Transactions of the Cambridge Philosophical Society, المجلد 22University Press, 1923 |
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النتائج 1-5 من 39
الصفحة 28
... maximum when 0 < t < 1 , viz . when 1 - tM : = R ( x ) ' provided that R ( x ) > l . Consequently if R ( x ) and 1 + 1 we have le ( 1 - tM ) exp { R ( x ) . ( tM − 1 ) } < < - when 0 < t < 1 . R ( x ) So that if be fixed , K e - Ex ( x ...
... maximum when 0 < t < 1 , viz . when 1 - tM : = R ( x ) ' provided that R ( x ) > l . Consequently if R ( x ) and 1 + 1 we have le ( 1 - tM ) exp { R ( x ) . ( tM − 1 ) } < < - when 0 < t < 1 . R ( x ) So that if be fixed , K e - Ex ( x ...
الصفحة 42
... maximum and minimum pressure are equidistant from the point of nearest approach , and the one value rises above the value of the pressure at that point by as much as the other value falls below it . It remains to calculate the resultant ...
... maximum and minimum pressure are equidistant from the point of nearest approach , and the one value rises above the value of the pressure at that point by as much as the other value falls below it . It remains to calculate the resultant ...
الصفحة 47
... maximum pressure is displaced nearer to the point of closest approach ; ( 3 ) the position of the minimum pressure is displaced further from that point . Steady Flow of Air under Pressure . In the same way that the steady flow of liquid ...
... maximum pressure is displaced nearer to the point of closest approach ; ( 3 ) the position of the minimum pressure is displaced further from that point . Steady Flow of Air under Pressure . In the same way that the steady flow of liquid ...
الصفحة 49
... maximum pressure the agreement is not so good in figure 5. In connection with the differences which still remain it needs to be pointed out that the theory is based on the assumption of an infinitely long bearing . In particular the ...
... maximum pressure the agreement is not so good in figure 5. In connection with the differences which still remain it needs to be pointed out that the theory is based on the assumption of an infinitely long bearing . In particular the ...
الصفحة 51
... Maximum pressure given by Pmax . - II = 3μ U ( do - d1 ) 2dod1 ( do + d1 ) - In the extension to the case of elastic ... maximum pressure , we notice that when dp dx = 0 , 6μ Uph = k Hence the position a1 of the maximum pressure is given ...
... Maximum pressure given by Pmax . - II = 3μ U ( do - d1 ) 2dod1 ( do + d1 ) - In the extension to the case of elastic ... maximum pressure , we notice that when dp dx = 0 , 6μ Uph = k Hence the position a1 of the maximum pressure is given ...
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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