improve the power conversion efficiency.
7. References</p>
    </sec>
  </body>
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