Philosophical Transactions of the Royal Society of London, Volume 126W. Bowyer and J. Nichols for Lockyer Davis, printer to the Royal Society, 1836 |
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Pagina 11
... Hence we have y for each H. P. by reducing the above = double maxima to arcs , and thence we have c , by finding the sines of these arcs . 573 16. By the equilibrium - theory , c should be inversely as the cube of the H. P .; therefore ...
... Hence we have y for each H. P. by reducing the above = double maxima to arcs , and thence we have c , by finding the sines of these arcs . 573 16. By the equilibrium - theory , c should be inversely as the cube of the H. P .; therefore ...
Pagina 12
... Hence the value of a is 60m + 4m ( p − 57 ) . - Effect of the Moon's Declination . 21. The effect of the changes of lunar declination upon the tide will be found in nearly the same way as the effect of changes in the parallax . Mr ...
... Hence the value of a is 60m + 4m ( p − 57 ) . - Effect of the Moon's Declination . 21. The effect of the changes of lunar declination upon the tide will be found in nearly the same way as the effect of changes in the parallax . Mr ...
Pagina 13
... Hence the non - periodical part is 11h 12m 84m sin2 d . ―― The remainder of the Table XII . ( a . ) exhibits the periodical part of the inequality ; and it will be seen that each column follows nearly the law of the mean semimenstrual ...
... Hence the non - periodical part is 11h 12m 84m sin2 d . ―― The remainder of the Table XII . ( a . ) exhibits the periodical part of the inequality ; and it will be seen that each column follows nearly the law of the mean semimenstrual ...
Pagina 14
... Hence 1- tan2 / = - 1.85 37 = tan2 / = 2.85 57 ; 1 = 30 ° 38 ' . 20 57 Hence it appears that the amount of the effect of declination on the time H. W. at Liverpool corresponds to the effect on an equilibrium - spheroid at a place in ...
... Hence 1- tan2 / = - 1.85 37 = tan2 / = 2.85 57 ; 1 = 30 ° 38 ' . 20 57 Hence it appears that the amount of the effect of declination on the time H. W. at Liverpool corresponds to the effect on an equilibrium - spheroid at a place in ...
Pagina 15
... Hence 15.86 sin2 d nearly is the non - periodical part of the Table . The periodical part , as appears by the remainder of Table XVI . ( b . ) , follows nearly the law of the mean height already explained . The sum of the maximum ...
... Hence 15.86 sin2 d nearly is the non - periodical part of the Table . The periodical part , as appears by the remainder of Table XVI . ( b . ) , follows nearly the law of the mean height already explained . The sum of the maximum ...
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