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Re: Averaging lunars: was Lunars with SNO-T

From: Herbert Prinz (no email)
Date: Mon Nov 01 2004 - 05:52:39 EST

  • Next message: George Huxtable: "Re: Lunars: A 90 Degree Miracle"

    George Huxtable wrote:

    > It may be interesting to read what Tobias Mayer had to say on this topic,
    > [...]

    Thanks to George Huxtable for posting and Steven Wepster for translating. While
    we are at it, Note I, immediately preceding the quoted passage might also be of
    interest. In an earlier message I had casually compared the repeating circle
    with our averaging technique. This note reminds me that the two methods are
    different in one respect.

    In Note I, Mayer says that the final error of an observation is inverse
    proportional to the number of individual distances that have been accumulated
    into this observation. Therefore, if one assumes an instrument error of 2' to
    3', six observations are plenty sufficient to get the error below 30".

    In passing I remark that the goal for accuracy that Mayer sets himself is truly
    down to earth, much less ambitious than that of some of our list members! But
    my question is: Is his arithmetic right?

    It is right, if we assume that the observer is perfect and the only purpose of
    the averaging process is the elimination of instrument error and reading error
    (due to limited resolution of the division of the limb). This is what Mayer had
    in mind.

    When we average with a sextant, we are in a different situation. We can never
    get around the instrument error or the reading error with repeated readings.
    Our assumption is that the observer is not perfect and each observation is
    fraught with random error. This error is inverse proportional to the square
    root of the number of observations. Given the above parameters, six
    observations would not be sufficient.

    If an imperfect observer producing random errors had a perfect sextant and a
    perfect repeating circle, the result of a repeated observation would be the
    same on both instruments (statistically). The error would obey the inverse
    square root law on both instruments. Mayer did not address this kind of error.
    He did not have the appropriate error theory. Might he have thought that he had
    divided random error by the number of observations, too? I don't know the
    answer.

    Herbert Prinz


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