The earth's motion of rotation including the theory of precession and nutation |
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Side
... of the varia- tion of arbitrary constants . In the SECOND PART the general rotation - formulæ are applied to the particular case of the Earth . These formulæ afford a simple and accurate proof of the important theorem.
... of the varia- tion of arbitrary constants . In the SECOND PART the general rotation - formulæ are applied to the particular case of the Earth . These formulæ afford a simple and accurate proof of the important theorem.
Side
... constants of integration . 5. Equations for determining the motion in space 6. The same when the invariable plane is the plane of reference 7. When the motion with reference to the invariable plane is known , to determine it with ...
... constants of integration . 5. Equations for determining the motion in space 6. The same when the invariable plane is the plane of reference 7. When the motion with reference to the invariable plane is known , to determine it with ...
Side 2
... constant of integration . Again , multiplying by Aw ,, Bw ,, Cw ,, 2 THE EARTH'S MOTION OF ROTATION . Reason of the smallness of the effect upon the rotation of planet of the attractions of other bodies Undisturbed Motion.
... constant of integration . Again , multiplying by Aw ,, Bw ,, Cw ,, 2 THE EARTH'S MOTION OF ROTATION . Reason of the smallness of the effect upon the rotation of planet of the attractions of other bodies Undisturbed Motion.
Side 3
... constant of integration . From these two equations we obtain = k2 – Bh + ( B − C ) Cw2 - ( A – B ) A 2 - k2 + Ah + ( C − A ) Cw * ( A - B ) B Substituting these values , the third equation of motion becomes - 2 ‚ dw ̧ _ { k3 — Bh + ...
... constant of integration . From these two equations we obtain = k2 – Bh + ( B − C ) Cw2 - ( A – B ) A 2 - k2 + Ah + ( C − A ) Cw * ( A - B ) B Substituting these values , the third equation of motion becomes - 2 ‚ dw ̧ _ { k3 — Bh + ...
Side 4
... and join PA , PB , CA , CB by arcs of great circles . N A Р B Let the angle ONA = 0 , ON = † , NA = 4 ; then if the angles 0 , 4 , be known , the position 4 THE EARTH'S MOTION OF ROTATION . Signification of the constants of integration.
... and join PA , PB , CA , CB by arcs of great circles . N A Р B Let the angle ONA = 0 , ON = † , NA = 4 ; then if the angles 0 , 4 , be known , the position 4 THE EARTH'S MOTION OF ROTATION . Signification of the constants of integration.
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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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