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    Numerical Fourier Transform Calculations for Pulse Testing Procedures

    Source: Journal of Fluids Engineering:;1967:;volume( 089 ):;issue: 002::page 445
    Author:
    Sidney Lees
    ,
    Ray C. Dougherty
    DOI: 10.1115/1.3609632
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Pulse testing of systems, where the input is a controlled function of time, is a well-established procedure. One data reduction technique numerically calculates the Fourier transforms of the input and the response. The complex ratio is the FT of the system function. It is shown (a) that the correction function usually employed to improve the respective FTs cancels out and is a useless operation; (b) that the numerical system function FT fails at high frequencies because the approximation to the integral fails to converge; (c) the upper limit in frequency is ωδ ≤ 0.1π, not π as predicted by the sampled data theorem; (d) generally it is necessary to use ten times as many data points as has been the practice to attain a given bandwidth.
    keyword(s): Testing , Fourier transforms , Transfer functions , Fourier transform spectroscopy , Approximation , Frequency AND Theorems (Mathematics) ,
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      Numerical Fourier Transform Calculations for Pulse Testing Procedures

    URI
    https://yetl.yabesh.ir/yetl1/handle/yetl/120324
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    contributor authorSidney Lees
    contributor authorRay C. Dougherty
    date accessioned2017-05-08T23:56:24Z
    date available2017-05-08T23:56:24Z
    date copyrightJune, 1967
    date issued1967
    identifier issn0098-2202
    identifier otherJFEGA4-27296#445_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/120324
    description abstractPulse testing of systems, where the input is a controlled function of time, is a well-established procedure. One data reduction technique numerically calculates the Fourier transforms of the input and the response. The complex ratio is the FT of the system function. It is shown (a) that the correction function usually employed to improve the respective FTs cancels out and is a useless operation; (b) that the numerical system function FT fails at high frequencies because the approximation to the integral fails to converge; (c) the upper limit in frequency is ωδ ≤ 0.1π, not π as predicted by the sampled data theorem; (d) generally it is necessary to use ten times as many data points as has been the practice to attain a given bandwidth.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleNumerical Fourier Transform Calculations for Pulse Testing Procedures
    typeJournal Paper
    journal volume89
    journal issue2
    journal titleJournal of Fluids Engineering
    identifier doi10.1115/1.3609632
    journal fristpage445
    journal lastpage449
    identifier eissn1528-901X
    keywordsTesting
    keywordsFourier transforms
    keywordsTransfer functions
    keywordsFourier transform spectroscopy
    keywordsApproximation
    keywordsFrequency AND Theorems (Mathematics)
    treeJournal of Fluids Engineering:;1967:;volume( 089 ):;issue: 002
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
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