超声测距相关毕业设计外文资料翻译
超声测距系统设计外文翻译

摘要:超声测距系统技校在工业场车辆导航水声工程等领域都具有了广泛的应用价值,目前已应用于物理测量,机器人自动导航以及空气中与水下的目标探测、识别定位等场合,因此,深入研究超声的探测理论和方法具有重要的实践意义,为了进一步提高测量的精确度,满足工程人员对测量精度测距量程和测距仪使用的要求,本文研制了一套基于单片机的使拱式超声测距系统。
关键词:超声波测距仪单片机1、前言随着科技的发展,人们生活水平的提高,城市发展建设加快,城市给排水系统也有较大发展,其状况不断改善,但是,由于历史原因合成时间性的许多不可预见因素,城市给排水系统,特别是排水系统往往落后于城市建设,因此,经常出现开挖已经建设好的建筑设施来改造排水系统的现象。
城市污水给人们带来的困扰,因此箱的排污疏通对大城市给排水系统污水理,人们生活舒适显得非常重要。
而设计研制箱涵排水疏通移动机器人的自动控制系统,保证机器人在箱涵中自由排污疏通,是箱涵排水系统疏通机器人的设计研制的核心部分,控制系统核心部分就是超声波测仪的研制。
因此,设计好的超声波测距仪就显得非常重要了。
1.1课题背景随着经济的发展与汽车科学技术的进步,公路交通呈现出行驶高速化、车流密集化和驾驶员非职业化的趋势。
同时,随着汽车工业的飞速发展,汽车的产量和保有量都在急剧增加。
但公路发展、交通管理却相对落后,导致了交通事故与日剧增,城市里尤其突出。
智能交通系统ITS是目前世界上交通运输科学技术的前沿技术,它在充分发挥现有基础设施的潜力,提高运输效率,保障交通安全,缓解交通赌塞,改善城市环境等方面的卓越效能,已得到各国政府的广泛关注。
中国政府也高度重视智能交通系统的研究开发与推广应用。
汽车防撞系统作为ITS 发展的一个基础,它的成功与否对整个系统有着很大的作用。
从传统上说,汽车的安全可以分为两个主要研究方向:一是主动式安全技术,即防止事故的发生,该种方式是目前汽车安全研究的最终目的;二是被动式安全技术,即事故发生后的乘员保护。
数字身高体重测量仪论文

学科分类号0805本科毕业设计题目(中文):体重及超声波远距测高仪-----体重检测(英文):Weight and ultrasonic distance altimeter-----weight detection姓名学号院(系)工程与设计学院专业、年级指导教师兆仁二〇一四年五月师大学本科毕业设计诚信声明本人重声明:所呈交的本科毕业设计,是本人在指导老师的指导下,独立进行研究工作所取得的成果,成果不存在知识产权争议,除设计中已经注明引用的容外,本设计不含任何其他个人或集体已经发表或撰写过的作品成果。
对本设计的研究做出重要贡献的个人和集体均已在文中以明确方式标明。
本人完全意识到本声明的法律结果由本人承担。
本科毕业设计作者签名:二〇一四年五月二十日师大学本科毕业设计任务书XX师大学工程与设计学院指导教师指导毕业设计情况登记表师大学本科毕业设计评审表优秀,80—89分记为良好,70—79分记为中等,60—69分记为及格,60分以下记为不及格。
若译文成绩为零,则不计总成绩,评定等级记为不及格。
师大学本科毕业设计答辩记录表目录摘要1Abstract21 引言31.1 选题背景及目的31.2 总体方案设计与论证41.2.1 设计任务41.2.2 设计容41.2.3 方案论证与选择52 硬件电路设计62.1 主控电路62.2 超声波测高模块电路82.2.1 超声波传感器及其测高原理82.2.2 超声波传感器电气参数及其时序图92.3 压力传感器称重模块112.3.1 压力传感器112.3.2 称重AD转换芯片132.3.3 称重部分AD转换基本原理152.3.4 称重传感器重量标定162.4 LCD1602液晶显示模块172.4.1 LCD1602介绍172.4.2 LCD1602主要技术参数及其时序图193 系统软件设计213.1 单片机初始化程序设计213.2 超声波测高模块程序设计223.3 测体重程序设计243.4 液晶显示模块程序设计24 结论26参考文献27附录28致58体重及超声波远距离测高仪-----体重检测专业:电子信息工程年级:2010级:练摘要在如今体检过程中,身高和体重是必要的测量部分。
超声波测距外文文献加中文翻译毕业设计

附录A 英文原文ULTASONIC RANGING IN AIRG. E. Rudashevski and A. A. GorbatovOne of the most important problems in instrumentation technology is the remote,contactless measurement of distances in the order of 0.2 to 10 m in air.Such a problem occurs,for instance,when measuring the relativethre edimensional position of separate machine members or structural units.Interesting possibilities for its solution are opened up by utilizing ultrasonic vibrations as an information carrier.The physical properties of air,in which the measurements are made,permit vibrations to be employed at frequencies up to 500 kHz for distances up to 0.5 m between a member and the transducer,or up to 60 kHz when ranging on obstacles located at distances up to 10 m.The problem of measuring distances in air is somewhat different from other problems in the a -pplication of ultrasound.Although the possibility of using acoustic ranging for this purpose has been known for a long time,and at first glance appears very simple,nevertheless at the present time there are only a small number of developments using this method that are suitable for practical purposes.The main difficulty here is in providing a reliable acoustic three-dimensional contact with the test object during severe changes in the air's characteristic.Practically all acoustic arrangements presently known for checking distances use a method of measuring the propagation time for certain information samples from the radiator to the reflecting member and back.The unmodulated acoustic(ultrasonic)vibrations radiated by a transducer are not in themselves a source of information.In order to transmit some informational communication that can then be selected at the receiving end after reflection from the test member,the radiated vibrations must be modulated.In this case the ultrasonic vibrations are the carrier of the information which lies in the modulation signal,i.e.,they are the means for establishing the spatial contact between the measuring instrument and the object being measured.This conclusion,however,does not mean that the analysis and selection of parameters for the carrier vibrations is of minor importance.On the contrary,the frequency of the carrier vibrations is linked in a very close manner with the coding method for the informational communication,with the passband of the receiving and radiating elements in the apparatus,with the spatial characteristics of the ultrasonic communication channel,and with the measuring accuracy.Let us dwell on the questions of general importance for ultrasonic ranging in air,namely:on the choice ofa carrier frequency and the amount of acoustic power received.An analysis shows that with conical directivity diagrams for the radiator and receiver,and assuming thatthe distance between radiator and receiver is substantially smaller than the distance to the obstacle,theamount of acoustic power arriving at the receiving area Pr for the case of reflection from an ideal planesurface located at right angles to the acoustic axis of the transducer comes towhere Prad is the amount of acoustic power radiated,B is the absorption coefficient for a plane wave inthe medium,L is the distance between the electroacoustic transducer and the test me -mber,d is the diameterof the radiator(receiver),assuming they are equal,and c~is the angle of the directivity diagram for theelectroacoustic transducer in the radiator.Both in Eq.(1)and below,the absorption coefficient is dependent on the amplitude and not on theintensity as in some works[1],and therefore we think it necessary to stress this difference.In the various problems of sound ranging on the test members of machines and structures,therelationship between the signal attenuations due to the absorption of a planewave and due to thegeometrical properties of the sound beam are,as a rule,quite different.It must be pointed out that the choiceof the geometrical parameters for the beam in specific practical cases is dictated by the shape of thereflecting surface and its spatial distortion relative to some average position.Let us consider in more detail the relationship betweenthe geometric and the power parameters ofacoustic beams for the most common cases of ranging on plane and cylindrical structural members.It is well known that the directional characteristic W of a circular piston vibrating in an infinite baffle is afunction of the ratio of the piston's diameter to the wavelength d/λ as found from the following expression:(2)where Jl is a Bessel function of the first order and α is the angle between a normal to the piston and aline projected from the center of the piston to the point of observation(radiation).From Eq.(2)it is readily found that a t w o-t o-o n e reduction in the sensitivity of a radiator with respectto sound pressure will occur at the angle(3)For angles α≤20.Eq.(3)can be simplified to(4) where c is the velocity of sound in the medimaa and f is the frequency of the radiated vibrations.It follows from Eq.(4)that when radiating into air where c=330 m/s e c,the necessary diameter of the radiator for a spedfied angle of the directivity diagram at the 0.5 level of pressure taken with respect to the fdc 76.05.0≈αaxis can befound to be(5)where disincm,f is in kHz,and α is in degrees of angle.Curves are shown in Fig.1 plotted from Eq.(5)for six angles of a radiator's directivity diagram.The directivity diagrm needed for a radiator is dictated by the maximum distance to be measured and bythe spatial disposition of the test member relative to the other structural members.In order to avoid theincidence of signals reflected from adjacent members onto the acoustic receiver,it is necessary to provide asmall angle of divergence for the sound beam and,as far as possible,a small-diameter radiator.These tworequirements are mutually inconsistent since for a given radiation frequency a reduction of the beam'sdivergence angle requires an increased radiator diameter.In fact,the diameter of the"sonicated"spot is controlled by two variables,namely:the diameter of theradiator and the divergence angle of the sound beam.In the general case the minimum diameter ofthe"sonicated"spot Dmin on a plane surface normally disposed to the radiator's axis is given by(6)where L is the least distance to the test surface. The specified value of Dmin corresponds to a radiator with a diameter(7)As seen from Eqs.(,6)and(7),the minimum diameter of the"sonieated"spot at the maximum requireddistancecannot be less than two radiator diameters.Naturally,with shorter distances to the obstacle the sizeof the"sonicated" surface is less.Let us consider the case of sound ranging on a cylindrically shaped object of radius R.The problem is to measure the distance from the electroacoustic transducer to the side surface of the cylinderwith its various possible displacements along the X and Y axes.The necessary angleαof the radiator'sdirectivity diagram is given in this case by the expression(8) whereα is the value of the angle for the directivity diagram,Ymax is the maximum displacement of the cylinder's center from the acoustic axis,and Lmin is the minimum distance from the center of theelectroacoustic transducer to the reflecting surface measured along the straight line connecting the center ofthe m e m b e r with the center of the transducer.It is clear that when measuring distance,the"running"time of the information signal is controlled by thefd α1400≈fcL d 5.1=fcLD 6min =min maxarcsinL R y +≥αlength of the path in a direction normal to the cylinder's surface,or in other words,the measure distance isalways the shortest one.This statement is correct for all cases of specular reflection of the vibrations from thetest surface.The simultaneous solution of Eqs.(2)and(8)when W=0.5 leads to the following expression:(9) In the particular case where the sound ranging takes place in air having c=330 m/sec,and on theasstunption that L min <<R,the necessary d i a m e t e r of a unidirectional piston radiator d can be found fromthe fomula (10) where d is in cm and f is in kHz. Curves are shown in Fig.2 for determining the necessary diameter of the radiator as a function of theratio of the cylinder's radius to the maximum displacement from the axis for four radiation frequencies.Alsoshown in this figure is the directivity diagram angle as a function of R and Y rnax for four ratios of m i n i m u mdistance to radius.The ultrasonic absorption in air is the second factor in determining the resolution of ultrasonic rangingdevices and their range of action.The results of physical investigations concerning the measurement ofultrasonic vibrations air are given in[1-3].Up until now there has been no unambiguous explanation of thediscrepancy between the theoretical and expe -rimental absorption results for ultrasonic vibrations inair.Thus,for frequencies in the order of 50 to 60 kHz at a temperature of+25oC and a relative humidity of37%the energy absorption coefficient for a plane wave is about 2.5dB/m while the theoretical value is 0.3 dB/m.The absorption coefficient B as a function of frequency for a temperature of+25o Cand a humidity of37%according to the data in[2]can be described by Table 1.The absorption coefficient depends on the relative humidity.Thus,for frequencies in the order of 10 to20kHz the highest value of the absorption coefficient occurs at 20%humidity[3],and at 40%humidity theabsorption is reduced by about two to one.For frequencies in the order of 60 kHz the maximum absorptionoccurs at 30.7o humidity,dropping when it is increased to 98% or lowered to 10%by a factor of approximatelyfour to one.The air temperature also has an appreciable effect on the ultrasonic absorption[1].When thetemperature of the medium is increased from+10 to+30,the absorption for frequencies between 30 and 50kHz increases by about three to one.Taking all the factors noted above into account we arrive at the following approximate values for theabsorption coefficient:at a frequency of 60 kHz /3min =0.15 m -1 and~max=0.5-1;at a frequency of 200 ()maxmin 76.0y L R d +=λmax25fy R d ≈kHz/~min=0.6 m -1 and B max =2 m -1.(11)The values for the minimum~min and rnaxil-num~max"transmittance"coefficients were obtained in thea bsence of aerosols and rain.Their difference is the result of the possible variations in temperature over therange from -3 0 to+50~and in relative hmnidity over the range from 10 to 98%.The overall value ofthe"transmittance"is obtained by multiplying the values of g and 0 for given values of L,f,and d.L I T E R A T U R E C I T E DMoscow(1957).Moscow(1960).附录B 中文翻译在空气中超声测距G. E. Rudashevski and A. A. Gorbatov在仪器技术中远程是最重要的一个问题。
超声波测距系统外文文献翻译

=======大学本科生毕业设计外文文献及中文翻译文献题目: ULTRASONIC RANGING SYSTEM 文献出处: United States Patent译文题目:超声波测距系统学生:指导教师:专业班级:自动化11-4学号: 110601140416电气信息工程学院2014年5月1日超声波测距系统摘要超声波测距系统,是指选择性地激励一个变压器,使之产生换能器驱动信号。
超声换能器发射的超声波脉冲用于响应驱动信号然后接收到一个在超声波信号发出之后的回波信号。
分路开关接在变压器的绕组上,当超声波信号的传输在允许的近距离范围内达到一个稳定的等级,分路开关选择性的闭合来阻止蜂鸣器报警。
第1章发明背景像在宝丽来相机中应用的可用范围测试系统,它们都是准确而且可靠的,但都不适用于近距离测距,举个例子,2到3英寸的距离内就不适用,所以他们在9英寸甚至更远的距离测距是可靠的。
它们可以应用在很多的应用程序中,但不适用于可移动机器人领域内。
机器人通常必须通过门口只有两三英寸的间隙,如果当可移动机器人被操作于避障模式下通过狭小空间,可能机器人的规避路径过于狭窄,此外,规避动作应该使偏指定的路径距离最小化。
近距离测距不用于超声波系统的一个原因是,近距离输出脉冲输出太长以至于它重叠在回波脉冲上,即使输出脉冲缩短,输出脉冲仍然重叠回波脉冲,因为声音紧跟着输出脉冲。
备中产生的回波信号脉冲的范围为100毫伏,但设置传感器响应所必需的电路回声脉冲是大约150伏到300伏之间。
因此即使是最小的声波也会盖过回声信号。
事实上,dual-diode钳位电路用于将150伏降低到二极管的击穿电压,即0.7伏特。
但是这700毫伏足以盖过100毫伏的回波信号。
目前系统需要50毫秒将300伏特的峰值发射电压降到0.7伏特,且额外需要500到600毫秒的时间将它稳定在1毫伏范围。
第2章发明总结本发明可以提供一种改进的超声波测距系统。
本发明也可以提供一个改进的多通道超声波测距系统。
超声波测距外文翻译

超声波测距摘要:本演示处理了测量距离的超声波传感器在当前环境中的准确性。
作为一个测量传感器的选择SFR08型配备了允许寻址的I ²C 通信接口。
这一事实使得创建传感器阵列变得简单。
控制和可视化系统是基于PC PC。
NI USB 8451是作为通信卡使用的。
验证测量的目标是确定实际的传感器精度,特别是当测量较长的距离。
当评估传感器的精度时,不包括在所测量的数据的温度补偿。
关键词:超声波传感器,I ²C 通信接口,虚拟仪器1 1 简介简介超声波传感器通常用于自动化的任务来测量距离,位置变化,电平测量,如存在检测器或在特殊应用中,例如,当测量透明材料的纯度。
它们是基于测量超声波的传播时间的原则。
这一原则确保可靠的检测是独立的颜色渲染的对象或其表面的设计和类型。
它可以可靠地检测甚至液体,散装材料,透明物体,玻璃等材料。
他们使用的另一个参数是他们在侵略性的环境中使用,不是非常敏感的污垢和测量距离的可能性。
超声波传感器在许多机械设计中被制造。
对于实验室用途,用于发射器和接收器单独或在一个单一的简单的住房,对于工业用途,往往建造坚固的金属外壳。
有些类型允许您使用电位计或数字来调整灵敏度。
此外,输出可以在统一的版本中或直接以数字形式的模拟信号直接中。
就传感器来说,可以通过通信接口连接到PC ,它是可以设置所有传感器的工作范围和测量距离的详细参数。
2 2 超声测量超声测量超声对环境中的声音具有相似的传播特性。
这是机械振动的粒子环境。
超声波可以在气体、液体和固体中传播。
对于超声波通常被认为是一个频率高于20千赫的声音。
千赫的声音。
根据超声波的用途可以分为两类: 主动超声:当应用表现出物理或化学效应。
生成的输出达到更高的值。
超声波用于清洁,焊接,钻孔等。
被动超声;输出是在低得多(通常是小)值产生的对比度。
他的主要应用领域是测量距离,检测材料的缺陷和材料的厚度,测量液体和气体的流量,以及医疗保健的诊断。
超声测距外文-超声波距离和速度利用互相关方法对LPM信号测量

Ultrasonic distance and velocity measurement using a pair of LPM signals for cross-correlation method:Improvement of Doppler-shift compensation and examination of Doppler velocity estimation超声波距离和速度利用互相关方法对LPM信号测量:多普勒频移补偿和多普勒速度估计检测的改进数据来源Elsevier Journal Elsevier期刊刊物名Ultrasonics, 2012, Vol.52 (7), pp.873-879 超声波,2012,卷(7),pp.873-879 作者Shinnosuke Hirata, Minoru Kuribayashi Kurosawashinnosuke平田,稔栗林黑泽明单位机械工程与智能系统1,信息工程学院,电子通信,1-5-1 chofugaoka e4-329,,,布,东京182-8585大学,日本信息处理系,跨学科研究生科学与工程学院,东京工业大学,4259首席人事官g2-32,长津田,绿区,横滨,神奈川226-8502,日本AbstractReal-time distance measurement of a moving object with high accuracy and high resolution using an ultrasonic wave is difficult due to the influence of the Doppler effect or the limit of the calculation cost of signal processing. An over-sampling signal processing method using a pair of LPM signals has been proposed for ultrasonic distance and velocity measurement of moving objects with high accuracy and high resolution. The proposed method consists of cross correlation by single-bit signal processing, high-resolution Doppler velocity estimation with wide measurement range and low-calculation-cost Doppler-shift compensation. The over-sampling cross-correlation function is obtained from cross correlation by single-bit signal processing with low calculation cost. The Doppler velocity and distance of the object are determined from the peak interval and peak form in the cross-correlation function by the proposed method of Doppler velocity estimation and Doppler-shift compensation. In this paper, the proposed method of Doppler-shift compensation is improved. Accuracy of the determined distance was improved from approximately within ±140 μm in the previous method to approximately within ±10μm in computer simulations. Then, the proposed method of Doppler velocity estimation is evaluated. In computer simulations, accuracy of the determined Doppler velocity and摘要实时测量移动物体的高精度和高分辨率超声波存在的多普勒效应或信号处理的计算成本的限制的影响。
(完整版)超声波测距仪学士毕业设计

超声波测距仪毕业论文中文摘要电子测距仪要求测量范围在50cm~500cm,测量精度1cm,测量时与被测物体无直接接触,能够清晰稳定地显示测量结果。
由于超声波指向性强,能量消耗缓慢,在介质中传播的距离较远,因而超声波经常用于距离的测量。
如测距仪和物位测量仪等都可以通过超声波来实现。
超声波测距器,可以应用于汽车倒车、建筑施工工地以及一些工业现场的位置监控,也可用于液位、井深、管道长度的测量等场合。
利用超声波检测往往比较迅速、方便、计算简单、易于做到实时控制,并且在测量精度方面能达到工业实用的要求。
因此在移动机器人的研制上也得到了广泛的应用。
我的超声波测距仪设计采用74hc04反相器和CX20106搭接电路实现了超声波的发射与接收。
采用AT89C51单片机为该测距仪的控制核心,此设计易于调试,成本低廉,具有很强的实用价值和良好的市场前景。
关键词:超声波传感器,单片机,测距仪ABSTRACTElectronic distance measurement instrument for measurement in the range of 20cm-2.5m, precision 1cm, with the measurement of the measured object without direct contact, can clearly demonstrate the stability of the measurement results. Because of the strong point of ultrasonic energy consumption, slow, medium of communication in the longer distance, which are often used for ultrasonic distance measurement. Such as the range finder and level measurement and so on can be achieved by ultrasound. Ultrasonic ranging, can be applied to car parking, construction sites and some industrial site location monitoring, and can also be used for liquid level, depth, pipe length measurement occasions. Use of ultrasonic testing is often more rapid, convenient, simple, easy to achieve real-time control, and measurement accuracy can meet the practical requirements of industry. In the mobile robot has been developed on a wide range of applications. My car anti-collision anti-theft alarm system design using 74hc04inverter and CX20106lap circuit to realize the ultrasonic transmitter and receiver. Using AT89C51 SCM as the control core of the range finder, this design easy debugging, low cost, has the very strong practical value and good market prospects. Key words: ultrasonic sensor, single chip microcomputer, range finder,目录第一章绪论 .............................................................................................................................................. - 1 - 1.1 设计项目概述 ..................................................................................................................................... - 1 - 1.2 设计要求 ............................................................................................................................................. - 1 - 1.3 超声波测距原理 ................................................................................................................................. - 1 - 第二章超声波测距仪的内容及意义 ...................................................................................................... - 3 - 2.1 超声波测距仪的意义 ......................................................................................................................... - 3 - 2.2超声波测距仪的内容 .......................................................................................................................... - 3 - 第三章系统方案选择 .............................................................................................................................. - 3 - 3.1 方案一 ................................................................................................................................................. - 4 - 3.2 方案二 ................................................................................................................................................. - 4 - 3.3 方案确定 ............................................................................................................................................. - 4 - 第四章系统硬件电路设计 ...................................................................................................................... - 4 - 4.1单片机模块 .......................................................................................................................................... - 4 -4.1.1 AT89C51标准功能 .................................................................................................................. - 5 -4.1.2管脚说明................................................................................................................................... - 6 - 4.2超声波谐振频率调理电路模块 .......................................................................................................... - 7 - 4.3超声波回路接收处理电路模块 .......................................................................................................... - 8 - 4.4数码管显示模块 .................................................................................................................................. - 8 - 第五章系统软件程序设计 ...................................................................................................................... - 9 -5.1 超声波测距程序设计 ......................................................................................................................... - 9 - 5.2 超声波测距流程图 ........................................................................................................................... - 10 - 第六章系统软硬件调试 ........................................................................................................................ - 10 -6.1 硬件调试 ........................................................................................................................................... - 10 - 6.2 软件调试 ........................................................................................................................................... - 11 - 6.3 测试结果 ........................................................................................................................................... - 11 - 第七章调试中遇到的问题 .................................................................................................................... - 11 -7.1 发射接收时间对测量精度的影响分析 ........................................................................................... - 11 - 7.2 当地声速对测量精度的影响分析 ................................................................................................... - 12 - 总结 ........................................................................................................................................................ - 13 - 参考文献 .................................................................................................................................................. - 14 -附录A ....................................................................................................................................................... - 0 - 附录B ........................................................................................................................................................ - 0 - 致谢 ........................................................................................................................................................ - 6 -第一章绪论声波在其传播介质中被定义为纵波。
毕业设计论文 外文文献翻译 超声波测距 中英文对照

毕业设计论文外文文献翻译超声波测距中英文对照The Circuit Design of UltrasonicRanging System超声波测距系统的电路设计Ultrasonic Distance Meter超声波测距仪姓名:专业: 测控技术与仪器学号: 2007071071指导教师姓名,职称,:The Circuit Design of Ultrasonic Ranging SystemThis article described the three directions (before, left, right) ultrasonic ranging system is to understand the front of the robot, left and right environment to provide a movement away from the information. (Similar to GPS Positioning System)A principle of ultrasonic distance measurement1, the principle of piezoelectric ultrasonic generatorPiezoelectric ultrasonic generator is the use of piezoelectriccrystal resonators to work. Ultrasonic generator, the internal structure as shown in Figure 1, it has two piezoelectric chip and a resonance plate. When it's two plus pulse signal, the frequency equal to the intrinsic piezoelectric oscillation frequency chip, the chip will happen piezoelectric resonance, and promote the development of plate vibrationresonance, ultrasound is generated. Conversely, if the two are notinter-electrode voltage, when the board received ultrasonic resonance,it will be for vibration suppression of piezoelectric chip, the mechanical energy is converted to electrical signals, then it becomes the ultrasonic receiver.2, the principle of ultrasonic distance measurementUltrasonic transmitter in a direction to launch ultrasound, in the moment to launch the beginning of time at the same time, the spread of ultrasound in the air, obstacles on his way to return immediately, the ultrasonic reflected wave received by the receiver immediately stop the clock. Ultrasound in the air as the propagation velocity of 340m / s, according to the timer records the time t, we can calculate the distance between the launch distance barrier (s), that is: s = 340t / 2 Ultrasonic Ranging System for the Second Circuit DesignSystem is characterized by single-chip microcomputer to control the use of ultrasonic transmitter and ultrasonic receiver since the launch from time to time, single-chip selection of 8751, economic-to-use, and the chip has 4K of ROM, to facilitate programming. Circuit schematic diagram shown in Figure 2. Draw only the front range of the circuit wiring diagram, left and right in front of Ranging circuits and the same circuit, it is omitted.1,40 kHz ultrasonic pulse generated with the launchRanging system using the ultrasonic sensor of piezoelectric ceramic sensors UCM40, its operating voltage of the pulse signal is 40kHz, whichby the single-chip implementation of the following procedures to generate.puzel: mov 14h, # 12h; ultrasonic firing continued 200mshere: cpl p1.0; output 40kHz square wavenop;nop;nop;djnz 14h, here;retRanging in front of single-chip termination circuit P1.0 input port, single chip implementation of the above procedure, the P1.0 port in a40kHz pulse output signal, after amplification transistor T, the drive to launch the first ultrasonic UCM40T, issued 40kHz ultrasonic pulse, and the continued launch of 200ms. Ranging the right and the left side of the circuit, respectively, then input port P1.1 and P1.2, the working principle and circuit in front of the same location.2, reception and processing of ultrasonicUsed to receive the first launch of the first pair UCM40R, the ultrasonic pulse modulation signal into an alternating voltage, the op-amp amplification IC1A and after polarization IC1B to IC2. IC2 is locked loop with audio decoder chip LM567, internal voltage-controlledoscillator center frequency of f0 = 1/1.1R8C3, capacitor C4 determine their target bandwidth. R8-conditioning in the launch of the carrier frequency on the LM567 input signal is greater than 25mV, the outputfrom the high jump 8 feet into a low-level, as interrupt request signals to the single-chip processing.Ranging in front of single-chip termination circuit output port INT0 interrupt the highest priority, right or left location of the output circuit with output gate IC3A access INT1 port single-chip, whilesingle-chip P1.3 and P1. 4 received input IC3A, interrupted by the process to identify the source of inquiry to deal with, interruptpriority level for the first left right after. Part of the source codeis as follows:receive1: push pswpush accclr ex1; related external interrupt 1jnb p1.1, right; P1.1 pin to 0, ranging from right to interrupt service routine circuitjnb p1.2, left; P1.2 pin to 0, to the left ranging circuit interrupt service routinereturn: SETB EX1; open external interrupt 1pop accpop pswretiright: ...; right location entrance circuit interrupt serviceroutineAjmp Returnleft: ...; left Ranging entrance circuit interrupt service routineAjmp Return4, the calculation of ultrasonic propagation timeWhen you start firing at the same time start the single-chipcircuitry within the timer T0, the use of timer counting function records the time and the launch of ultrasonic reflected wave received time. When you receive the ultrasonic reflected wave, the receivercircuit outputs a negative jump in the end of INT0 or INT1 interrupt request generates a signal, single-chip microcomputer in response to external interrupt request, the implementation of the external interrupt service subroutine, read the time difference, calculating the distance . Some of its source code is as follows:RECEIVE0: PUSH PSWPUSH ACCCLR EX0; related external interrupt 0MOV R7, TH0; read the time valueMOV R6, TL0?CLR CMOV A, R6SUBB A, # 0BBH; calculate the time differenceMOV 31H, A; storage resultsMOV A, R7SUBB A, # 3CHMOV 30H, ASETB EX0; open external interrupt 0POP ACCPOP PSWRETIFourth, the ultrasonic ranging system software designSoftware is divided into two parts, the main program and interrupt service routine, shown in Figure 3 (a) (b) (c) below. Completion of the work of the main program is initialized, each sequence of ultrasonic transmitting and receiving control.Interrupt service routines from time to time to complete three ofthe rotation direction of ultrasonic launch, the main external interrupt service subroutine to read the value of completion time, distance calculation, the results of the output and so on.V. CONCLUSIONSRequired measuring range of 30cm ~ 200cm objects inside the plane to do a number of measurements found that the maximum error is 0.5cm, and good reproducibility. Single-chip design can be seen on the ultrasonic ranging system has a hardware structure is simple, reliable, small features such as measurement error. Therefore, it can be used not only for mobile robot can be used in other detection systems.Thoughts: As for why the receiver do not have the transistoramplifier circuit, because the magnification well, CX20106 integrated amplifier, but also with automatic gain control level, magnification to 76dB, the center frequency is 38k to 40k, is exactly resonant ultrasonic sensors frequency.超声波测距系统的电路设计本文所介绍的三方向(前、左、右)超声波测距系统,就是为机器人了解其前方、左侧和右侧的环境而提供一个运动距离信息。
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毕业设计(论文)外文资料翻译系(院):电子与电气工程学院专业:电气工程及其自动化姓名:学号:外文出处:United States Patent 5442592(用外文写)附件: 1.外文资料翻译译文;2.外文原文。
指导教师评语:签名:(手写签名)年月日注:请将该封面与附件装订成册。
外文资料翻译译文超声波测距仪文件类型和数目:美国专利5442592摘要:提出了一种可以抵消温度的影响和湿度的变化的新型超声波测距仪,包括测量单元和参考资料。
在每一个单位,重复的一系列脉冲的产生,每有一个重复率,直接关系到各自之间的距离,发射机和接收机。
该脉冲序列提供给各自的计数器,计数器的产出的比率,是用来确定被测量的距离。
出版日期:1995年8月15日主审查员:罗保.伊恩j.一、背景发明本发明涉及到仪器的测量距离,最主要的是,这种仪器,其中两点之间传输超声波。
精密机床必须校准。
在过去,这已经利用机械设备来完成,如卡钳,微米尺等。
不过,使用这种装置并不利于本身的自动化技术发展。
据了解,两点之间的距离可以通过测量两点之间的行波传播时间的决定。
这样的一个波浪型是一种超声波,或声波。
当超声波在两点之间通过时,两点之间的距离可以由波的速度乘以测量得到的在分离的两点中波中转的时间。
因此,本发明提供仪器利用超声波来精确测量两点之间的距离对象。
当任意两点之间的介质是空气时,声音的速度取决于温度和空气的相对湿度。
因此,它是进一步的研究对象,本次的发明,提供的是独立于温度和湿度的变化的新型仪器。
二、综述发明这项距离测量仪器发明是根据上述的一些条件和额外的一些基础原则完成的,其中包括一个参考单位和测量单位。
参考和测量单位是相同的,每个包括一个超声波发射机和一个接收机。
间隔发射器和接收器的参考值是一个固定的参考距离,而间距之间的发射机和接收机的测量单位是有最小距离来衡量的。
在每一个单位,发射器和接收器耦合的一个反馈回路,它会导致发射器产生超声脉冲,这是由接收器和接收到一个电脉冲然后被反馈到发射机转换,从而使重复系列脉冲的结果。
重复率脉冲是成反比关系之间的距离发射器和接收器。
在每一个单位,脉冲提供一个反馈。
由于参考的距离是众所周知的声速,比例反产出是利用数学以确定所期望的距离来衡量。
由于这两方面都是相同的影响,温度和湿度的变化,采取的比例相同,由此产生的测量变得准确。
三、详细说明一超声波测距原理1、压电式超声波发生器原理压电式超声波发生器实际上是利用压电晶体的谐振来工作的。
超声波发生器内部结构如下所示,它有两个压电晶片和一个共振板。
当它的两极外加脉冲信号,其频率等于压电晶片的固有振荡频率时,压电晶片将会发生共振,并带动共振板振动,便产生超声波。
反之,如果两电极间未外加电压,当共振板接收到超声波时,将压迫压电晶片作振动,将机械能转换为电信号,这时它就成为超声波接收器了。
2、超声波测距原理超声波发射器向某一方向发射超声波,在发射时刻的同时开始计时,超声波在空气中传播,途中碰到障碍物就立即返回来,超声波接收器收到反射波就立即停止计时。
超声波在空气中的传播速度为340m/s,根据计时器记录的时间t,就可以计算出发射点距障碍物的距离(s),即:s=340t/2二超声波测距系统的电路设计系统的特点是利用单片机控制超声波的发射和对超声波自发射至接收往返时间的计时,单片机选用8751,经济易用,且片内有4K的ROM,便于编程。
电路原理图如图2所示。
其中只画出前方测距电路的接线图,左侧和右侧测距电路与前方测距电路相同,故省略之。
1、40kHz 脉冲的产生与超声波发射测距系统中的超声波传感器采用UCM40的压电陶瓷传感器,它的工作电压是40kHz的脉冲信号,这由单片机执行下面程序来产生。
puzel:mov 14h, #12h;超声波发射持续200mshere:cpl p1.0 ;输出40kHz方波nop ;nop ;nop ;djnz 14h,here;ret前方测距电路的输入端接单片机P1.0端口,单片机执行上面的程序后,在P1.0 端口输出一个40kHz的脉冲信号,经过三极管T放大,驱动超声波发射头UCM40T,发出40kHz的脉冲超声波,且持续发射200ms。
右侧和左侧测距电路的输入端分别接P1.1和P1.2端口,工作原理与前方测距电路相同。
2、超声波的接收与处理接收头采用与发射头配对的UCM40R,将超声波调制脉冲变为交变电压信号,经运算放大器IC1A和IC1B两极放大后加至IC2。
IC2是带有锁定环的音频译码集成块LM567,内部的压控振荡器的中心频率f0=1/1.1R8C3,电容C4决定其锁定带宽。
调节R8在发射的载频上,则LM567 输入信号大于25mV,输出端8脚由高电平跃变为低电平,作为中断请求信号,送至单片机处理。
前方测距电路的输出端接单片机INT0端口,中断优先级最高,左、右测距电路的输出通过与门IC3A的输出接单片机INT1端口,同时单片机P1.3和P1.4接到IC3A的输入端,中断源的识别由程序查询来处理,中断优先级为先右后左。
部分源程序如下:receive1:push pswpush accclr ex1 ;关外部中断1jnb p1.1, right ;P1.1引脚为0,转至右测距电路中断服务程序jnb p1.2, left ;P1.2引脚为0,转至左测距电路中断服务程序return:SETB EX1;开外部中断1pop? accpop? pswretiright:...? ;右测距电路中断服务程序入口? ajmp? returnleft:... ;左测距电路中断服务程序入口? ajmp? return3、计算超声波传播时间在启动发射电路的同时启动单片机内部的定时器T0,利用定时器的计数功能记录超声波发射的时间和收到反射波的时间。
当收到超声波反射波时,接收电路输出端产生一个负跳变,在INT0或INT1端产生一个中断请求信号,单片机响应外部中断请求,执行外部中断服务子程序,读取时间差,计算距离。
其部分源程序如下:RECEIVE0:PUSH PSWPUSH ACCCLR EX0 ;关外部中断0? MOV R7, TH0 ;读取时间值MOV R6, TL0?CLR CMOV A, R6SUBB A, #0BBH;计算时间差MOV 31H, A ;存储结果MOV A, R7SUBB A, #3CHMOV 30H, A?SETB EX0 ;开外部中断0POP ACC?POP PSWRETI四、超声波测距系统的软件设计软件分为两部分,主程序和中断服务程序,如图3(a)(b)(c) 所示。
主程序完成初始化工作、各路超声波发射和接收顺序的控制。
定时中断服务子程序完成三方向超声波的轮流发射,外部中断服务子程序主要完成时间值的读取、距离计算、结果的输出等工作。
五、结论对所要求测量范围30cm~200cm内的平面物体做了多次测量发现,其最大误差为0.5cm,且重复性好。
可见基于单片机设计的超声波测距系统具有硬件结构简单、工作可靠、测量误差小等特点。
因此,它不仅可用于移动机器人,还可用在其它检测系统中。
思考:至于为什么接收不用晶体管做放大电路呢,因为放大倍数搞不好,CX20106集成放大电路,还带自动电平增益控制,放大倍数为76dB,中心频率是38k到40k,刚好是超声波传感器的谐振频率。
2:外文原文(复印件)Ultrasonic distance meterDocument Type and Number:United States Patent 5442592 Abstract:An ultrasonic distance meter cancels out the effects of temperature and humidity variations by including a measuring unit and a reference unit. In each of the units, a repetitive series of pulses is generated, each having a repetition rate directly related to the respective distance between an electroacoustic transmitter and an electroacoustic receiver. The pulse trains are provided to respective counters, and the ratio of the counter outputs is utilized to determine the distance being measured.Publication Date:08/15/1995Primary Examiner:Lobo, Ian J.A.BACKGROUND OF THE INVENTIONThis invention relates to apparatus for the measurement of distance and, more particularly, to such apparatus which transmits ultrasonic waves between two points. Precision machine tools must be calibrated. In the past, this has been accomplished utilizing mechanical devices such as calipers, micrometers, and the like. However, the use of such devices does not readily lend itself to automation techniques. It is known that the distance between two points can be determined by measuring the propagation time of a wave travelling between those two points. One such type of wave is an ultrasonic, or acoustic, wave. When an ultrasonic wave travels between two points, the distance between the two points can be measured by multiplying the transit time of the wave by the wave velocity in the medium separating the two points. It is therefore an object of the present invention to provide apparatus utilizing ultrasonic waves to accurately measure the distance between two points.When the medium between the two points whose spacing is being measured is air, the sound velocity is dependent upon the temperature and humidity of the air. It is therefore a further object of the,present invention to provide apparatus of the type described which is independent of temperature and humidity variations.B.SUMMARY OF THE INVENTIONThe foregoing and additional objects are attained in accordance with the principles of this invention by providing distance measuring apparatus which includes a reference unit and a measuring unit. The reference and measuring units are the same and each includes an electroacoustic transmitter and an electroacoustic receiver. The spacing between the transmitter and the receiver of the reference unit is a fixed reference distance, whereas the spacing between the transmitter and receiver of the measuring unit is the distance to be measured. In each of the units, the transmitter and receiver are coupled by a feedback loop which causes the transmitter to generate an acoustic pulse which is received by the receiver and converted into an electrical pulse which is then fed back to the transmitter, so that a repetitive series of pulses results. The repetition rate of the pulses is inversely related to the distance between the transmitter and the receiver. In each of the units, the pulses are provided to a counter. Since the reference distance is known, the ratio of the counter outputs is utilized to determine the desired distance to be measured. Since both counts are identically influenced by temperature and humidity variations, by taking the ratio of the counts, the resultant measurement becomes insensitive to such variations. C.DETAILED DESCRIPTIONA.principle of ultrasonic distance measurement1, the principle of piezoelectric ultrasonic generatorPiezoelectric ultrasonic generator is the use of piezoelectric crystal resonators to work. Ultrasonic generator, the internal structure as shown in Figure 1, it has two piezoelectric chip and a resonance plate. When it's two plus pulse signal, the frequency equal to the intrinsic piezoelectric oscillation frequency chip, the chip will happen piezoelectric resonance, and promote the development of plate vibration resonance, ultrasound is generated. Conversely, if the two are not inter-electrode voltage, when the board received ultrasonic resonance, it will be for vibration suppression of piezoelectric chip, the mechanical energy is converted to electrical signals, then it becomes the ultrasonic receiver.2, the principle of ultrasonic distance measurementUltrasonic transmitter in a direction to launch ultrasound, in the moment to launch the beginning of time at the same time, the spread of ultrasound in the air, obstacles on his way to return immediately, the ultrasonic reflected wave received by the receiver immediately stop the clock. Ultrasound in the air as the propagation velocity of 340m / s, according to the timer records the time t, we can calculate the distance between the launch distance barrier (s), that is: s = 340t / 2B.Ultrasonic Ranging System for the Second Circuit DesignSystem is characterized by single-chip microcomputer to control the use of ultrasonic transmitter and ultrasonic receiver since the launch from time to time, single-chip selection of 8751, economic-to-use, and the chip has 4K of ROM, to facilitate programming. Circuit schematic diagram shown in Figure 2. Draw only the front range of the circuit wiring diagram, left and right in front of Ranging Ranging circuits and the same circuit, it is omitted.1,40 kHz ultrasonic pulse generated with the launchRanging system using the ultrasonic sensor of piezoelectric ceramic sensors UCM40, its operating voltage of the pulse signal is 40kHz, which by the single-chip implementation of the following procedures to generate.puzel: mov 14h, # 12h; ultrasonic firing continued 200mshere: cpl p1.0; output 40kHz square wavenop;nop;nop;djnz 14h, here;retRanging in front of single-chip termination circuit P1.0 input port, single chip implementation of the above procedure, the P1.0 port in a 40kHz pulse output signal, after amplification transistor T, the drive to launch the first ultrasonic UCM40T, issued 40kHz ultrasonic pulse, and the continued launch of 200ms. Ranging the right and the left side of the circuit, respectively, then input port P1.1 and P1.2, the working principle and circuit in front of the same location.2, reception and processing of ultrasonicUsed to receive the first launch of the first pair UCM40R, the ultrasonic pulse modulation signal into an alternating voltage, the op-amp amplification IC1A and after polarization IC1B to IC2. IC2 is locked loop with audio decoder chip LM567, internal voltage-controlled oscillator center frequency of f0 = 1/1.1R8C3, capacitor C4 determine their target bandwidth. R8-conditioning in the launch of the carrier frequency on the LM567 input signal is greater than 25mV, the output from the high jump 8 feet into a low-level, as interrupt request signals to the single-chip processing.Ranging in front of single-chip termination circuit output port INT0 interrupt the highest priority, right or left location of the output circuit with output gate IC3A access INT1 port single-chip, while single-chip P1.3 and P1. 4 received input IC3A, interrupted by the process to identify the source of inquiry to deal with, interrupt priority level for the first left right after. Part of the source code is as follows:receive1: push pswpush accclr ex1; related external interrupt 1jnb p1.1, right; P1.1 pin to 0, ranging from right to interrupt service routine circuitjnb p1.2, left; P1.2 pin to 0, to the left ranging circuit interrupt service routinereturn: SETB EX1; open external interrupt 1pop? accpop? pswretiright: ...?; right location entrance circuit interrupt service routine? Ajmp? Returnleft: ...; left Ranging entrance circuit interrupt service routine? Ajmp? Return3, the calculation of ultrasonic propagation timeWhen you start firing at the same time start the single-chip circuitry within the timerT0, the use of timer counting function records the time and the launch of ultrasonic reflected wave received time. When you receive the ultrasonic reflected wave, the receiver circuit outputs a negative jump in the end of INT0 or INT1 interrupt request generates a signal, single-chip microcomputer in response to external interrupt request, the implementation of the external interrupt service subroutine, read the time difference, calculating the distance . Some of its source code is as follows:RECEIVE0: PUSH PSWPUSH ACCCLR EX0; related external interrupt 0? MOV R7, TH0; read the time valueMOV R6, TL0?CLR CMOV A, R6SUBB A, # 0BBH; calculate the time differenceMOV 31H, A; storage resultsMOV A, R7SUBB A, # 3CHMOV 30H, A?SETB EX0; open external interrupt 0POP ACC?POP PSWRETID.Fourth, the ultrasonic ranging system software designSoftware is divided into two parts, the main program and interrupt service routine, shown in Figure 3 (a) (b) (c) below. Completion of the work of the main program is initialized, each sequence of ultrasonic transmitting and receiving control.Interrupt service routines from time to time to complete three of the rotation direction of ultrasonic launch, the main external interrupt service subroutine to read the value of completion time, distance calculation, the results of the output and so on.E. CONCLUSIONSRequired measuring range of 30cm ~ 200cm objects inside the plane to do a number of measurements found that the maximum error is 0.5cm, and good reproducibility. Single-chip design can be seen on the ultrasonic ranging system has a hardware structure is simple, reliable, small features such as measurement error. Therefore, it can be used not only for mobile robot can be used in other detection systems.Thoughts: As for why the receiver do not have the transistor amplifier circuit, because the magnification well, CX20106 integrated amplifier, but also with automatic gain control level, magnification to 76dB, the center frequency is 38k to 40k, is exactly resonant ultrasonic sensors frequency。