Transactions of the Cambridge Philosophical Society, المجلد 22University Press, 1923 |
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... Jacobian Figure . By R. HARGREAVES , M.A. ... ... ... ... ... ... ... ... ... ... ... PAGE 1 15 39 ... 55 61 ... VI . On the Fifth Book of Euclid's Elements ( Third Paper ) . By M. J. M. HILL , M.A. , LL.D. , Sc.D. , F.R.S. , Astor ...
... Jacobian Figure . By R. HARGREAVES , M.A. ... ... ... ... ... ... ... ... ... ... ... PAGE 1 15 39 ... 55 61 ... VI . On the Fifth Book of Euclid's Elements ( Third Paper ) . By M. J. M. HILL , M.A. , LL.D. , Sc.D. , F.R.S. , Astor ...
الصفحة 60
... JACOBIAN FIGURE BY R. HARGREAVES , M.A. CAMBRIDGE : AT THE UNIVERSITY PRESS M. DCCCC . XIV . ADVERTISEMENT THE Society as a body is not to be TRANSACTIONS The Domains of Steady Motion for a Liquid Ellipsoid, and the Oscillations of ...
... JACOBIAN FIGURE BY R. HARGREAVES , M.A. CAMBRIDGE : AT THE UNIVERSITY PRESS M. DCCCC . XIV . ADVERTISEMENT THE Society as a body is not to be TRANSACTIONS The Domains of Steady Motion for a Liquid Ellipsoid, and the Oscillations of ...
الصفحة 61
... Jacobian Figure . By R. HARGREAVES , M.A. [ Received 8 February 1914. ] ONE of the oscillations of ellipsoidal type for Maclaurin's figure of equilibrium has , at the junction with Jacobi's series , a period exactly one - half that of ...
... Jacobian Figure . By R. HARGREAVES , M.A. [ Received 8 February 1914. ] ONE of the oscillations of ellipsoidal type for Maclaurin's figure of equilibrium has , at the junction with Jacobi's series , a period exactly one - half that of ...
الصفحة 62
... Jacobian , and also for a range of Maclaurin's spheroids on each side of the junction , the periods differ little from the half - day in excess or defect , both cases being represented . The position for spheroids is that the ...
... Jacobian , and also for a range of Maclaurin's spheroids on each side of the junction , the periods differ little from the half - day in excess or defect , both cases being represented . The position for spheroids is that the ...
الصفحة 63
... and y or taking the two axes about which there is no rotation in a different order . The whole field is then a flattened oval , with Maclaurin's line for a line of symmetry 9-2 ELLIPSOID , AND THE OSCILLATIONS OF THE JACOBIAN FIGURE . 63.
... and y or taking the two axes about which there is no rotation in a different order . The whole field is then a flattened oval , with Maclaurin's line for a line of symmetry 9-2 ELLIPSOID , AND THE OSCILLATIONS OF THE JACOBIAN FIGURE . 63.
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a₁ angle approximately asymptotic expansion atmosphere Axiom of Archimedes axis b₁ c₁ calculated coefficients considered constant convergent convex set cordon corresponding cos² curve d₁ definition denote density determined differential equations disturbance diurnal diurnal variations dyadic earth equal escape expression factor finite follows formula free path function G. H. Hardy giant star given h₂ Hence integral equation invariant Jacobian k₁ k₂ magnitude molecules obtained orbit paper parameters partitions plane positive potential Primitive Roots ratio relation respectively result rotation scalar shew shewn sin² solar solid angle solutions substitution suppose surface t₁ theorem theory v₁ values vector velocity w₁ X₁ XXII zero Σ Σ дх