Monthly Notices of the Royal Astronomical SocietyPriestly and Weale, 1861 |
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Page 31
... complete values g + de , vv . Then putting d P P - бе + d P dv dv + d P de + de dP dv ' , dv ' On the Secular Acceleration of the Moon's Mean Motion . By A. Cayley , Esq . ( Abstract . ) The inclination and excentricity of the Moon's ...
... complete values g + de , vv . Then putting d P P - бе + d P dv dv + d P de + de dP dv ' , dv ' On the Secular Acceleration of the Moon's Mean Motion . By A. Cayley , Esq . ( Abstract . ) The inclination and excentricity of the Moon's ...
Page 37
... complete outline of the method of investigation , and it was thought better to omit altogether the details of the working rather than present them in an incomplete manner . The Transit of Mercury , Nov. 11 , 1861 . ( Extract of a Letter ...
... complete outline of the method of investigation , and it was thought better to omit altogether the details of the working rather than present them in an incomplete manner . The Transit of Mercury , Nov. 11 , 1861 . ( Extract of a Letter ...
Page 61
... complete . The preceding account relates to north declination to 81 ° . It was considered impossible to continue the observations in zones beyond this point , on account of the extremely slow movement of the stars , and recourse was had ...
... complete . The preceding account relates to north declination to 81 ° . It was considered impossible to continue the observations in zones beyond this point , on account of the extremely slow movement of the stars , and recourse was had ...
Page 70
... complete , and if the graduation of the thermometer is correct . The difference between them is so small that the result must , I think , be deemed satisfactory . Let us study the same differences with the cooling in air : - = Atr 5 ...
... complete , and if the graduation of the thermometer is correct . The difference between them is so small that the result must , I think , be deemed satisfactory . Let us study the same differences with the cooling in air : - = Atr 5 ...
Page 76
... complete differential coefficient of is d ( n ) dt = d'o dt ΦΩ n ' dv ' where denotes , as usual , the differential coefficient in d'a dt regard to the time , in so far as it enters through the co - ordi- nates r , v , y of the ...
... complete differential coefficient of is d ( n ) dt = d'o dt ΦΩ n ' dv ' where denotes , as usual , the differential coefficient in d'a dt regard to the time , in so far as it enters through the co - ordi- nates r , v , y of the ...
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Common terms and phrases
2r+g Airy Alhazen Annex appears April Astronomer Royal bright Calculation CAYLEY clock Comet computed corrected crater Decl declination diameter difference distance Ditto ditto edge Ephemeris equations Equatoreal error excentricity eye-piece Greenwich inches aperture instrument July June Jupiter Jupiter's Satellites latitude light limb longitude Lunar m² e m² n² Mars Mean Solar measures Memoir meridian Minor Planets Monthly Notices Moon Moon's Mean Motion N.P.D. from Observation Nautical Almanac nearly Nebula nucleus Number of Observations obtained Occultation orbit parallax perihelion photographs Prof R.A. from Observation Radcliffe Catalogue radiation Right Ascension ring Royal Observatory Saturn Secular Acceleration shadow Sirius Small Planets Society Solar Eclipse soleil stars Struve Sun's disk surface T. W. Webb taches telescope term thermometer tion Transit of Mercury Ursa Variable Variable Stars W. R. Dawes Weisse