<em id="rw4ev"></em>

      <tr id="rw4ev"></tr>

      <nav id="rw4ev"></nav>
      <strike id="rw4ev"><pre id="rw4ev"></pre></strike>
      合肥生活安徽新聞合肥交通合肥房產生活服務合肥教育合肥招聘合肥旅游文化藝術合肥美食合肥地圖合肥社保合肥醫院企業服務合肥法律

      5CCYB041代寫、C++設計程序代做
      5CCYB041代寫、C++設計程序代做

      時間:2025-03-06  來源:合肥網hfw.cc  作者:hfw.cc 我要糾錯



      Object-Oriented Programming Page 1 of 6 Coursework 1
      BEng Biomedical Engineering
      Object-Oriented Programming
      Coursework 1
      Objective
      To gain practical experience of C++ coding to solve a simple problem. 
      Introduction 
      Magnetic Resonance Imaging is a powerful imaging technique capable of producing images of 
      internal organs with good soft tissue contrast. It relies on a number of hardware components, as 
      illustrated in Figure 1: a powerful permanent magnet; magnetic field gradients provided by 
      dedicated gradient coils (Figure 1, right); and radio-frequency coils to excite the nuclear spins 
      (typically 1H) and detect the resulting nuclear magnetic resonance signal. 
       
      Figure 1: the different hardware components of a typical MRI scanner. Left: a cutaway view showing the 
      arrangement of the main magnet, gradient coils and RF coil. Right: an example of the design of a gradient 
      coil, showing the different concentric windings required to impart magnetic field gradients along the x, 
      y & z axes. 
      The role of the gradient coils is to impart a linear change in the resonance frequency of the 1H 
      nuclear spins as a function of position, which allows the position of the signal to be inferred. To 
      provide full images, these magnetic field gradients need to be rapidly modulated in time, which is 
      done by driving very large currents through the gradient coils and switching them rapidly on & 
      off at appropriate times along the appropriate axes. 
      5CCYB041
      Object-Oriented Programming Page 2 of 6 Coursework 1
      Eddy-currents in MRI
      Because of Faraday’s law of electromagnetic induction, these rapid and intense changes in the
      magnetic fields induce voltages, which in turn drive currents in nearby conductive structures.
      These eddy currents create magnetic fields that oppose the change in magnetic field that created 
      them (this is called Lenz’s law). 
      In MRI, the net result is that the temporal evolution of the magnetic field gradient actually 
      produced will differ from the waveform provided to the gradient amplifier. This is illustrated in 
      Figure 2, showing how an ideal trapezoidal input waveform will end up distorted and lagging 
      behind what was expected, and the resulting impact on images acquired using echo-planar 
      imaging (a single-shot imaging technique). Eddy currents can affect the images in many different 
      ways, depending on the type of MRI sequence used and other factors, but they are invariably 
      problematic. For this reason, a variety of techniques are used to minimise eddy-currents, 
      including hardware solutions (e.g. actively shielded gradients) and gradient pre-emphasis.
      Figure 2: illustration of the effect of eddy-currents. (a) the expected waveform (dotted line) is distorted 
      due to eddy-currents, resulting in the delayed time evolution of the actual gradients (solid line). (b) The 
      eddy-currents (solid line) originate from the rapid changes in the magnetic field that occur when there 
      is a change in the gradient (dotted line). (c) image that would ideally be acquired using echo-planar 
      imaging (EPI). (d) the image acquired when eddy currents introduce significant delays in the signal 
      shows clear ‘ghosting’ artefacts.
      Gradient pre-emphasis
      Gradient pre-emphasis involves modifying the signal time course provided to the gradient 
      amplifier to compensate for the expected effect of eddy-currents, as illustrated in Figure 3. If the 
      properties of the eddy-currents are known, it is possible to predict the time course of the actual
      gradient for a given input waveform. With pre-emphasis, the input waveform is modified so that 
      the time course of the actual gradient matches the desired waveform more accurately.
      For the purposes of pre-emphasis, eddy-currents are typically modelled as multiple components, 
      each with a given amplitude and decay rate constant. The parameters of the different eddy current components are measured during routine maintenance as part of the calibration of the 
      MRI scanner, and stored on the system for use in gradient pre-emphasis.
      5CCYB041
      Object-Oriented Programming Page 3 of 6 Coursework 1
      Figure 3: illustration of gradient pre-emphasis. (a) the desired gradient waveform. (b) the actual gradient 
      time course obtained differs due to the effects of eddy-currents. (c) with pre-emphasis, a modified
      waveform is provided as input to the amplifier, designed in such a way that the actual gradient time 
      course matches the desired waveform.
      Instructions 
      Your task in this coursework is to write a C++ program to implement a simple gradient pre emphasis strategy. This program should perform the following main steps (these are described in 
      more detail below): 
      1. Load the parameters describing the eddy-currents for the system from the file provided.
      2. Load the desired time course for the gradient from the file provided.
      3. Make a copy the desired time course, which will be the initial input gradient time course.
      4. Compute the predicted time course for the input time course by taking the effects of eddy currents into account.
      5. Compute the maximum absolute deviation between the desired and predicted time 
      courses, and display this value on the terminal
      6. Display the input and predicted time courses on the terminal.
      7. Compute the difference between the desired and predicted time course.
      8. Add that difference back to the current input time course.
      9. Go back to step 4 and repeat for the desired number of iterations
      10. If requested, write the final estimate of the compensated input time course to the file 
      specified on the command-line
      Command-line interface
      Your program should accept at least 2 arguments: the configuration file containing the parameters 
      for the eddy-currents, and the file containing the desired time course. If a third argument is 
      provided, this should be interpreted as a request to store the estimated compensated time course 
      to the file specified in that argument.
      Your program should also accept a “-n num” command-line option to override the default number 
      of iterations. If left unspecified, the default number of iterations should be set to 10.
      5CCYB041
      Object-Oriented Programming Page 4 of 6 Coursework 1
      Loading the input data
      You are provided with a text file called parameters.txt file containing the eddy-current 
      parameters. Each line in this file contains two values: the amplitude and the rate constant for each 
      eddy-current component. 
      You are also provided with a text file called gradient.txt file containing the intensity values at 
      regular sampling intervals for the desired gradient time course. 
      Computing the predicted gradient time course 
      The impact of the eddy-currents can be predicted using a simple model. Each eddy-current 
      component can be modelled independently, and will have an associated current 𝐼𝑛 (with initial
      value zero). The instantaneous chance in the gradient, 𝑑𝐺, causes the current to increase in 
      proportion. At the same time, the resistance in the system causes the current to reduce in 
      proportion to the magnitude of the current. The predicted gradient is then given as the input
      gradient minus the eddy-current contributions, which is the sum of their currents weighted by 
      their respective amplitude parameter. 
      This can be written in simplified form as:
      𝑑𝐺𝑡 = 𝐺𝑡 − 𝐺𝑡−1
      𝐼𝑛,𝑡 = 𝐼𝑛,𝑡−1 + 𝑑𝐺𝑡 − 𝑅𝑛 × 𝐼𝑛,𝑡−1
      𝐺𝑡
      ′ = 𝐺𝑡 − ∑𝐴𝑛 × 𝐼𝑛,𝑡
      𝑁
      𝑛
      where:
      • 𝐺𝑡 and 𝐺𝑡

      are the input and predicted waveforms at time point 𝑡 respectively
      • 𝐼𝑛,𝑡
      is the value of the current at time point 𝑡 for the nth eddy-current component
      • 𝐴𝑛 and 𝑅𝑛 are the amplitude and rate constant parameters for the nth eddy-current 
      component.
      • 𝑁 is the number of eddy-current components listed in the parameter file.
      Computing the compensated time course
      The compensation to be applied to the waveform can be computed using the following iterative 
      approach:
      Given the desired waveform:
      • Initialise the current estimate of the (compensated) input waveform as the desired
      waveform
      • Repeat for the desired number of iterations:
      o Compute the predicted waveform for the current input waveform
      o Compute the difference between the desired and predicted waveforms
      o Add the computed difference to the current input waveform, to produce the next 
      estimate of the input waveform
      5CCYB041
      Object-Oriented Programming Page 5 of 6 Coursework 1
      Displaying the waveforms
      The various waveforms can be displayed using the terminal_graphics library. Refer to the relevant 
      course slides and the project README for detailed instructions. 
      Briefly: download the terminal_graphics.h header and place it in your project folder, alongside 
      your own code. Make sure to #include that header into your code. Then use the TG::plot()
      functionality as illustrated below:
      #include "terminal_graphics.h"
      ...
      std::vector<float> desired_gradient, predicted_gradient; 
      ... 
      TG::plot (width, height)
       .add_line (desired_gradient)
       .add_line (predicted_gradient, 3);
      Writing the final compensated time course
      Your program should only store the output if provided with a third argument on the command line. If this is the case, you should write the final compensated time course to the file specified as 
      the last argument, in the same format as the original desired time course. 
      Example output
      The example below only shows the initial and last iteration of the algorithm:
      5CCYB041
      Object-Oriented Programming Page 6 of 6 Coursework 1
      Reporting Requirements 
      You should submit a C++ project that meets as many of the requirements as possible. You do not 
      need to submit any written report but do try to use variable/function naming, comments and 
      indentation to make your program as easy to understand as possible. Also try to make your 
      program as resilient to runtime errors as possible. 
      Submission will be via the KEATS system. The submission point will only allow you to upload a 
      single file so you should combine all files into a single ZIP file. Please only include your .cpp and
      .h files (please run “oop_build clean” first to remove any executables or object files). 
      The hand-in date is 25 Feb 2025, 4 pm. Late submissions (within 24 hours of this deadline) will 
      be accepted but will be capped at the module pass mark (i.e. 40%). 
      If your program does not meet all requirements, then please submit what you have written by the 
      deadline. 
      Assessment 
      Your coursework will be marked on a number of factors: 
      • Does the program work? Does it meet all requirements? Has it been tested extensively? 
      (60%) 
      • Program design and appropriate use of C++ language features, e.g. control structures, 
      functions, data types, etc. (30%)
      • Use of comments, indentation and variable/function names to make code easy to 
      understand (10%)
      The overall mark for this coursework will make up 10% of your total mark for this module. 
      This is an individual assignment. You are not permitted to work together with any other 
      student. Note that general discussions about design decisions and/or coding strategies are 
      permitted, and such discussions can be a useful learning experience for you. But you should not, 
      under any circumstances, share details of designs or code. 
      Code generated using AI assistants, etc. is also not permitted. While these tools may 
      (potentially) be useful in your learning to help clarify certain concepts, this is only true if they are 
      used very cautiously and sparingly. Over-reliance on these tools to give you ready answers will 
      inhibit your learning by preventing you from working things out for yourself. This will result in
      failure in the final exam where you will have no access to these tools (note that the final exam
      accounts for 60% of the overall marks on this module). We therefore strongly discourage the use 
      of any form of AI assistants – in our opinion (and that of many others), these are detrimental to 
      your performance on the course.

      請加QQ:99515681  郵箱:99515681@qq.com   WX:codinghelp

      掃一掃在手機打開當前頁
    1. 上一篇:紅星花客服電話24小時在線解決客戶下款問題!
    2. 下一篇:極借花全國客服電話-極借花24小時服務熱線電話
    3. 無相關信息
      合肥生活資訊

      合肥圖文信息
      挖掘機濾芯提升發動機性能
      挖掘機濾芯提升發動機性能
      戴納斯帝壁掛爐全國售后服務電話24小時官網400(全國服務熱線)
      戴納斯帝壁掛爐全國售后服務電話24小時官網
      菲斯曼壁掛爐全國統一400售后維修服務電話24小時服務熱線
      菲斯曼壁掛爐全國統一400售后維修服務電話2
      美的熱水器售后服務技術咨詢電話全國24小時客服熱線
      美的熱水器售后服務技術咨詢電話全國24小時
      海信羅馬假日洗衣機亮相AWE  復古美學與現代科技完美結合
      海信羅馬假日洗衣機亮相AWE 復古美學與現代
      合肥機場巴士4號線
      合肥機場巴士4號線
      合肥機場巴士3號線
      合肥機場巴士3號線
      合肥機場巴士2號線
      合肥機場巴士2號線
    4. 幣安app官網下載 短信驗證碼 丁香花影院

      關于我們 | 打賞支持 | 廣告服務 | 聯系我們 | 網站地圖 | 免責聲明 | 幫助中心 | 友情鏈接 |

      Copyright © 2024 hfw.cc Inc. All Rights Reserved. 合肥網 版權所有
      ICP備06013414號-3 公安備 42010502001045

      成人久久18免费网站入口