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Appendix B - Dimensions and Units

from Part VIII - Fundaments

Published online by Cambridge University Press:  26 October 2017

David E. Loper
Affiliation:
Florida State University
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Summary

The fundaments of kinematics presented include:

  • • B.1: an introduction to dimensional analysis;

  • • B.2: an introduction to the international system of units; and

  • • B.3: a table of parameters relevant to waves and flows on Earth and their estimated magnitudes.

  • Dimensional Analysis

    This fundament provides an orientation to the process of dimensional analysis, whereby a problem is simplified by analyzing the dimensions of its variables and parameters. The theoretical basis for this process is provided by the Buckingham Pi theorem. An essential part of the process is the formation of a minimal number of dimensionless parameters, typically denoted by , each of which is an algebraic combination of the dimensional parameters in the problem. One advantage of dimensional analysis is that we do not need a set of governing equations (though that is, of course, quite helpful). All that is needed is a “grocery list” of relevant parameters.

    A related procedure is non-dimensionalization, whereby a set of governing equations and the parameters within it are made dimensionless. Often the equations are significantly simplified by this procedure, making them more amenable to analysis and solution.

    Dimensional analysis employs the seven base dimensions (length, mass, time, temperature, electric current, amount of substance and luminous intensity) of the SI system. Mechanical systems involve only the first three (length, mass and time), denoted by L, M and T:

    L = length M= mass T = time.

    Commonly the dimensions of a variable are identified using square brackets; for example, [g] = L·T−2 means that the dimensions of acceleration are length divided by time squared.

    In addition to the seven base dimensions, the SI system contains two supplemental units: plane and solid angle. These do not play a direct role in dimensional analysis and non-dimensionalization, but they do affect the numerical relationships among the dimensionless variables. The number of dimensionless parameters involved in a physical problem can easily be determined by use of the Buckingham Pi theorem which states that

    N = NpNd,

    where N is the number of dimensionless parameters, Np is the number of dimensional

    parameters and Nd is the number of base dimensions contained in all parameters.

    Type
    Chapter
    Information
    Geophysical Waves and Flows
    Theory and Applications in the Atmosphere, Hydrosphere and Geosphere
    , pp. 405 - 411
    Publisher: Cambridge University Press
    Print publication year: 2017

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    • Dimensions and Units
    • David E. Loper, Florida State University
    • Book: Geophysical Waves and Flows
    • Online publication: 26 October 2017
    • Chapter DOI: https://doi.org/10.1017/9781316888858.046
    Available formats
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    • Dimensions and Units
    • David E. Loper, Florida State University
    • Book: Geophysical Waves and Flows
    • Online publication: 26 October 2017
    • Chapter DOI: https://doi.org/10.1017/9781316888858.046
    Available formats
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    To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Google Drive.

    • Dimensions and Units
    • David E. Loper, Florida State University
    • Book: Geophysical Waves and Flows
    • Online publication: 26 October 2017
    • Chapter DOI: https://doi.org/10.1017/9781316888858.046
    Available formats
    ×