Transactions of the Cambridge Philosophical Society, المجلد 22University Press, 1923 |
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الصفحة
... of a Cylindrical Bearing under Variable Load , and of a Pivot Bearing . By W. J. HARRISON , M.A. , Fellow of Clare College , Cambridge ... ... 361 ... 373 0311 .234 V22 602775 PAGE P 425 XIX . On Integers which satisfy the.
... of a Cylindrical Bearing under Variable Load , and of a Pivot Bearing . By W. J. HARRISON , M.A. , Fellow of Clare College , Cambridge ... ... 361 ... 373 0311 .234 V22 602775 PAGE P 425 XIX . On Integers which satisfy the.
الصفحة 15
... variable . Let f ( x ) be a function defined by Taylor's series f ( x ) = co + c1x + Сqx2 + ... , .. ( 1 ) , and let it be possible to define a function ( s ) , which is analytic in certain regions ( to be specified presently ) of the ...
... variable . Let f ( x ) be a function defined by Taylor's series f ( x ) = co + c1x + Сqx2 + ... , .. ( 1 ) , and let it be possible to define a function ( s ) , which is analytic in certain regions ( to be specified presently ) of the ...
الصفحة 17
... variables x and y and also of a variable integer k . 3 . PART I. Preliminary asymptotic formulae . Let us define the integral function + Ex ( x ) by the series , 00 Ex ( x ) = 2 = Xn n = 0 г ( n + k + 1 ) where k is a ( large ) integer ...
... variables x and y and also of a variable integer k . 3 . PART I. Preliminary asymptotic formulae . Let us define the integral function + Ex ( x ) by the series , 00 Ex ( x ) = 2 = Xn n = 0 г ( n + k + 1 ) where k is a ( large ) integer ...
الصفحة 40
... variable speed and variable load on the lubrication of a cylindrical bearing is taken into account . Case of Incompressible Liquid . In proceeding to determine the equations which give the motion and the pressure of a film of liquid ...
... variable speed and variable load on the lubrication of a cylindrical bearing is taken into account . Case of Incompressible Liquid . In proceeding to determine the equations which give the motion and the pressure of a film of liquid ...
الصفحة 41
... variable distance between the surfaces and is a function of x . Since the surfaces are nearly parallel v will be small compared with u , and the rate of variation of u in the direction of a will be very small compared with its rate of ...
... variable distance between the surfaces and is a function of x . Since the surfaces are nearly parallel v will be small compared with u , and the rate of variation of u in the direction of a will be very small compared with its rate of ...
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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