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Theory of the astronomical transit instrument applied to the portable transit instrument Wuerdemann no.26: a compilation from various authorities, with original observations by Harry Edward Burton, 1903

Theory of the astronomical transit instrument applied to the portable transit instrument Wuerdemann no. 26: a compilation from various authorities, with original observations by Harry Edward Burton, 1903, Page 60

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Mayer's Formula. If the transit instrument were in perfect adjustment we would have, as the relation between the right ascension, the clock time of transit of a star, and Δt, α = t + Δt ; but considering the effects of the errors in level, azimuth, and collimation, this equation become[s?] α = t + Δt + ((sin(0-δ))/cos δ) a[superscript][s?][/superscript] + ((cos(0-δ))/cos δ)b[superscript][s?][/superscript] + (1/cos δ)c[superscript][s?][/superscript] or α = t + Δt + Aa[superscript][s?][/superscript] + Bb[superscript][s?][/superscript] + Cc[superscript][s?][/superscript] . (1). This is Mayer's formula. The constants A, B, and C have been computed and tabulated for latitude 41° 40' and for declinations from -35° to 90° for upper culminations, and from 90° to 55° for lower culminations. By means of the equation (1) we can find Δt by the following method: α is given by the Nautical Almanac; A, B, and C are computed when the latitude is given; b[superscript][s?][/superscript] is determined by level readings, and t is observed; so the only unknown quantities are Δt, a[superscript][s?][/superscript], and c[superscript][s?][/superscript]. Transposing the unknown quantities to the
 
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