ImageVerifierCode 换一换
格式:DOCX , 页数:12 ,大小:206.62KB ,
资源ID:833835      下载积分:3 金币
快捷下载
登录下载
邮箱/手机:
温馨提示:
快捷下载时,用户名和密码都是您填写的邮箱或者手机号,方便查询和重复下载(系统自动生成)。 如填写123,账号就是123,密码也是123。
特别说明:
请自助下载,系统不会自动发送文件的哦; 如果您已付费,想二次下载,请登录后访问:我的下载记录
支付方式: 支付宝    微信支付   
验证码:   换一换

加入VIP,免费下载
 

温馨提示:由于个人手机设置不同,如果发现不能下载,请复制以下地址【https://www.bingdoc.com/d-833835.html】到电脑端继续下载(重复下载不扣费)。

已注册用户请登录:
账号:
密码:
验证码:   换一换
  忘记密码?
三方登录: 微信登录   QQ登录  

下载须知

1: 本站所有资源如无特殊说明,都需要本地电脑安装OFFICE2007和PDF阅读器。
2: 试题试卷类文档,如果标题没有明确说明有答案则都视为没有答案,请知晓。
3: 文件的所有权益归上传用户所有。
4. 未经权益所有人同意不得将文件中的内容挪作商业或盈利用途。
5. 本站仅提供交流平台,并不能对任何下载内容负责。
6. 下载文件中如有侵权或不适当内容,请与我们联系,我们立即纠正。
7. 本站不保证下载资源的准确性、安全性和完整性, 同时也不承担用户因使用这些下载资源对自己和他人造成任何形式的伤害或损失。

版权提示 | 免责声明

本文(热释电红外传感器中英文对照外文翻译文献Word格式文档下载.docx)为本站会员(wj)主动上传,冰点文库仅提供信息存储空间,仅对用户上传内容的表现方式做保护处理,对上载内容本身不做任何修改或编辑。 若此文所含内容侵犯了您的版权或隐私,请立即通知冰点文库(发送邮件至service@bingdoc.com或直接QQ联系客服),我们立即给予删除!

热释电红外传感器中英文对照外文翻译文献Word格式文档下载.docx

1、可见光的波长通常在1 m以下,而1 m以上的光人眼是看不到的,但是可以通过适当的仪器对辐射的能量进行检测。当一些晶体受热时,在晶体两端将会产生数量相等而符号相反的电荷,这种由于热变化产生的电极化现象,被称为热释电效应。通常,晶体自发极化所产生的束缚电荷被来自空气中附着在晶体表面的自由电子所中和,其自发极化电矩不能表现出来。当温度变化时,晶体结构中的正负电荷重心相对移位,自发极化发生变化,晶体表面就会产生电荷耗尽,电荷耗尽的状况正比于极化程度,图1表示了热释电效应形成的原理。能产生热释电效应的晶体称之为热释电体或热释电组件,其常用的材料有单晶(LiTaO3 等)、压电陶瓷(PZT 等)及高分子薄

2、膜(PVFZ 等)2 当以LiTaO3为代表的热释电材料处于自极化状态时,吸收红外线入射波后,结晶的表面温度改变,自极化也发生改变,结晶表面的电荷变得不平衡,把这种不平衡电荷的电压变化取出来,便可测出红外线。热释电材料只有在温度变化时才产生电压,如果红外线一直照射, 则没有不平衡电压,一旦无红外线照射时,结晶表面电荷就处于不平衡状态,从而输出电压。热释电红外线传感器因红外光线的照射与遮挡得到或失去热量,从而产生电压输出。从原理上讲应与波长无关,但由热释电材料做成的传感器有一个透光窗,而透光窗的选材与波长有关系。如以SiO2为窗材的传感器,它可以透过几乎全部的可见光,而有的窗材只能通过4 m附近

3、波长的光,有的能透过6.1 m波长的光,有的能透过8 m14 m波长的光,所以使用不同的窗材就可确认是哪个波长的光产生的热。量子型的红外光探测器量子型的红外光探测器与红外光的波长有关,它的特点是灵敏度高,响应速度快,响应的灵敏度与红外线波长有关。每个入射光子产生的能量 E=hc/ =1124 式中,h普朗克常数,h=4.1410-15(evs)=6.62510-34(JS) c光速,c=31010cm/s 1 m红外光的能量为1.24eV,10 m红外光的能量为0.12eV,与可见光相比,红外线光的能量较小。量子型的红外传感器又分为光导电型和光电动势型两种。光导电型的组件材料有PbS、PbSe

4、、Hg、Cd、Te等,它是利用红外线照射时阻抗减少的特点来获取检测信号的;而光电动势型是在Ge、IrSb等半导体基片上形成PN结,当红外线照射时产生光电动势,Ge 的禁带宽度为0.6ev,Ge二极管对0.6 m和1.9 m的红外光较敏感,当入射红外光的波长在0.6 m1.9 m时,在PN结上形成的电动势随入射光量的增大而增大,从而经放大可输出探测电信号。热释电传感器热释电传感器利用的正是热释电效应,是一种温度敏感传感器。它由陶瓷氧化物或压电晶体组件组成,组件两个表面做成电极,当传感器监测范围内温度有 T的变化时,热释电效应会在两个电极上会产生电荷 Q,即在两电极之间产生一微弱电压 V。热释电红

5、外传感器和热电偶都是基于热电效应原理的热电型红外传感器不同的是热释电红外传感器的热电系数远远高于热电偶。结构图热释电红外传感器的结构及内部电路见图2所示。传感器主要有外壳、干涉滤光片、热释电组件PZT、场效应管FET等组成。滤光片人体辐射的红外线中心波长为910-um,而探测组件的波长灵敏度在0.220-um范围内几乎稳定不变。在传感器顶端开设了一个装有滤光镜片的窗口,这个滤光片可通过光的波长范围为710-um,正好适合于人体红外辐射的探测,而对其它波长的红外线由滤光片予以吸收,这样便形成了一种专门用作探测人体辐射的红外线传感器。热电组件将高热电材料制成一定厚度的薄片,并在它的两面镀上金属电极

6、,然后加电对其进行极 化,这样便制成了热释电探测元由于加电极化的电压是有极性的,因此极化后的探测元也是有正负极性的 内部的热电元由高热电系数的铁钛酸铅汞陶瓷以及钽酸锂硫酸三甘铁等,其极化强度 随温度的变化而变化为了抑制因自身温度变化而产生的干扰可以在工艺上将两个特征一致的热电元反向串联或接成差动平衡电路方式, 以抑制由于自身温度升高而产生的干扰。因而能以非接触式检测出物体放出的红外线能量变化,并将其转换为电信号输出 阻抗变换场效应管热释电红外传感器在结构上引入场效应管的目的在于完成阻抗变换由于热电元输出的是电荷信号,阻抗高达104M ,故引入的N沟道结型场效应管应接成共漏形式,即源极跟随器来完

7、成阻抗变换 由于它的输出阻抗极高,所以传感器中有一个场效应管进行阻抗变换。热释电效应所产生的电荷 Q会跟空气中的离子所结合而消失,当环境温度稳定不变时, T=0,传感器无输出。当人体进入检测区时,因人体温度与环境温度有差别,产生 T,则有信号输出;若人体进入检测区后不动,则温度没有变化,传感器也没有输出,所以这种传感器能检测人体或者动物的活动。选型参考目前常用的热释电红外传感器型号主要有P228、LHl958、LHI954、RE200B、KDS209、PIS209、LHI878、PD632等。热释电红外传感器通常采用3引脚金属封装,各引脚分别为电源供电端(内部开关管D极,DRAIN)、信号输出

8、端(内部开关管S极,SOURCE)、接地端(GROUND)。热释电红外传感器的主要工作参数有 工作电压(常用的热释电红外传感器工作电压范围为315V) 工作波长(通常为7.514 m) 源极电压(通常为0.41.1V,R=47k ) 输出信号电压(通常大于 2.0V) 红外模块使用注意事项:1、人体感应器模块属于高度敏感的器件,它对电源要求很高,必须经过良好的稳压滤波, 例如 9V 的层叠电池就可能因为内阻较大不能正常工作,建议客户用 LM7808 稳压芯片稳压后再通过 220UF 和 0.1UF 的电容滤波后供电。2 、模块不接负载时能正常工作,接上负载后工作紊乱,一种原因是因为电源容量很小

9、负载比较耗电,负载工作时引起的电压波动导致模块误动作,另一种原因是负载得电工作时会产生干扰,例如继电器或者电磁铁等感性负载会产生反向电动势,315M 发射板工作时会有电磁辐射等都会影响模块。解决办法如下:A、电源部分加电感滤波。B、采用负载和模块使用不同的电压的方法,例如:负载使用 24V 工作电压,模块使用 12V 工作电压,其间用 LM7812 三端稳压器隔离。C: 使用更大容量的电源。3 、人体感应器模块工作环境应该避免阳光、强光直接照射,若工作环境有强大的射频干扰, 可采用屏蔽措施。若遇有强烈气流干扰,关闭门窗或阻止对流。感应区尽量避免正对着发热电器和物体,以及容易被风吹动的杂物和衣物

10、 4、人体感应器模块必须装配在密封的盒里,否则一直会有输出信号。探头(PIR)与镜片有一聚焦距离,通常在2030mm 范围调整。5 、如果要求红外探测器的探测角度小于90 度时,可以用不透明胶纸遮挡镜片或裁剪缩小镜片来实现。6 、人体感应器模块采用双元探头,人体的手脚和头部运动方向与感应灵敏度有着密切的联系,如果设置安装不当,会影响感应效果。7 、模块中的探头(PIR)可以装焊在电路板的另一面。也可将探头用双芯屏蔽线延长,长度应在 2 米以内为好。结束语热释电红外传感器具有价格低廉、技术性能稳定、开发使用简单等特点,除了以上的监控报警和自动开关典型应用外,在众多其它领域有广泛应用,如自动开停的

11、空调机、饮水机、电视机、自动拍摄人和动物活动的摄像机或数码相机等,随着电子技术发展,热释电红外传感器必将更加广泛地应用在自动控制领域。Pyroelectric infrared sensorPrefacePyroelectric infrared sensor is a very potential applications of the sensor.It can detect people or animals, the infrared transmitter and converted into anelectrical signal output. As early as 1938,

12、 it was proposed detection using pyroelectric infrared radiation effect, but not taken seriously. Until the sixties, with the laser, infrared technology is developing rapidly, it has contributed tothe pyroelectric effect and research on pyroelectric crystals application development. In recent years,

13、 along with the rapid development of integrated circuit technology, as well as the characteristics of the sensor depth study of the relevant applicationspecific integrated circuit processing technology is also growing rapidly.This article first describes the principle of the pyroelectric sensor, and

14、 then describe the relevant ASIC processing technology.Pyroelectric effectIn nature, any more than the absolute temperature (-273K) objects will have infrared spectra, objects at different temperatures the wavelength of infrared energy released is not the same, so the level of infrared wavelengths i

15、s related to temperature, and radiation energy size and surface temperature.1m wavelength of visible light is usually less, but more than 1m light the human eye can not see, but can be an appropriate instrument to detect the energy oradiation.When some of the crystal is heated, the crystal will have

16、 an equal number of both ends of the opposite sign of charge, such as heat of changes in the polarization phenomenon, known as the pyroelectric effect. Typically, the crystals produced by the spontaneous polarization bound charge is attached to the air from the surface of free electrons in the cryst

17、al and in its spontaneous polarization electric moment can not bedemonstrated. When the temperature changes, positive and negative charges in the crystal structure of the relative center of gravity shifts, the spontaneous polarization changes, the crystal surface will have run out of charge, charge

18、depletion is proportional to the polarization degree of the situation, Figure 1 shows the pyroelectric The principle effect of the formation.Pyroelectric effect can produce a crystal or call the pyroelectric pyroelectric body components, the material commonly used in single crystal (LiTaO3, etc.), p

19、iezoelectric ceramic (PZT, etc.) and polymer film (PVFZ, etc.) 2When represented LiTaO3 pyroelectric material is self-polarized state, the absorption of infrared incident, the crystallization of the surface temperature change, since the polarization has changed, crystal surface charge becomes imbala

20、nced, the imbalance taken out of charge voltage can be measured by infrared. Pyroelectric materials produced only when the temperature changes the voltage, if the infrared radiation has been, there is no imbalance in voltage, if no infrared radiation, the crystal surface charge on the in an unbalanc

21、ed state, so the output voltagePyroelectric infrared sensors, infrared light irradiation due to gain or lose heat and shelter, resulting in voltage output. In principle should be independent of the wavelength, but the material made by the pyroelectric sensor has a light transmission window, the tran

22、slucent windows and wavelength selection of a relationship. To SiO2 as the window material, such as sensors, it can almost all visible light, while others near the window material can only 4m wavelength of light, and some wavelengths of light through 6.1m, and some through 8m 14m wavelength of light

23、, so use a different window materials which can be confirmed that the heat generated by the wavelength of light.Quantum-type infrared detectorQuantumponse, response sensitivity and infrared wavelength. The energy generated by each incident photonE = hc / = 1124Where, h - Planck constant, h = 4.14 10

24、-15 (evs) = 6.625 10-34 (JS) c - the speed of light, c = 3 1010cm / s1m infrared light energy 1.24eV, 10m infrared light energy of 0.12eV, compared with the visible light, infrared light energy smaller. Quantum-type infrared sensor light conductive type and is divided into two kinds of light force.

25、Components of light conductive material PbS, PbSe, Hg, Cd, Te, etc., it is the use of infrared radiation to reduce the characteristics of impedance detection signal to obtain; and light force type is in Ge, IrSb formed on a substrate such as semiconductor PN Results, when the infrared radiation gene

26、rated when the light force, Ge band gap for the 0.6ev, Ge diode of 0.6m and 1.9m more sensitive to infrared light, infrared light when the wavelength of the incident in the 0.6m 1.9m, in the PN junction force formed with the increase of the amount of incident light, thereby detecting amplified outpu

27、t signal.Pyroelectric sensorPyroelectricsensorusingthepyroelectriceffectis,isa temperature-sensitive sensor. It consists of oxides or ceramic piezoelectric crystal components, the component made of two surface electrodes, when the temperature within the sensor monitoring the change T, the pyroelectr

28、ic effect in the two electrodes will produce the charge Q, ie between two electrodes in a weak voltage V.Pyroelectric infrared sensors and thermocouples are based on the principle of thermoelectric thermoelectric infrared sensors. Different pyroelectric infrared sensors is the thermoelectric coeffic

29、ient is much higher than the thermocouple.ChartPyroelectric infrared sensor structure and the internal circuit shown in Figure2.Sensors are mainly case, interference filters, pyroelectric component PZT,FET, FET and other components.FilterHuman central wavelength of infrared radiation 9 10 - um, the

30、wavelength sensitivity of the detection component in 0.2 20 - um range is almost constant. The top of the sensor chip has opened a window with filter, this filter through the wavelength range of 7 10 - um, just right for the detection of infrared radiation inthe human body, while the other infrared wavelengths by the filter film to be absorbed, thus forming a special body for detection of infrared radiation sensor.Thermoelectric componentsThermoelectric materials will be a certai

copyright@ 2008-2023 冰点文库 网站版权所有

经营许可证编号:鄂ICP备19020893号-2