Transactions of the Cambridge Philosophical Society, المجلد 22University Press, 1923 |
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الصفحة 7
... corresponding partitions of the bipartite number ( pq ) are those which appertain to the group ( p1 " 1p2 TM 3 ... ) , ( q1 * q ... ) } , which contain exactly ET + 8 parts , the zero bipart 00 not being excluded as a permissible bipart ...
... corresponding partitions of the bipartite number ( pq ) are those which appertain to the group ( p1 " 1p2 TM 3 ... ) , ( q1 * q ... ) } , which contain exactly ET + 8 parts , the zero bipart 00 not being excluded as a permissible bipart ...
الصفحة 9
... corresponding partitions of the bipartite number ( pq ) are those which appertain to the group { ( p1 " p " ... ) , ( q1 × 1q2X2 X2 • ) } , which contain exactly Σ + 8 parts , the zero part 00 not being excluded from being an admissible ...
... corresponding partitions of the bipartite number ( pq ) are those which appertain to the group { ( p1 " p " ... ) , ( q1 × 1q2X2 X2 • ) } , which contain exactly Σ + 8 parts , the zero part 00 not being excluded from being an admissible ...
الصفحة 12
... corresponding partitions of the group zero parts 000 being admissible as parts ; then the numbers found indicate the number of partitions which have no repeated parts . Thus of 2 parts there are 4 partitions in which no part is repeated ...
... corresponding partitions of the group zero parts 000 being admissible as parts ; then the numbers found indicate the number of partitions which have no repeated parts . Thus of 2 parts there are 4 partitions in which no part is repeated ...
الصفحة 36
... corresponding determination of the value of arg is now made in precisely the same manner as in § 8 , subsections ( A ) ... ( D ) . Remembering that the first 1 + h + B ' -b of the coefficients bo , b1 , ... vanish , we see that the ...
... corresponding determination of the value of arg is now made in precisely the same manner as in § 8 , subsections ( A ) ... ( D ) . Remembering that the first 1 + h + B ' -b of the coefficients bo , b1 , ... vanish , we see that the ...
الصفحة 43
... corresponding forces and couples are R ' ( acting upwards through O ' ) = R , - 4πμυα 2 ( 1 − c2 ) S ' = 1 - ης M ' = 4πμυα * ( 1 – c ) n ( 2 + c2 ) 2+ c2 In the first place it is to be noticed that S and S ' are not equal and opposite ...
... corresponding forces and couples are R ' ( acting upwards through O ' ) = R , - 4πμυα 2 ( 1 − c2 ) S ' = 1 - ης M ' = 4πμυα * ( 1 – c ) n ( 2 + c2 ) 2+ c2 In the first place it is to be noticed that S and S ' are not equal and opposite ...
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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