The earth's motion of rotation including the theory of precession and nutation |
Inni boken
Resultat 1-5 av 12
Side 3
... Substituting these 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 ...
... Substituting these 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 ...
Side 6
... substituting the 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 ...
... substituting the 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 ...
Side 21
... Substituting these values , and reducing , therefore . 1 k k ( u v ) ds d = √ ( AB ) ( - ) de dh = 1 dl 2 dk ' dl dk - | ( uv ) from above ; 2 dh Again , from equation ( 2 ) , we have GENERAL THEORY OF ROTATION . 21 Recapitulation of ...
... Substituting these values , and reducing , therefore . 1 k k ( u v ) ds d = √ ( AB ) ( - ) de dh = 1 dl 2 dk ' dl dk - | ( uv ) from above ; 2 dh Again , from equation ( 2 ) , we have GENERAL THEORY OF ROTATION . 21 Recapitulation of ...
Side 22
... substituting for dv from equations ( 1 ) , dh do . 2 tan 1 sec2 1 dh also from equation ( 4 ) , = A B - Bv - Au v2 Au Au + Bv tan 4 , sec2 41 = √ ( Au • Bv hence , by substitution , do , 1 dh dl do , therefore = 2 ds dh uv ; du and dh ...
... substituting for dv from equations ( 1 ) , dh do . 2 tan 1 sec2 1 dh also from equation ( 4 ) , = A B - Bv - Au v2 Au Au + Bv tan 4 , sec2 41 = √ ( Au • Bv hence , by substitution , do , 1 dh dl do , therefore = 2 ds dh uv ; du and dh ...
Side 25
... substituting the above value of all dt ' terms not depending upon the disturbing force will dis- appear : thus dl dl dh dl dk dl dv = + + dt dh dt dk dt ds do dh or , substituting the values of and from Arts . 11 and 15 , dl dk dt dt dV ...
... substituting the above value of all dt ' terms not depending upon the disturbing force will dis- appear : thus dl dl dh dl dk dl dv = + + dt dh dt dk dt ds do dh or , substituting the values of and from Arts . 11 and 15 , dl dk dt dt dV ...
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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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