<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">EPE</journal-id><journal-title-group><journal-title>Energy and Power Engineering</journal-title></journal-title-group><issn pub-type="epub">1949-243X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/epe.2015.710047</article-id><article-id pub-id-type="publisher-id">EPE-60122</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Finite Element Analysis of Vehicle Load Effect on Harvesting Energy Properties of a Piezoelectric Unit
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hunhua</surname><given-names>Sun</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hongbing</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jie</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Guangqing</surname><given-names>Shang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mechanic and Electronic Engineering, Suzhou Vocational University, Suzhou, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>chh_sunny@163.com(HS)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>10</day><month>09</month><year>2015</year></pub-date><volume>07</volume><issue>10</issue><fpage>500</fpage><lpage>508</lpage><history><date date-type="received"><day>4</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>27</month>	<year>September</year>	</date><date date-type="accepted"><day>30</day>	<month>September</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  To realize the goal of harvesting energy from pavement vibration on a large scale, a new type of piezoelectric harvesting units as the energy transducer has been proposed. The piezoelectric harvesting units are paved 40 mm below the asphalt, which is the same as thickness of the top layer of typical asphalt pavement in China. The spacing distance is 2200 mm, which is the same as the one between two tires of a normal vehicle. A mathematical model of the unit is deduced on Meda empirical formula and Hamilton principle and piezoelectric equations. Effects of the external vehicle load on its harvesting energy properties and pavement deformation and stress are analyzed with the finite element method. The results show that the excited voltage is linearly variation with contact pressure while the harvested electrical energy exponential varies with contact pressure. The more the contact pressure is, the larger the harvested electrical energy and the deformation and stress are. The harvested electrical energy also increases with the load frequency. At least 100 mJ of electrical energy can be collected with the proposed piezoelectric harvesting unit. It shows that the technology application of the piezoelectric harvesting energy from pavement is promising.
 
</p></abstract><kwd-group><kwd>Pavement Vibration</kwd><kwd> Piezoelectric Harvesting Unit</kwd><kwd> Positive Piezoelectric Effect</kwd><kwd> Finite Element Analysis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Vibration-based piezoelectric harvesting energy technology has received growing attention over the last decade. The main application of the technology is to power small electronic devices by using the vibration energy available in ambient environment, such as MEMS micro-power devices [<xref ref-type="bibr" rid="scirp.60122-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60122-ref2">2</xref>] . Recently, there also has a breakthrough in large power generation by using the technology. According to the report [<xref ref-type="bibr" rid="scirp.60122-ref3">3</xref>] , when a vehicle is driven along the road, the piezoelectric harvester embedded under the pavement is deformed and produces electric charge. Although one piezoelectric harvester can only produce a small amount of electricity, millions of the harvesters generate huge electrical power, which can be transported into the state grid for accumulating or storing it for later use. If the technology is widely applied, the vast road will become a large electricity farm for supplying human being with inexhaustible energy.</p><p>The technology of vibration-based piezoelectric energy harvesting from pavement has attracted more and more attention of academia and industry. It will be one important direction of piezoelectric harvesting energy by replacing conventional electricity generation. It also will be a groundbreaking systematic works. However, as a new concept, the state of studying the technology is still in its infancy, a complete theoretical system has not been established. Few researches have dealt with it until now. Patent on the piezoelectric method and system for harvesting vibration from road was invented [<xref ref-type="bibr" rid="scirp.60122-ref4">4</xref>] . Finite element analysis of Cymbal piezoelectric transducers for harvesting energy from asphalt pavement was done in Ref. [<xref ref-type="bibr" rid="scirp.60122-ref5">5</xref>] . Effects of structural parameters and the planted depth of the piezoelectric harvester on electromechanical properties and pavement deformation were studied via the finite element method (FEM), a new kind of piezoelectric harvesting unit was proposed [<xref ref-type="bibr" rid="scirp.60122-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.60122-ref7">7</xref>] . Based on this structure, this paper proposes the road paving ways and builds piezoelectric harvesting energy model under vehicle loads. Effect of loads on piezoelectric harvesting properties will then be simulated and analyzed. Some conclusions will finally be drawn.</p></sec><sec id="s2"><title>2. Layout of the Piezoelectric Harvesting Unit</title><p>To efficiently harvest vibration energy from pavement on large scale and do not affect the vehicle’s safety and comfort, the piezoelectric harvesting unit (PHU) proposed in Ref. [<xref ref-type="bibr" rid="scirp.60122-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.60122-ref7">7</xref>] is adopted here. That is, a piezoelectric vibrator is made up a cylinder disk of &#248;30 &#215; 10 mm and copper electrodes welded on up and down surfaces. A 8 &#215; 8 layout of the piezoelectric vibrators in electrically parallel is arranged to constitute a 280 &#215; 280 &#215; 20 mm square of PHU. The space between the vibrators is 4 mm.</p><p>Taking the typical pavement structure in China into consideration, the surface of asphalt pavement always includes 2 - 3 layers. The thickness of the top layer is 40 mm. For the better comprehensive result, the PHU is embedded 40 mm under the bottom of the top asphalt layer. About the optimal design for layouting the PHUs is discussed in detail in Ref. [<xref ref-type="bibr" rid="scirp.60122-ref7">7</xref>] . During the process of reforming the pavement, the top asphalt layer of 40 mm height is firstly whipped, two trenches of 280 mm width perpendicular to the vehicle’s traveling direction, whose space is 2200 mm, are then excavated. PHU is finally put into the trenches. After the asphalt is replaced, the pavement with PHU is finished. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the schematic diagram of paving PHU. The PHU width of 280 mm is larger than the standard tire’s width (≤240 mm) for completely harvesting energy from the vehicle load. The spacing distance of 2200 mm is the same as the standard wheelbase. Each PHU is closely layout. All these are to ensure that each PHU is not only able to absorb road vibration energy, but also to avoid a direct impact on PHU from being damaged.</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Schematic graph of paving PHU under asphalt surface. (a) Longitudinal section; (b) Transverse section.</title></caption><fig id ="fig1_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-6201878x5.png"/></fig></fig-group></sec><sec id="s3"><title>3. Model of PHU under Vehicle Load</title><p>Assuming that vertical load uniformly acts on the pavement when a vehicle passes, the pressure between the tire and the pavement can be deduced from the Meda’s empirical formula [<xref ref-type="bibr" rid="scirp.60122-ref8">8</xref>] :</p><disp-formula id="scirp.60122-formula1375"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x6.png"  xlink:type="simple"/></disp-formula><p>where F is the contact pressure in MPa, F' is wheel weight in kN, F<sub>i</sub> is tire inner pressure in MPa.</p><p>Based on Hamilton principle, the pavement’s dynamic finite element equation is</p><disp-formula id="scirp.60122-formula1376"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x7.png"  xlink:type="simple"/></disp-formula><p>where [M], [C], [K] are pavement quality matrix, damping and stiffness matrices, respectively.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x8.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x9.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x10.png" xlink:type="simple"/></inline-formula> are the node’s accelerator, speed and displacement vectors.</p><p>The damping matrix of [C] is usually calculated according to the Raleigh damping assumption in the following equation</p><disp-formula id="scirp.60122-formula1377"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x11.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x12.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x13.png" xlink:type="simple"/></inline-formula>are damping co-efficiencies, which are respectively set to be 0.4 and 0.05 based on the empirical value.</p><p>When a piezoelectric vibrator is embedded under the pavement, it will generate strain under the vehicle load. The piezoelectric equations are described as the following equations</p><disp-formula id="scirp.60122-formula1378"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x14.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60122-formula1379"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x15.png"  xlink:type="simple"/></disp-formula><p>where, i, j = 1, 2, 3, ∙∙∙, 6; m, k = 1, 2, 3; S is the strain tensor; T is the stress tensor; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x16.png" xlink:type="simple"/></inline-formula>is the compliance tensor of constant electric field condition; E is the external electric field; D is the charge displacement tensor; d is piezoelectric strain constant tensor; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x17.png" xlink:type="simple"/></inline-formula>(permittivity) is dielectric constant tensor measure at constant stress condition.</p><p>The system, which is constituted by vehicle, pavement and PHU, is a complex multi-bodies dynamics one. To meet the requirement of large stress, low frequency and random vibration and to improve the usage life, the designed PHU adopts the d<sub>33</sub> mode. According to the above Equations (1), (2), the pavement node displacement <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x18.png" xlink:type="simple"/></inline-formula> is obtained. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x19.png" xlink:type="simple"/></inline-formula>is then used as the boundary condition of the system to the node of E<sub>i</sub> based on Equations (4), (5). Thus, the excited voltage of one vibrator is calculated by Equation (6)</p><disp-formula id="scirp.60122-formula1380"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x20.png"  xlink:type="simple"/></disp-formula><p>where U<sub>3</sub> is the electric potential (voltage) at the direction 3 caused by polarization changing, which can be obtained via the finite element analysis (FEA); t is the thickness of PZT disk. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x21.png" xlink:type="simple"/></inline-formula>is piezoelectric voltage constant, which is deduced from the following equation</p><disp-formula id="scirp.60122-formula1381"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x22.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x23.png" xlink:type="simple"/></inline-formula>is vacuum dielectric constant,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x24.png" xlink:type="simple"/></inline-formula>.</p><p>The electric energy stored in one piece of piezoelectric vibrator can be calculated by</p><disp-formula id="scirp.60122-formula1382"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x25.png"  xlink:type="simple"/></disp-formula><p>where, P<sub>1</sub> is the stored electric energy of a vibrator; A is the surface area of PZT disk.</p><p>As described above, a PHU, which is the 8 &#215; 8 array of the vibrator, can then harvest the total electric energy</p><disp-formula id="scirp.60122-formula1383"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x26.png"  xlink:type="simple"/></disp-formula><p>where, P<sub>2</sub> is electric energy harvested by one piece of PHU.</p><p>According to the above proposed PHU size and laying way, about 14, 280 pieces of PHU are embedded under one mile of two-side pavement. Thus, one piece of PHU may be harvested minimal energy, but the total electric energy is still considerable if the PHU is paved on large scale. Therefore, study on the technology of piezoelectric harvesting energy from pavement vibration will cause a major contribution to social and environment, especially to some countries which mainly rely on coal power generation. The resulting low carbon effect is immeasurable.</p><p>It can be drawn from the Formula (1)-(9) that the harvested electric energy of a PHU is relevant to the properties of piezoelectric material and the wheel weight and tire pressure. Here, the effect of wheel weight and tire pressure on the harvested electric energy is discussed.</p></sec><sec id="s4"><title>4. The Finite Element Model and Material Parameters</title><p>The typical semi-rigid pavement structure is adopted to be the pavement model. The material’s parameters of pavement layer and steel are shown in <xref ref-type="table" rid="table1">Table 1</xref>. Because the contact area between tire and pavement is near a rectangle, tire weight can be treated to evenly act on this area. <xref ref-type="table" rid="table2">Table 2</xref> shows the relationship among wheel weight, tire pressure and tire width. The tire contact pressure is also calculated according to Equation (1), as shown in <xref ref-type="table" rid="table2">Table 2</xref>. PZT -5A material parameters are shown in <xref ref-type="table" rid="table3">Table 3</xref>. Here, it is supposed that only one tire load is considered and the pressure contact width is the same as the tire’s width. Meanwhile, in order to put more attention on the PHU, only the asphalt layer is considered in FEM and the layers of asphalt surface possess the same properties. In viewing to axial symmetry, the finite element model of the pavement piezoelectric harvesting system is built in <xref ref-type="fig" rid="fig2">Figure 2</xref> via ANSYS 10.0.</p><p>During simulation, Plane13 is chosen to mesh PZT disk and Plane42 is used to mesh pavement and steel. The electrical potential of the top layer of PZT disk is set to zero, the same potential is set for the bottom of PZT disk. The displacement of the bottom of the model is set to zero. These boundary conditions are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p></sec><sec id="s5"><title>5. Simulation Results and Analysis</title><sec id="s5_1"><title>5.1. The Excited Voltage of PHU</title><p>Effect of the contact pressure on the excited voltage is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. It can be concluded that the excited voltage is linear with the contact pressure. The relationship can be expressed as following</p><disp-formula id="scirp.60122-formula1384"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x27.png"  xlink:type="simple"/></disp-formula><p>From the equation, it can be known that intercept and slope are 0.523 and 1123.255, respectively. It shows that the fitted line is almost through the origin and the contact pressure takes great influence on the excited voltage.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Asphalt and steel material parameters</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Material</th><th align="center" valign="middle" >Elastic modulus/MPa</th><th align="center" valign="middle" >Poisson ratio</th><th align="center" valign="middle" >Density/kg∙m<sup>−3</sup></th></tr></thead><tr><td align="center" valign="middle" >Asphalt</td><td align="center" valign="middle" >1800</td><td align="center" valign="middle" >0.32</td><td align="center" valign="middle" >2400</td></tr><tr><td align="center" valign="middle" >Metal</td><td align="center" valign="middle" >200,000</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >7800</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Tire’s weight and pressure and width [<xref ref-type="bibr" rid="scirp.60122-ref9">9</xref>] </title></caption><table><tbody><thead><tr><th align="center" valign="middle" >No.</th><th align="center" valign="middle" >Tires’ weight F'/kN</th><th align="center" valign="middle" >Tire pressure F<sub>i</sub>/MPa</th><th align="center" valign="middle" >Tire width/mm</th><th align="center" valign="middle" >Contact pressure F/MPa</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >220</td><td align="center" valign="middle" >0.4</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >220</td><td align="center" valign="middle" >0.52</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >220</td><td align="center" valign="middle" >0.573</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >60</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >220</td><td align="center" valign="middle" >0.63</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >0.74</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >0.855</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> PZT -5A material parameters</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameters</th><th align="center" valign="middle" >Value</th></tr></thead><tr><td align="center" valign="middle" >Density (kg/m<sup>3</sup>)</td><td align="center" valign="middle" >7500</td></tr><tr><td align="center" valign="middle" >Poisson’s ratio</td><td align="center" valign="middle" >0.32</td></tr><tr><td align="center" valign="middle" >Relative permittivity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x28.png" xlink:type="simple"/></inline-formula> (10<sup>−</sup><sup>9</sup> F/m)</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x29.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Piezoelectric voltage constant matrix [d] (pC/N)<sup> </sup></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x30.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Flexible piezoelectric constant matrix [s] (GPa)</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-6201878x31.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Finite element model</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-6201878x32.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Excited voltage vary with contact pressure</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-6201878x33.png"/></fig><p>The fitted error between the simulation data and the fitted ones is shown in <xref ref-type="table" rid="table4">Table 4</xref>. The Adj. R-Square is 0.99985, which is almost near to 1. It proves that the fitted result of the excited voltage via contact pressure fits very well with the simulation data.</p></sec><sec id="s5_2"><title>5.2. The Harvested Electrical Energy of PHU</title><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows the harvested electrical energy with one piece of the proposed PHU. It can be seen that at least 100 mJ of the electric energy is collected with PHU. The relationship of the harvested electrical energy and the contact pressure is expressed as the following exponential equation</p><disp-formula id="scirp.60122-formula1385"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x34.png"  xlink:type="simple"/></disp-formula><p>According to the fitted statistics, the error and adj. R-square are listed in <xref ref-type="table" rid="table5">Table 5</xref>. The fitted exponential curve fits very well with the simulation data.</p><p>Expanding the project to a length of one kilometer along two lanes, about 450 KWh electrical energy can be harvested with these PHU modules, provided that approximately 600 heavy trucks travel along through the interval per hour on average.</p></sec><sec id="s5_3"><title>5.3. The Maximum Deformation of the Pavement</title><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows relationship of the maximum deformation of pavement with contact pressure. The relationship can be expressed as a liner equation as follows</p><disp-formula id="scirp.60122-formula1386"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-6201878x35.png"  xlink:type="simple"/></disp-formula><p>The error is also calculated, as shown in <xref ref-type="table" rid="table6">Table 6</xref>. The Adj. R-square is 0.99995. It indicates that the fitted result of the maximum deformation of pavement via contact pressure fits very well with the simulation data.</p><p>Taken these comprehensive factors into consideration, when the contact pressure increases, the harvested electrical energy increases. Meanwhile, the pavement displacement also increases. The maximum deformation of pavement is located on the model of x = 0, the point of the contact center of the tire and the pavement.</p></sec><sec id="s5_4"><title>5.4. The Maximum Stress</title><p><xref ref-type="fig" rid="fig6">Figure 6</xref> shows the stress distribution on the piezoelectric harvesting system from pavement. It can be seen that the maximum stress is located on PZT disk. The maximum stress changes with the contact pressure, as shown in</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> The error of the fitted voltage line</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >Intercept</th><th align="center" valign="middle"  colspan="2"  >Slope</th><th align="center" valign="middle" >Statistics</th></tr></thead><tr><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >Adj. R-Square</td></tr><tr><td align="center" valign="middle" >0.523</td><td align="center" valign="middle" >3.92849</td><td align="center" valign="middle" >1123.255</td><td align="center" valign="middle" >6.16763</td><td align="center" valign="middle" >0.99985</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> The error of the fitted electrical energy</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >y<sub>0</sub></th><th align="center" valign="middle"  colspan="2"  >A<sub>1</sub></th><th align="center" valign="middle"  colspan="2"  >t<sub>1</sub></th><th align="center" valign="middle" >Statistics</th></tr></thead><tr><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >Adj. R-Square</td></tr><tr><td align="center" valign="middle" >0.00114</td><td align="center" valign="middle" >0.00136</td><td align="center" valign="middle" >0.69773</td><td align="center" valign="middle" >0.00213</td><td align="center" valign="middle" >0.58519</td><td align="center" valign="middle" >0.03272</td><td align="center" valign="middle" >0.99978</td></tr></tbody></table></table-wrap><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> The error of the fitted deformation line</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >Intercept</th><th align="center" valign="middle"  colspan="2"  >Slope</th><th align="center" valign="middle" >Statistics</th></tr></thead><tr><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >Adj. R-Square</td></tr><tr><td align="center" valign="middle" >0.00114</td><td align="center" valign="middle" >0.00136</td><td align="center" valign="middle" >0.69773</td><td align="center" valign="middle" >0.00213</td><td align="center" valign="middle" >0.99995</td></tr></tbody></table></table-wrap><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Electric energy vary with contact pressure</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-6201878x36.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Deformation vary with contact pressure</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-6201878x37.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Stress distribution</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-6201878x38.png"/></fig><p><xref ref-type="fig" rid="fig7">Figure 7</xref>. The variation of stress linearly changes with the contact pressure.</p><p>The maximum stress on a PZT disk is 8.8 MPa when the maximum contact pressure acts on the pavement. Contrast to the allowable limit stress of 100 MPa, 8.8 MPa is so small that the PHU can normally work.</p></sec><sec id="s5_5"><title>5.5. Effect of Contact Pressure Frequency</title><p>When a vehicle is driven at different speed, the frequency of the vehicle load varies. Taken a vehicle with 2 axes and the axial distance of 4.5 m, two tire weight of 80 kN for example, the various speeds cause different frequencies of the vehicle load, as shown in <xref ref-type="table" rid="table7">Table 7</xref>. According to the transit analysis via FEM, the excited voltage also changes with the speed. The simulation result is shown in <xref ref-type="table" rid="table7">Table 7</xref>.</p><p>The excited voltage increases with the increase of the vehicle load frequency. However, its effect is significantly smaller than contact pressure.</p><p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows real-time change characteristics of the excited voltage at 80 km/h speed. Obviously, the frequency of excited voltage is the same as the frequency of the vehicle load.</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Stress vary with contact pressure</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-6201878x39.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Real-time vary of the excited voltage</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-6201878x40.png"/></fig><table-wrap id="table7" ><label><xref ref-type="table" rid="table7">Table 7</xref></label><caption><title> Excited voltages under different speeds</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Speed (km/h)</th><th align="center" valign="middle" >Frequency (Hz)</th><th align="center" valign="middle" >Excited voltage (V)</th></tr></thead><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >3.71</td><td align="center" valign="middle" >847.6</td></tr><tr><td align="center" valign="middle" >70</td><td align="center" valign="middle" >4.32</td><td align="center" valign="middle" >850</td></tr><tr><td align="center" valign="middle" >80</td><td align="center" valign="middle" >4.94</td><td align="center" valign="middle" >852.6</td></tr><tr><td align="center" valign="middle" >90</td><td align="center" valign="middle" >5.56</td><td align="center" valign="middle" >855</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >6.18</td><td align="center" valign="middle" >857.5</td></tr><tr><td align="center" valign="middle" >110</td><td align="center" valign="middle" >6.79</td><td align="center" valign="middle" >860</td></tr><tr><td align="center" valign="middle" >120</td><td align="center" valign="middle" >7.41</td><td align="center" valign="middle" >862.4</td></tr></tbody></table></table-wrap></sec></sec><sec id="s6"><title>6. Conclusions</title><p>The layout of piezoelectric harvesting energy units is discussed. Effect of vehicle loads on piezoelectric energy properties is discussed via the finite element analysis. The harvested energy variation with contact pressure is concluded.</p><p>The results show that the maximum stress happens on the PZT disk and lies within the allowable limit stress. Effect of vehicle speed on the excited voltage and the harvested electrical energy is significantly smaller than contact pressure. One piece of PHU can harvest at least 100 mJ electrical power.</p><p>All proves that the technology of piezoelectric harvesting energy from pavement vibration has a promising prospect. The future work will focus on the consistency of PHUs and pavement along with the pavement test.</p></sec><sec id="s7"><title>Acknowledgements</title><p>This research was supported by the National Natural Science Foundation of China (No. 51175359) and the 4th “333 Engineering” Research Funding Project of Jiangsu Province (BRA2014086).</p></sec><sec id="s8"><title>Cite this paper</title><p>ChunhuaSun,HongbingWang,JieLiu,GuangqingShang, (2015) Finite Element Analysis of Vehicle Load Effect on Harvesting Energy Properties of a Piezoelectric Unit. Energy and Power Engineering,07,500-508. doi: 10.4236/epe.2015.710047</p></sec></body><back><ref-list><title>References</title><ref id="scirp.60122-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Leland, E.S., Lai, E.M. and Wright, P.K. (2004) A Self-Powered Wireless Sensor for Indoor Environmental Monitoring. WNCG Conference, Austin.</mixed-citation></ref><ref id="scirp.60122-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Arms, S., Townsend, C.P., et al. (2005) Power Management for Energy Harvesting Wireless. Smart Structures and Materials 2005: Smart Electronic, MEMS, BioMEMS, and Nanotechnology, Proc of SPIE 2005, 5763, 267-275.  
http://dx.doi.org/10.1117/12.600302</mixed-citation></ref><ref id="scirp.60122-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">http://www.innowattech.co.il/index.aspx</mixed-citation></ref><ref id="scirp.60122-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Cao, B.-G., Gao, Z.-H., Song, Z.-P., et al. (2005) Method and System of Highway Harvesting Energy from Piezoelectric Vibration: China, 1633009A.</mixed-citation></ref><ref id="scirp.60122-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Zhao, H.D., Yu, J. and Ling, J.M. (2010) Finite Element Analysis of Cymbal Piezoelectric Transducers for Harvesting Energy from Asphalt Pavement. Journal of the Ceramic Society of Japan, 118, 909-915.  
http://dx.doi.org/10.2109/jcersj2.118.909</mixed-citation></ref><ref id="scirp.60122-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Sun, C.-H., Du, J.-H., Wang, H.-B. and Shang, G.-Q. (2013) Properties Analysis of Piezoelectric Harvesters from Pavement Vibration. Piezoelectics &amp; Acoustooptics, 35, 556-560.</mixed-citation></ref><ref id="scirp.60122-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Sun, C.-H., Shang, G.-Q., Zhang, Y.-K. and Du, J.-H. (2013) Designing Piezoelectric Harvesting Unit from Road Vibration. Advanced Materials Research, 712-715, 1368-1371.</mixed-citation></ref><ref id="scirp.60122-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Shan, J.-S., Huang, X.-M. and Liao, G.-Y. (2007) Dynamic Response Analysis of Pavement Structure under Moving Load. Journal of Highway and Transportation Research and Development, 24, 10-13.</mixed-citation></ref><ref id="scirp.60122-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Shi, C.-X., Yang, Q. and Guo, Z.-Y. (2008) Research on Mechanical Properties of Asphalt Pavement in Highway Tunnel. Journal of Highway and Transportion Research and Development, 25, 8-11.</mixed-citation></ref></ref-list></back></article>