欢迎来到毕设资料网! | 帮助中心 毕设资料交流与分享平台
毕设资料网
全部分类
  • 毕业设计>
  • 毕业论文>
  • 外文翻译>
  • 课程设计>
  • 实习报告>
  • 相关资料>
  • ImageVerifierCode 换一换
    首页 毕设资料网 > 资源分类 > DOC文档下载
    分享到微信 分享到微博 分享到QQ空间

    外文翻译--底土的土壤结构和饱和导水率

    • 资源ID:128227       资源大小:537KB        全文页数:11页
    • 资源格式: DOC        下载积分:100金币
    快捷下载 游客一键下载
    账号登录下载
    三方登录下载: QQ登录
    下载资源需要100金币
    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。
    支付方式: 支付宝   
    验证码:   换一换

     
    账号:
    密码:
    验证码:   换一换
      忘记密码?
        
    友情提示
    2、PDF文件下载后,可能会被浏览器默认打开,此种情况可以点击浏览器菜单,保存网页到桌面,就可以正常下载了。
    3、本站不支持迅雷下载,请使用电脑自带的IE浏览器,或者360浏览器、谷歌浏览器下载即可。
    4、本站资源下载后的文档和图纸-无水印,预览文档经过压缩,下载后原文更清晰。

    外文翻译--底土的土壤结构和饱和导水率

    1、英文原文 : Low-cost programmable pulse generator for particle telescope calibration Abstract In this paper we present a new calibration system for particle telescopes including multi pulse generator and digital controller. The calibration system generates synchronized pulses of variable height for every

    2、 detector channel on the telescope. The control system is based on a commercial microcontroller linked to a personal computer through an RS-232 bidirectional line. The aim of the device is to perform laboratory calibration of multi-detector telescopes prior to calibration at accelerator. This task i

    3、ncludes evaluation of linearity and resolution of each detector channel, as well as coincidence logic. The heights of the pulses sent to the detectors are obtained by Monte Carlo simulation of telescope response to a particle flux of any desired geometry and composition. Elsevier Science B.V. All ri

    4、ghts reserved. To assure a correct interpretation of data obtained with scientific instruments onboard satellites, as well as to compare these data with those of similar instruments, a thorough pre-flight calibration is required. For solar and cosmic ray particle telescopes, this calibration is usua

    5、lly carried out in two steps: first, a calibration of each individual detector using radioactive sources and standard nuclear instrumentation (NIM or CAMAC modules),following by a final test of the whole telescope performed in a particle accelerator site. The success of calibration on accelerator re

    6、quires that, prior to the experiences, all detectors and electronics parameter (polarization voltages, amplifier gains and shaping times, thresholds, etc.) have nearly definitive values. Here we propose a cheap and simple pre-calibration procedure based on a new system that we have called Programmab

    7、le Pulse Generator (PPG). The PPG developed in our laboratory has been designed for a specific instrument, a four-detector cosmic ray telescope, but it can easily be modified for similar experiments. The standard calibration procedure for individual detectors and their electronic chains consists of

    8、introducing pulses of known amplitudes coming from a pulse generator, together with the pulses released in the detector by particles coming from a radioactive source. However, these standard pulse generators do present several limitations: The pulse amplitude must be set manually. Thus, to generate

    9、the pulses that different particles with different energies would release on the detectors, it is necessary to change the pulse heights every time. Standard pulse generators only provide one output signal, so either several modules are needed to calibrate a complete telescope, or it is necessary to

    10、split the single output in order to get several signals. It is difficult to check the coincidence logic because the four signals are not independent. To overcome these difficulties, pulse generators of programmable amplitude and rate have been proposed. Abdel-Aal 1presented a programmable random pul

    11、se generator where the height and separation of individual pulses are controlled by software.But in his scheme the pulses are released directly from a digital-to-analog converter(DAC),thus having the temporal characteristics of the DAC output. Our purpose is to generate variable height analog pulses

    12、 with similar shape to that released by nuclear detectors. The low-cost PPG presented here is intended to introduce every detector channel , the pulses released by any particle flux supposed to be encountered by the instrument on real experiments (in our case, on outer space environment). The propos

    13、ed pre-calibration scheme is sketched in the diagram of Fig 1. For a big number of simulated events, the energy signals released at the different detectors of the telescope are stored on a personal computer (PC). For each individual event, the energy signal data are sent through a bidirectional RS-2

    14、32-C line to the PPG, which transforms the results of the simulation into real pulses and sends them to the real instrument. Fig 1 2 PPG description The design of the PPG is divided into two functional modules: digital electronics and analog electronics, whose block diagrams are enclosed in dashed b

    15、oxes shown in Fig2. The data arriving at the digital module from the PC are sent to 12 bit DAC. The DAC output voltages are transformed in the analog module into suitable pulses, ready to be introduced into the test input of the related detector channel of the telescope. Analog and digital modules a

    16、re described with some detail in Sections 2.1 and 2.2. In Section 2.3 we describe some noise problems related with the microcontroller, and the way we found to solve them. 2.1 Analog module This module must be capable of producing signal pulses similar to those generated in the detectors by the pass

    17、age of energetic charged particles, whose shape can be described by the following function: V t e x p e x p .1/R F R FA t t (1) The relevant signal parameters are the pulse height or amplitude A, the rise time R and the fall time F (here expressed as 1/e times rather than 10-90% times). Using semico

    18、nductor detectors, typical values for R and F are approximately 5 ns and 10 us, respectively. Our particular telescope has four detectors, therefore four almost simultaneous pulses with different amplitudes 14AA have to be generated for each simulated event. These amplitudes are sent by the digital

    19、module to the analog module, together with a start pulse (see Fig 2). The communication is performed through a coupler circuit for isolation purposes. The start signal is sent to a reference pulse generator, which generates a pulse of constant amplitude, rise and fall times. One of the inputs of each multiplier is this reference pulse, and the other is one of the DAC amplitude signals. Thus, every multiplier acts as a modulator: when the reference pulse arrives,


    注意事项

    本文(外文翻译--底土的土壤结构和饱和导水率)为本站会员(泛舟)主动上传,毕设资料网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,请联系网站客服QQ:540560583,我们立即给予删除!




    关于我们 - 网站声明 - 网站地图 - 资源地图 - 友情链接 - 网站客服 - 联系我们
    本站所有资料均属于原创者所有,仅提供参考和学习交流之用,请勿用做其他用途,转载必究!如有侵犯您的权利请联系本站,一经查实我们会立即删除相关内容!
    copyright@ 2008-2025 毕设资料网所有
    联系QQ:540560583