<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>1794-1237</journal-id>
<journal-title><![CDATA[Revista EIA]]></journal-title>
<abbrev-journal-title><![CDATA[Rev.EIA.Esc.Ing.Antioq]]></abbrev-journal-title>
<issn>1794-1237</issn>
<publisher>
<publisher-name><![CDATA[Escuela de ingenieria de Antioquia]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S1794-12372017000100009</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[UNDESIRED SPLASH OVER ON EQUIPMENTS USING INDUCTIVE SENSORS FOR MONITORING AUTOMOTIVE VEHICLES' CONTROLLED SPEED]]></article-title>
<article-title xml:lang="es"><![CDATA[PRESENCIA NO DESEADA DEL SPLASH OVER EN EQUIPOS QUE UTILIZAN SENSORES INDUCTIVOS PARA EL MONITOREO DE LA VELOCIDAD CONTROLAD EN VEHÍCULOS AUTOMOTORES]]></article-title>
<article-title xml:lang="pt"><![CDATA[PRESENÇA NÃO DESEJADA DO SPLASH OVER EM INSTRUMENTOS DE SENSORES INDUTIVOS QUE CONTROLAM OS VEÍCULOS AUTOMOTORES]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Monteiro]]></surname>
<given-names><![CDATA[Silvio]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Réche]]></surname>
<given-names><![CDATA[Maurício]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[de Assis]]></surname>
<given-names><![CDATA[Altair S]]></given-names>
</name>
<xref ref-type="aff" rid="A03"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,National Institute of Metrology, Quality and Techonology  ]]></institution>
<addr-line><![CDATA[Rio de Janeiro ]]></addr-line>
<country>Brasil</country>
</aff>
<aff id="A02">
<institution><![CDATA[,National Institute of Metrology, Quality and Techonology  ]]></institution>
<addr-line><![CDATA[Rio de Janeiro ]]></addr-line>
<country>Brasil</country>
</aff>
<aff id="A03">
<institution><![CDATA[,Fluminense Federal University Applied Mathematics Department ]]></institution>
<addr-line><![CDATA[Niterói ]]></addr-line>
<country>Brasil</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>06</month>
<year>2017</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>06</month>
<year>2017</year>
</pub-date>
<numero>27</numero>
<fpage>97</fpage>
<lpage>109</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_arttext&amp;pid=S1794-12372017000100009&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_abstract&amp;pid=S1794-12372017000100009&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_pdf&amp;pid=S1794-12372017000100009&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[This article aims to evaluate instruments that oversight traffic flow electronically, using inductive surface sensors, based on the change of local magnetic field. More specifically, we study the possibility of false speed detections, due to the manifestation of the phenomenon called splash over - which means a space splash of the magnetic field lines out of the measuring zone. We show, through the literature, and practical simulations, the damage that can be caused by splash on the correct speed measurement and identification of the car under suspicions. It is also presented solutions to inhibiting unwanted velocity measurements due to this effect.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Este artículo busca evaluar los instrumentos que supervisan el flujo de tráfico electrónicamente mediante el uso sensores de superficie inductiva con base en la modificación del campo magnético. Más específicamente, estudiamos la posibilidad de detecciones falsas de velocidad debido a la manifestación del fenómeno llamado splash over - que es un espacio registrado en las líneas del campo magnético por fuera del área de medición. Demostramos a través de la literatura, y las simulaciones prácticas, el daño que puede ser causado por el splash en la medición de la velocidad correcta y la identificación del vehículo bajo sospecha. También se presentan soluciones para inhibir las mediciones de velocidad no deseadas debido a este efecto.]]></p></abstract>
<abstract abstract-type="short" xml:lang="pt"><p><![CDATA[Este artigo trata de instrumentos que supervisionam o tráfico eletronicamente mediante o uso de sensores de superfície inductive, baseado na modificação do campo magnético. Mais especificamente, a possibilidade de detecções falsas de veículos devido à manifestação do fenômeno chamado splash over. Demonstrando através dos fundamentos bibliográfico e simulações práticas, o dano que pode ser causado pelo splash over sobre a medida da velocidade correta e a identificação do mensurando. Também é possível expor soluções para a inibição de falhas devido a este fenômeno.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Oversight Traffic]]></kwd>
<kwd lng="en"><![CDATA[Speed Meters]]></kwd>
<kwd lng="en"><![CDATA[Legal Metrology]]></kwd>
<kwd lng="en"><![CDATA[Splash Over]]></kwd>
<kwd lng="en"><![CDATA[Magnetic Field]]></kwd>
<kwd lng="es"><![CDATA[Supervisión del tráfico]]></kwd>
<kwd lng="es"><![CDATA[medición de velocidad]]></kwd>
<kwd lng="es"><![CDATA[metrología legal]]></kwd>
<kwd lng="es"><![CDATA[splash over]]></kwd>
<kwd lng="es"><![CDATA[campo magnético]]></kwd>
<kwd lng="pt"><![CDATA[Supervisão do trânsito]]></kwd>
<kwd lng="pt"><![CDATA[medidores de velocidade]]></kwd>
<kwd lng="pt"><![CDATA[metrologia legal]]></kwd>
<kwd lng="pt"><![CDATA[splash over]]></kwd>
<kwd lng="pt"><![CDATA[campo magnético]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  <font face="verdana" size="2">     <p align="center"><font size="4"><b>UNDESIRED SPLASH OVER ON EQUIPMENTS USING INDUCTIVE SENSORS FOR MONITORING AUTOMOTIVE VEHICLES' CONTROLLED SPEED</b></font></p>     <p align="center"><font size="3"><b>PRESENCIA NO DESEADA DEL SPLASH OVER EN EQUIPOS QUE UTILIZAN SENSORES INDUCTIVOS PARA EL MONITOREO DE LA VELOCIDAD CONTROLAD EN VEH&Iacute;CULOS AUTOMOTORES</b></font></p>     <p align="center"><font size="3"><b>PRESEN&Ccedil;A N&Atilde;O DESEJADA DO SPLASH OVER EM INSTRUMENTOS DE SENSORES INDUTIVOS QUE CONTROLAM OS VE&Iacute;CULOS AUTOMOTORES</b></font></p>     <p>&nbsp;</p>     <p><b>Silvio Monteiro<sup>1</sup>, Maur&iacute;cio R&eacute;che<sup>2</sup>, Altair S. de Assis<sup>3</sup></b></p>     <p>1 Mechanical Engineer, Rio de Janeiro State  University; Master in Metrology and Quality, National Institute of Metrology,  Quality and Techonology. Researcher Technologist at National Institute of  Metrology, Quality and Techonology (Inmetro). Rio de Janeiro, Brasil.  Caixa Postal 100294. Post code: 24001-970, Niter&oacute;i, Rio de Janeiro, Brazil. Correo electr&oacute;nico: <a href="mailto:altair@vm.uff.br">altair@vm.uff.br</a>.    <br> 2 Physicist, Rio de Janeiro Federal University;  Master of Integrated Management System, Fluminense Federal University.  Researcher Technologist at National Institute of Metrology, Quality and  Techonology (Inmetro). Rio de Janeiro, Brasil.    <br> 3 Physicist, Fluminense Federal University, Rio  de Janeiro; Master in Plasma Physics, Fluminense Federal University; Ph.D.  Plasma Physics, State University of Campinas; Full Professor, Applied  Mathematics Department, Fluminense Federal University. Niter&oacute;i, Brasil.</p>     <p>Art&iacute;culo recibido: 10-IV-2013/ Aprobado: 18-II-2017    ]]></body>
<body><![CDATA[<br>   Disponible online: 30 de agosto de 2017    <br> Discusi&oacute;n abierta hasta octubre de 2018</p> <hr size="1" />     <p><font size="3"><b>ABSTRACT</b></font></p>     <p>This article aims to evaluate instruments that  oversight traffic flow electronically, using inductive surface sensors, based on the change of local magnetic field. More  specifically, we study the possibility of false speed detections, due to the manifestation of the phenomenon called splash over -  which means a space splash of the magnetic field lines out of the measuring zone. We show, through the literature, and  practical simulations, the damage that can be caused by splash on the correct speed measurement and identification of  the car under suspicions. It is also presented solutions to inhibiting unwanted velocity measurements due to this effect.</p>     <p><b><font size="3">KEY WORDS</font></b>: Oversight Traffic, Speed Meters, Legal Metrology, Splash Over, Magnetic Field.</p> <hr size="1" />     <p><b><font size="3">RESUMEN</font></b></p>     <p>Este art&iacute;culo  busca evaluar los instrumentos que supervisan el flujo de tr&aacute;fico electr&oacute;nicamente  mediante el uso sensores de  superficie inductiva con base en la modificaci&oacute;n del campo magn&eacute;tico. M&aacute;s espec&iacute;ficamente,  estudiamos la posibilidad de  detecciones falsas de velocidad debido a la manifestaci&oacute;n del fen&oacute;meno llamado <i>splash over </i>- que es un espacio registrado en  las l&iacute;neas del campo magn&eacute;tico por fuera del &aacute;rea de medici&oacute;n. Demostramos a  trav&eacute;s de la literatura, y las  simulaciones pr&aacute;cticas, el da&ntilde;o que puede ser causado por el <i>splash </i>en la medici&oacute;n de la velocidad  correcta y la identificaci&oacute;n  del veh&iacute;culo bajo sospecha. Tambi&eacute;n se presentan soluciones para inhibir las  mediciones de velocidad no deseadas debido a este efecto.</p>     <p><font size="3"><b>PALABRAS CLAVE</b></font>: Supervisi&oacute;n del tr&aacute;fico, medici&oacute;n de velocidad, metrolog&iacute;a legal, splash over, campo magn&eacute;tico.</p> <hr size="1" />     <p><font size="3"><b>RESUMO</b></font></p>     <p>Este artigo  trata de instrumentos que supervisionam o tr&aacute;fico eletronicamente mediante o uso  de sensores de superf&iacute;cie  inductive, baseado na modifica&ccedil;&atilde;o do campo magn&eacute;tico. Mais especificamente, a  possibilidade de detec&ccedil;&otilde;es falsas de ve&iacute;culos  devido &agrave; manifesta&ccedil;&atilde;o do fen&ocirc;meno chamado splash over. Demonstrando atrav&eacute;s dos  fundamentos bibliogr&aacute;fico e  simula&ccedil;&otilde;es pr&aacute;ticas, o dano que pode ser causado pelo splash over sobre a  medida da velocidade correta e a identifica&ccedil;&atilde;o do mensurando. Tamb&eacute;m &eacute; poss&iacute;vel expor solu&ccedil;&otilde;es para a  inibi&ccedil;&atilde;o de falhas devido a este fen&ocirc;meno.</p>     ]]></body>
<body><![CDATA[<p><font size="3"><b>PALAVRAS-CHAVE</b></font>: Supervis&atilde;o do tr&acirc;nsito, medidores de velocidade, metrologia legal, splash over, campo magn&eacute;tico.</p> <hr size="1" />     <p><font size="3"><b>1. INTRODUCTION</b></font></p>     <p>Traffic accidents, according to the World Health Organization (2004) victimize fatally annually more than 1.2 million people worldwide and injure about 50 million others.</p>     <p>Excessive speed alone, or combined with other factors, may be considered as fundamental agent to induce traffic accidents. Data from the Brazilian Federal Highway Police on accidents occurring on federal highways in Brazil confirm the impact of high speeding in the statistics of traffic accidents, directly or leveraging other factors (Rizzoto, 2010).</p>     <p>Monitoring speed electronically through instruments gauge speed of motor vehicles is considered a powerful ally in the effort to curb speeding and accidents resulting from this condition. Such tools are already widely used for over 30 years in various parts of the world.</p>     <p>The principal means used commercially in the speed measurement of vehicles are:</p>     <p>Radar: Its operation is based on the   movement of vehicles. The instrument emits an   electromagnetic wave, usually radiofrequency   waves, which reaches some object, it is reflected and   recaptured by the radar receiver. The movement   of the target will result in a change in the emitted   frequency. The difference between the emitted and   reflected frequencies is translated by the decoder   on the radar as a speed value.</p>     <p>Optical (Laser): The instruments with this technology to measure speeds use monochromatic waves emitted by a laser. The time a laser pulse takes to reach the target and return is directly proportional  to the distance of this target. Thus the emission of various known pulses in times can determine the distance to a vehicle in this time interval and hence the speed.</p>     <p>Image processing: The speed measurement using imaging is performed through structure equipped with digital cameras with high capacity. Its working principle is based on the use of algorithms for image processing. The measurement points are virtually certain in his own image and are handled through software. The combination of multiple detection points makes it possible to measure the speed.</p>     <p>Inductive Sensors Surface: The inductive sensing is discussed more in detail in Section 2.</p>     ]]></body>
<body><![CDATA[<p>Each of these methods have inherent limitations to the technology used, and this may cause failures in the detection of the measured object, as shown in <b><a href="#tab1">Table 1</a></b>.</p>     <p align="center"><a name="tab1"></a><a href="img/revistas/eia/n27/n27a09tab1.gif" target="_blank">Table 1</a></p>     <p>Instruments that use sensors inductive  surface, the main goal of this article, are used  since the '60s across the world in several different  applications of traffic control.</p>     <p>Due to its low cost of installation and maintenance and its high reliability, they  have considered the most common equipment for electronic speed trap.</p>     <p>Initially, these instruments were limited to notifying the presence or absence of  metal mass on the inductive sensor. However,  with the advent of techniques for digital signal  processing, new features have been implemented to  those instruments (Nishimoto, 2006). Standing  out:</p> <ul>       <li>  Measurement of vehicle speed;</li>       <li>The detection of small metal mass of     vehicles, like scooters, bicycles;</li>       <li>The classification of vehicles within  each     category, based on information on the  magnetic     profile (Andreotti, 2001).</li>     </ul>     <p>Despite the obvious advantages of using inductive sensing for traffic control,  such technology has some weaknesses, as shown in <b><a href="#tab1">Table 1</a></b>.</p>     ]]></body>
<body><![CDATA[<p>The article focuses on the issue of splash over. The phenomenon of splash over is  present between adjacent traffic lanes. The  combination of the physical properties of inductive  sensors with certain conditions of instrument  configuration can enable its occurrence.</p>     <p>The splash over occurs due to the  spreading of the magnetic field lines, formed around  the inductive windings (Nishimoto, 2006). When these  lines extrapolate the traffic lane, the correct  detection of the vehicles speed may be affected  decisively.</p>     <p>In this paper, we present in section 2 the concept of traffic velocity control  through inductive circuit principle and the physics that  enables its operation, and therefore describing the  process of measuring the speed of vehicles. In  Section 3, we discuss the phenomenon the Splah over,  presenting the results of the tests carried on this  research. Finally, in section 4 we present the  conclusions.</p>     <p><b><font size="3">2. CIRCUIT CONSIDERATIONS</font></b></p>     <p>Briefly speaking, the instruments which  use   inductive sensors can detect the vehicle  speed due   changes in its inductive properties, they  are caused   by the passage of the metal structure of  the vehicle   in its detection area.</p>     <p>These instruments are basically formed by inductive sensor (inductive loop), feeder  cable, and an electronic control unit.</p>     <p>The inductive loop is in fact a coil,  usually with three to five turns of an insulated  cable buried in grooves in the floor. The feeder cable  is used to connect the junction box to the cabin  electronics. The electronic control unit hardware is  essential for the operation of the instrument. The  electronics unit feeds the sensor or bonds typically with  frequencies of 10 kHz to 200 kHz (Magalh&atilde;es, 2008).</p>     <p>The instruments which use inductive  sensors are able to detect the presence of a  conductive metallic surface by altering the physical  quantities of the oscillator circuit RLC present in  this type of instrument.</p>     <p>The current flowing in this circuit gives  rise to a magnetic field around the wires  forming the inductive loops, according to Ampere's  law. Since the circuit is powered by an alternating  current it has a magnetic flux varying with time.  Thus, when a vehicle cross the area of influence of  the magnetic field generated by the inductive loop, a  low-intensity currents is induced (Fullerton, Mills and  Kell, 1990).</p>     <p>The induced currents formed in the  conductive parts of the vehicle give rise to another  magnetic field that interacts with the field  initially established in the loop, causing a mutual inductance  between the inductive loop and the vehicle.  Fullerton, Mills and Kell (1990) report that the magnetic  flux generated by the current on the vehicle in  this condition has opposite direction to that  induced by the current flow, as expected by Lenz's  law, then causing a decrease in the total  magnetic field initially established around the loop.</p>     ]]></body>
<body><![CDATA[<p>The direct result of change in magnetic flux is the decreased inductance of the loop, since the inductance is proportional to the magnetic flux as shown below <b>(<a href="#for1">1</a>)</b>.</p>     <p><a name="for1"></a><img src="img/revistas/eia/n27/n27a09for1.gif"></p>     <p>Where:</p>     <p>  <i>L </i>= inductance;    <br>  <i>N </i>= number of turns;    <br>   <i>&Phi;</i><i>B </i>= magnetic flux;    <br>   <i>i </i>= electric current.</p>     <p>However, the electronic units do not detect directly the change in inductance. In general it has the ability to identify the increase of the resonance frequency of the circuit or decreasing the amplitude of the signal on the loop as shown in Nishimoto (2006).</p>     <p>The frequency of an LCR resonant circuit powered by an alternating current (Klein, Gibson, 2006), such as speed meters used by automotive vehicles is given by:</p>     <p><a name="for2"></a><img src="img/revistas/eia/n27/n27a09for2.gif"></p>     ]]></body>
<body><![CDATA[<p>Where:</p>     <p> f = frequency of the oscillator;    <br>   L = total circuit inductance;    <br>   C = total capacitance of the circuit.</p>     <p>It can be demonstrated using the known differential equation that models a LCR circuit with external source present:</p>     <p><a name="for3"></a><img src="img/revistas/eia/n27/n27a09for3.gif"></p>     <p>Where:</p>     <p> I = current;    <br>   E = electromotive force;    <br>   R = total resistance of the circuit.</p>     ]]></body>
<body><![CDATA[<p>The solution to <a href="#for3"><b>Equation (3)</b></a> can be given by (assuming that the external source has a given time dependence as shown below):</p>     <p><a name="for4"></a><img src="img/revistas/eia/n27/n27a09for4.gif"></p>     <p>Inserting the above equations in <b>(<a href="#for3">3</a>)</b>, one can   obtain:</p>     <p><a name="for4"></a><img src="img/revistas/eia/n27/n27a09for5.gif"></p>     <p>Because the system is forced by the source, the   circuit as a whole oscillates with the frequency of   the source, namely:</p>     <p><a name="for13"></a><img src="img/revistas/eia/n27/n27a09for13.gif"></p>     <p>Resulting in:</p>     <p><a name="for6"></a><img src="img/revistas/eia/n27/n27a09for6.gif"></p>     <p>Looking at equation <b>(<a href="#for6">5</a>)</b> we have that the   current amplitude will reach its maximum value   when:</p>     <p><a name="for7"></a><img src="img/revistas/eia/n27/n27a09for7.gif"></p>     ]]></body>
<body><![CDATA[<p>The frequency that aloud Io to have its maximum   value is called the natural frequency of oscillation  of   the circuit, and when the external source is equal to   this natural frequency it is usual to say that the  circuit   is in resonance with the external source.</p>     <p>Therefore the frequency of oscillation of a resonant circuit is given, respectively, by the formulas <b>(<a href="#for8">7</a>)</b> and <b>(<a href="#for8">8</a>)</b>:</p>     <p><a name="for8"></a><img src="img/revistas/eia/n27/n27a09for8.gif"></p>     <p> <a href="#for8"><b>Equations (7)</b></a> and <b>(<a href="#for8">8</a>)</b> show the dependence  of   the frequency with the inductance of the  circuit. For   better clarity the relationship, one can  derive the   frequency f to get df/dL:</p>     <p><a name="for9"></a><img src="img/revistas/eia/n27/n27a09for9.gif"></p>     <p>From <b>(<a href="#for9">9</a>)</b> we can write:</p>     <p><a name="for10"></a><img src="img/revistas/eia/n27/n27a09for10.gif"></p>     <p>Dividing both sides of the equation by  making   faith possible simplifications, we arrive  at:</p>     <p><a name="for11"></a><img src="img/revistas/eia/n27/n27a09for11.gif"></p>     <p><b><a href="#for11">Equation (11)</a></b> shows that the normalized   frequency varies with half the normalized   inductance. The negative sign means that  if there   exist variation in inductance, due to for  instance, the   presence of the metal mass of a passing  vehicle, it   will correspond to an opposite - contrary  increased   frequency. Increasing the inductance gives  rise to a   decreasing frequency.</p>     ]]></body>
<body><![CDATA[<p>The detection, by the electronics unit, of  the presence of a vehicle with speed above the  legal value occurs when the change in inductance  due to the interaction between the loop and  the vehicle exceeds a certain threshold previously  configured on the instrument.</p>     <p>The electronics unit of the instrument  allows making various adjustments of detection  sensitivity. This sensitivity defines the amount of  conductive metal mass that must be present in the  region of influence of the sensors to the vehicle is  detected by the instrument.</p>     <p><b><i><font size="3">2.1 Measuring speed with  inductive</font></i></b>   <font size="3"><b><i>sensors</i></b></font></p>     <p>The measurement of vehicles speed is one  of   the main applications of inductive sensors  in the   Brazilian traffic control. In Brazil,  together with   dedicated sensors, to monitor the  violation of the   red traffic light, this system is widely  used through   the instruments speed meters.</p>     <p>The speed control system uses generally  two or three inductive sensors that remain  installed on the monitored street or highway  maintaining a fixed distance from each  other.</p>     <p align="center"><a name="fig1"></a><img src="img/revistas/eia/n27/n27a09fig1.gif"></p>     <p>The operation of these instruments is  based on the basic kinematic equation:</p>     <p><a name="for12"></a><img src="img/revistas/eia/n27/n27a09for12.gif"></p>     <p>Where:</p>     <p> <i>d </i>= distance between sensors;    ]]></body>
<body><![CDATA[<br>  <i>t </i>= time elapsed between the firing  of the first   and second sensors.</p>     <p>The vehicle speed is calculated from the elapsed time between the setting of the  first and second sensor, which occur when the  activation threshold set on the instrument is  reached. Since the distance between the loops is known, the  velocity can be obtained using <a href="#for12"><b>Equation (12)</b></a>.</p>     <p><b><font size="3">3. THE SPLASH OVER</font></b></p>     <p>The splash over can induce false detection   (Coifman 2009), and this can be caused by  a vehicle   traveling on a highway adjacent to that in  which the   velocity detection equipment is installed.</p>     <p>This manifestation, unwanted, appears when long links operate at high levels of  sensibility, in general when the transit authority is  seeking to monitor small vehicles such as  motorcycles. This problem  can also affect facilities where the inductive sensor is positioned very close to the division between bands of the same highway.</p>     <p>The magnetic field lines formed around the coils of the sensor are not restricted to the  perimeter of the loop. Thus depending on the position of the loop towards the region of the splash, the magnetic field may invade the adjacent lane, particularly when operating at high sensitivities. With this condition, even a small change in the equilibrium conditions of the loop circuit / electronics unit, can cause  false identification of a vehicle offender.</p>     <p><b><a href="#fig2">Figure 2</a> </b>illustrates an example of occurrence of splash over. The bus interferes with the adjacent strip loop, which can cause the instrument to detect the presence of a ghost vehicle.</p>     <p align="center"><a name="fig2"></a><img src="img/revistas/eia/n27/n27a09fig2.gif"></p>     <p>According to Andreoti (2001), vehicles  that more induce splash over are buses and  cars. Both have small height above the ground and  large vertical metallic mass (vehicle sides)  that moves parallel side near the sensor borders.</p>     <p><b><i><font size="3">3.1 Test of the splash  proof over</font></i></b></p>     ]]></body>
<body><![CDATA[<p>In this investigation we want to certify  the   actual occurrence of the splash over, and  on what   conditions this unwanted phenomenon can be   present.</p>     <p>The tests were performed using a model of speed meter motor vehicles used in several  Brazilian cities for speed monitoring.</p>     <p>The speed meter is basically constituted  by devices of detecting and measuring,  processing, storage and registration with the  following characteristics:</p> <ul>       <li> Device detection and measurement:     consists of 1 pair of inductive sensors  and eletronics     unit  Reno A&#38;E Model 222. In this module are     contained components endowed with higher     metrological relevance.</li>       <li> Device processing: consists of hardware     and software capable of processing the  information     from the detection and measurement device. Integrate this module components necessary  for the     management of the instrument.</li>       <li> Storage Device: constituted of hard  drive     capable of storing the records of the  measurements.</li>       <li> Logging device: constituted digital  camera     with the ability to identify the measured  vehicle.</li>       <li> The instrument was installed in the test     field configured to monitor the speed of  one traffic     lane using one pair of inductive sensors.</li>       <li> Inductive sensors were fixed on the     pavement watching the default installation  of the     model, ie, distance between sensors 4 m, both     having 2 m long and 0.80 cm wide (<b><a href="#fig3">Figure 3</a></b>).</li>     </ul>     ]]></body>
<body><![CDATA[<p align="center"><a name="fig3"></a><img src="img/revistas/eia/n27/n27a09fig3.gif"></p>     <p>The unit vehicle detector is responsible for detecting the presence of a metal mass via the inductive sensors that are connected to it. This is possible by varying magnitudes related to the inductance of the circuit, such as frequency or amplitude. The board is able to inform the moments in which a vehicle enters and leaves the measuring zone, enabling the measurement of time and speed.</p>     <p>The model used in this study uses the board Reno A &#38; E to measure changes in the resonant frequency of each of the circuits formed by the sensors, connecting cables and a detection unit. The aim is to determine if a vehicle has entered into the detection zone. The detector applies a control voltage into the generating circuit. The passage of a metallic conductor causes the resonance frequency of the circuit increases. If this change exceeds a selectable threshold, determined by the sensitivity setting, the detector activates an output signal (Reno 2006).</p>     <p>Among other adjustments at the plate, it is possible to set the sensitivity of detection of the instrument. The model Reno A &#38; E setting allows eight different levels of detection thresholds. Thus, depending on the setting, you can discard the capture of small vehicles such as bicycles and motorcycles.</p>     <p>The manual of the operation detection plate used in the test indicates how the inductance of the circuit should vary in each level of sensitivity for  the detection to occur.</p>     <p>The methodology consisted of performing the pass test when for vehicles with dimensions beyond of the sensors in order to verify the detection capability and speed measuring instrument.</p>     <p>Two parameters were varied during testing: the detection sensitivity of the instrument and the distance of the passageways carried by the test vehicle at the sensors.</p>     <p>The test used as initial parameters in the detector plate the value AL / L = 0.32% at 20 cm away from the edge of the sensor.</p>     <p align="center"><a name="tab2"></a><img src="img/revistas/eia/n27/n27a09tab2.gif"></p>     <p align="center"><a name="fig4"></a><img src="img/revistas/eia/n27/n27a09fig4.gif"></p>     ]]></body>
<body><![CDATA[<p>We have made ten (10) passes with the test vehicle in each interval set, and observed the behavior of the instrument for this situation. The measuring speed was increased to 20 cm interval chain, thus determining the new distance at which the vehicle should pass the test. However, when the instrument was no longer able to measure the speed, a new sensitivity was settled, above the latter was set on the plate and another series of passages when the vehicle was performed. This procedure was repeated until the distance at which the instrument was no longer able to measure the speed of the last level of sensitivity that could be configured on the board model detector used in the test.</p>     <p>In the splash over simulation test was used four (4) levels of sensitivity and five (5) different  intervals were scored from the side of inductive sensors.</p>     <p>The instrument operating with the initial sensitivity did not detect the passage of the vehicle 20 cm far from the sensors, as shown in <b><a href="#tab3">Table 2</a></b>. Thus, according to the methodology established a new tuning was performed to make the instrument more sensitive, enabling the measurement of velocity in outer region of the sensors.</p>     <p align="center"><a name="tab3"></a><a href="img/revistas/eia/n27/n27a09tab3.gif" target="_blank">Table 2</a></p>     <p>The second sensitivity level used in the test was 0.04% (<b><a href="#tab4">Table 3</a></b>). In this configuration with the vehicle to passing at a distance of 20 cm from the sensor, the instrument was able to measure the speed of the test vehicle and issue the corresponding photographic record. With this sensitivity the instrument also detected the metal mass of the vehicle in all passages performed at 40 cm far from the edge of the sensor.</p>     <p align="center"><a name="tab4"></a><a href="img/revistas/eia/n27/n27a09tab4.gif" target="_blank">Table 3</a></p>     <p align="center"><a name="fig5"></a><img src="img/revistas/eia/n27/n27a09fig5.gif"></p>     <p>The third level of sensitivity used was 0.02%. At this stage of the trial, initially, the test  vehicle went to 60 cm from the edge of the loop. The instrument measured the speed and the photo was issued to a distance of 80 cm from the edge of the loop, as shown in <b><a href="#tab5">Table 4</a></b>.</p>     <p align="center"><a name="tab5"></a><a href="img/revistas/eia/n27/n27a09tab5.gif" target="_blank">Table 4</a></p>     <p align="center"><a name="fig6"></a><img src="img/revistas/eia/n27/n27a09fig6.gif"></p>     ]]></body>
<body><![CDATA[<p>The fourth and final level of sensitivity was 0.01% (<b><a href="#tab6">Table 5</a></b>). In order to find the maximum distance from the edge of the loop, where the metal mass is able to interfere significantly with the magnetic field generated around the sensors, the instrument was set to operate with the highest possible sensitivity. With this setting, the  instrument measured the velocity (<b><a href="#fig7">Figure 7</a></b>) with the test vehicle through a distance of at least 1 m from the edge of the sensor.</p>     <p align="center"><a name="tab6"></a><a href="img/revistas/eia/n27/n27a09tab6.gif" target="_blank">Table 5</a></p>     <p align="center"><a name="fig7"></a><img src="img/revistas/eia/n27/n27a09fig7.gif"></p>     <p>As expected, the maximum distance from the edge of the loop in which the metallic mass was able to significantly interfere in the magnetic field created around the sensors occurred with the instrument regulated to operate with the highest level of sensitivity possible. With this setting the instrument detected and measured speed (<a href="#fig4"><b>Figure 4</b></a>) of the test vehicle to 1meter at the edge of the tie (Monteiro, 2012).</p>     <p>This result is reasonable, since the vehicle crossing is considered in a way that increasing the distance away from the sensor implies a smaller amount of conductive metal mass in interaction with the local magnetic field. Additionally, the magnetic field in the region external to the sensor faces a gradual decrease over the existing ones nearby the sensors. The consequence of the association of these two conditions is that the presence of a vehicle in regions outside the sensor will cause a small variation in inductance of the circuit, compared to condition occurred with the crossing of a vehicle over the sensors. Thus, sensitive  settings are necessary in order one to able to detect these smaller changes.</p>     <p>Aiming to show how false detection can occur due to the splash over particularly critical  situations have been simulated with the aid of two test vehicles.</p>     <p>In these simulations the instrument was set to operate with the sensitivity level of 0.04%, thus being able to capture a passing vehicle up to 40 cm from the edge of the loop, as shown in <b><a href="#tab4">Table 3</a></b>.</p>     <p align="center"><a name="fig8"></a><img src="img/revistas/eia/n27/n27a09fig8.gif"></p>     <p align="center"><a name="fig9"></a><img src="img/revistas/eia/n27/n27a09fig9.gif"></p>     <p><b><a href="#fig5">Figure 5</a> </b>shows a vehicle in lane 1, where  the pair of sensors are installed, and the  other is in track 2. The vehicle 1 has lower speed then the  maximum velocity set in the instrument for the  purpose of detection, on the other hand, the second  vehicle in track 2 has speed above the limit speed  where the instrument can detect the violation.</p>     ]]></body>
<body><![CDATA[<p>The vehicle 1 according to the splash over could be identified as the holder of the  speed measured by the instrument, and the actual  excess of speeding was in reality in vehicle 2.</p>     <p>The usual photographic record, as shown in <a href="#fig6"><b>Figure 6</b></a>, makes it more feasible to false identification of the holder of the  vehicle speed. The zoom setting of the camera does not show  the image the other vehicle on the adjacent track  and that is generating the splash over.</p>     <p><b><font size="3">4 CONCLUSIONS</font></b></p>     <p>The splash over is a phenomenon inherent   when using inductive sensors for  monitoring excess   of speed. As described in this work, the  presence of   vehicles traveling in adjacent lanes can  cause false   detections or errors in the velocity  measurement.</p>     <p>The simulation showed that the instrument, when adjusted to operate at high levels of  sensitivity, was able to detect a vehicle traveling  outside the perimeter of the sensors. Such extreme  settings may be required for the detection of small  vehicles or high altitude from the ground.</p>     <p>The problem of over splash becomes more critical as the area of detection and  intensity of the magnetic field formed around the  sensors are dependent on particular conditions of  installation of each instrument. It is not possible to  establish a standard sensitivity setting that meets  all prototypes of a given instrument model.</p>     <p>The sensitivity adjustment performed on  the detector board can be touted as the most  relevant factor in the configuration of an  instrument. A less sensitive setting run the detector inhibit  measuring speed of vehicles traveling in the  adjacent lane, but with this setting the instrument would  find difficulty in capturing vehicles as motorcycles that  have reduced metal mass and distant from the  ground. In contrast, very sensitive adjustments  ensure the measurement of all types of vehicles, but  permit instrument to show false speed values.</p>     <p>Finding the balance that allows  satisfactory operation of the speed meter is not always  trivial. The instrument calibration must be  performed at installation and is usually performed  empirically.</p>     <p>Thus, after the installation or  maintenance, the speed meter can operate with  susceptibility, even if unintentionally, the phenomenon of splash  over.</p>     <p>There are ways to minimize the undesired effect of splash over.</p>     ]]></body>
<body><![CDATA[<p>The installation of sensors lagged, non installing sensors near of dividing  boundary and the adjacent bands graphical measurement  zone, which is the region of influence of the  magnetic field generated by the photographic  recording instrument are measures if used could  provide solutions for this anomaly.</p>     <p>Finally, it is important to emphasize that  this research was used in the refinement of  technical regulations metrology gauges speed of  vehicles in effect in Brazil.</p>     <p><b><font size="3">REFERENCES</font></b></p>     <!-- ref --><p>Andreoti, Marcel. <i>Inductive  sensing for automotive vehicles</i>. Curitiba: Technological Center Federal do  Paran&aacute;, 2001. 52 p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099892&pid=S1794-1237201700010000900001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>Coifman, Benjamin. <i>Lenght  classfication vehicle based</i> <i>on freeways form single  loop detectors. </i>Columbus: Nextrans, 2009. 13-14 p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099894&pid=S1794-1237201700010000900002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>Fullerton, Iris; Kell, James and Mills,  Milton. <i>Traffic</i> <i>Detector Handbook - Second  Edition</i>, Virginia: Federal Higway Administration, 1990. 18-19  p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099896&pid=S1794-1237201700010000900003&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>Klein, Lawrence; Gibson, David and Mills,  Milton. <i>Traffic</i> <i>Detector Handbook - Third  Edition</i>. Virginia:  Federal Higway Administration, 2006. 81-84 p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099898&pid=S1794-1237201700010000900004&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>Magalh&atilde;es, Hermes. <i>Analysis  of high-resolution magnetic</i> <i>profiles of the inductive  loop sensors for classification</i> <i>of vehicles</i>. Belo Horizonte: Federal  University of Minas  Gerais, 2008. 44-46 p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099900&pid=S1794-1237201700010000900005&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>Monteiro,  Silvio. <i>Study  on the inclusion of the measurement</i> <i>zone in legal control of  speed meters of automotive</i> <i>vehicles</i>. Rio de Janeiro: National  Institute of Metrology, Quality and Technology, 2012.  55-75 p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099902&pid=S1794-1237201700010000900006&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>Nishimoto, R&eacute;gis. <i>New  geometries inductive loop</i>. Curitiba: Technological University of Paran&aacute;, 2006. 4-6 p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099904&pid=S1794-1237201700010000900007&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>Reno  A&#38;E. <i>Operation manual reno AE -  model 222</i>. Reno: Reno  AE, 2006. 13-16 p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099906&pid=S1794-1237201700010000900008&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>Rizzotto,  Rodolfo. <i>Accidents  do not happen. </i>Rio de Janeiro: National School of Insurance, 2010. 56 p.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099908&pid=S1794-1237201700010000900009&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     <!-- ref --><p>World Health Organization. Road traffic  injuries. 2004: &#91;Accessed on May 2012&#93; Available at: &lt;<a href="www.who.int/features/2004/road_safety" target="_blank">www.who.int/features/2004/road_safety</a>&gt;    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3099910&pid=S1794-1237201700010000900010&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref -->.</p> </font>      ]]></body><back>
<ref-list>
<ref id="B1">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Andreoti]]></surname>
<given-names><![CDATA[Marcel]]></given-names>
</name>
</person-group>
<source><![CDATA[Inductive sensing for automotive vehicles]]></source>
<year>2001</year>
<page-range>52</page-range><publisher-loc><![CDATA[Curitiba ]]></publisher-loc>
<publisher-name><![CDATA[Technological Center Federal do Paraná]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B2">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Coifman]]></surname>
<given-names><![CDATA[Benjamin]]></given-names>
</name>
</person-group>
<source><![CDATA[Lenght classfication vehicle based on freeways form single loop detectors]]></source>
<year>2009</year>
<page-range>13-14</page-range><publisher-loc><![CDATA[Columbus ]]></publisher-loc>
<publisher-name><![CDATA[Nextrans]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B3">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Fullerton]]></surname>
<given-names><![CDATA[Iris]]></given-names>
</name>
<name>
<surname><![CDATA[Kell]]></surname>
<given-names><![CDATA[James]]></given-names>
</name>
<name>
<surname><![CDATA[Mills]]></surname>
<given-names><![CDATA[Milton]]></given-names>
</name>
</person-group>
<source><![CDATA[Traffic Detector Handbook]]></source>
<year>1990</year>
<edition>Second Edition</edition>
<page-range>18-19</page-range><publisher-loc><![CDATA[Virginia ]]></publisher-loc>
<publisher-name><![CDATA[Federal Higway Administration]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B4">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Klein]]></surname>
<given-names><![CDATA[Lawrence]]></given-names>
</name>
<name>
<surname><![CDATA[Gibson]]></surname>
<given-names><![CDATA[David]]></given-names>
</name>
<name>
<surname><![CDATA[Mills]]></surname>
<given-names><![CDATA[Milton]]></given-names>
</name>
</person-group>
<source><![CDATA[Traffic Detector Handbook]]></source>
<year>2006</year>
<edition>Third Edition</edition>
<page-range>81-84</page-range><publisher-loc><![CDATA[Virginia ]]></publisher-loc>
<publisher-name><![CDATA[Federal Higway Administration]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B5">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Magalhães]]></surname>
<given-names><![CDATA[Hermes]]></given-names>
</name>
</person-group>
<source><![CDATA[Analysis of high-resolution magnetic profiles of the inductive loop sensors for classification of vehicles]]></source>
<year>2008</year>
<page-range>44-46</page-range><publisher-loc><![CDATA[Belo Horizonte ]]></publisher-loc>
<publisher-name><![CDATA[Federal University of Minas Gerais]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B6">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Monteiro]]></surname>
<given-names><![CDATA[Silvio]]></given-names>
</name>
</person-group>
<source><![CDATA[Study on the inclusion of the measurement zone in legal control of speed meters of automotive vehicles]]></source>
<year>2012</year>
<page-range>55-75</page-range><publisher-loc><![CDATA[Rio de Janeiro ]]></publisher-loc>
<publisher-name><![CDATA[National Institute of Metrology, Quality and Technology]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B7">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Nishimoto]]></surname>
<given-names><![CDATA[Régis]]></given-names>
</name>
</person-group>
<source><![CDATA[New geometries inductive loop]]></source>
<year>2006</year>
<page-range>4-6</page-range><publisher-loc><![CDATA[Curitiba ]]></publisher-loc>
<publisher-name><![CDATA[Technological University of Paraná]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B8">
<nlm-citation citation-type="book">
<collab>Reno AE</collab>
<source><![CDATA[Operation manual reno A&#38;E - model 222]]></source>
<year>2006</year>
<page-range>13-16</page-range><publisher-loc><![CDATA[Reno ]]></publisher-loc>
<publisher-name><![CDATA[Reno AE]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B9">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Rizzotto]]></surname>
<given-names><![CDATA[Rodolfo]]></given-names>
</name>
</person-group>
<source><![CDATA[Accidents do not happen]]></source>
<year>2010</year>
<page-range>56</page-range><publisher-loc><![CDATA[Rio de Janeiro ]]></publisher-loc>
<publisher-name><![CDATA[National School of Insurance]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B10">
<nlm-citation citation-type="">
<collab>World Health Organization</collab>
<source><![CDATA[Road traffic injuries]]></source>
<year>2004</year>
</nlm-citation>
</ref>
</ref-list>
</back>
</article>
