The earth's motion of rotation including the theory of precession and nutation |
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Side
... values of 0 and ... 47 Luni - solar Precession 37 . 38 . 39. Geometrical representation of the motion of the Earth's axis in consequence of Precession and Nutation 40. Annual Luni - solar Precession ........ 41. Effect of Planetary ...
... values of 0 and ... 47 Luni - solar Precession 37 . 38 . 39. Geometrical representation of the motion of the Earth's axis in consequence of Precession and Nutation 40. Annual Luni - solar Precession ........ 41. Effect of Planetary ...
Side 3
... values , the third equation of motion becomes - 2 ‚ dw ̧ _ { k3 — Bh + ( B − C ) Cw ̧2 } 1 { − k2 + Ah + ( C − A ) Cw , 3 } i — — ( C − A ) C = di whence t + 1 √ ( AB ) dw3 = C ' √ ( AB ) ] { k2 — Bh + ( B — C ' ) Cœ ̧ ...
... values , the third equation of motion becomes - 2 ‚ dw ̧ _ { k3 — Bh + ( B − C ) Cw ̧2 } 1 { − k2 + Ah + ( C − A ) Cw , 3 } i — — ( C − A ) C = di whence t + 1 √ ( AB ) dw3 = C ' √ ( AB ) ] { k2 — Bh + ( B — C ' ) Cœ ̧ ...
Side 6
... values of w1 , w ,, w , obtained as above ( Art 3 ) , and then integrating these equations , 0 , & , and would be determined , and thus the position of the principal axes at any time would be known . The integration , how- ever , canno ...
... values of w1 , w ,, w , obtained as above ( Art 3 ) , and then integrating these equations , 0 , & , and would be determined , and thus the position of the principal axes at any time would be known . The integration , how- ever , canno ...
Side 12
... values of x , y , z so obtained be now substituted in the expression for V , it will become a function of 0 , 4 , ; and , in so far as it depends upon the disturbed planet , of quantities indepen- dent of the time . ( ii ) As a function ...
... values of x , y , z so obtained be now substituted in the expression for V , it will become a function of 0 , 4 , ; and , in so far as it depends upon the disturbed planet , of quantities indepen- dent of the time . ( ii ) As a function ...
Side 13
... values of the elements at any time , commencing with h , the element of vis viva . Let T denote the vis viva due to the rotation of the planet , Sm , do dv1 the resolved part of the disturbing force on an element Sm , of its mass in the ...
... values of the elements at any time , commencing with h , the element of vis viva . Let T denote the vis viva due to the rotation of the planet , Sm , do dv1 the resolved part of the disturbing force on an element Sm , of its mass in the ...
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The Earth's Motion of Rotation: Including the Theory of Precession and Nutation Charles Hartwell Horne Cheyne Uten tilgangsbegrensning - 1867 |
The Earth's Motion of Rotation: Including the Theory of Precession and Nutation Charles Hartwell Horne Cheyne Uten tilgangsbegrensning - 1867 |
The Earth's Motion of Rotation: Including the Theory of Precession and Nutation Charles Hartwell Horne Cheyne Uten tilgangsbegrensning - 1867 |
Vanlige uttrykk og setninger
area conserved axis in space calculating Cambridge centre of gravity Church cloth cos² Crown 8vo denote determine the motion dh dt dh dV differential coefficient disturbing force dk dt dl dh ds dh dt 2n dt dk dt dt dt dv dt dy dV dg dv ds dv dt dV dv dv dy Earth's axis ecliptic Elementary Treatise English equations of Art Extra fcap Fcap fixed plane formulæ Fourth Edition Heir of Redclyffe Hence HENRY KINGSLEY Illustrations integration invariable plane JOSEPH BAYMA longitude M. A. Second Edition maximum areas Moon's orbit motion of translation Nutation obtained order of approximation plane of maximum plane of reference Planetary Theory Poems point of Aries preceding Article Precession principal axes revised Sermons preached sin'i Sir NOEL PATON Spherical substituting Sun's Third Edition tion undisturbed motion Vignette vis viva Vols w₁ w₂ Y₁
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