Transactions of the Cambridge Philosophical SocietyUniversity Press, 1912 |
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الصفحة 12
... formula sin απ . . ( 8 ) , COS aπ ... .. ( 9 ) . So x Ja ( x ) sin mx dx = - 2a√πT г ( } − a ) ( m2 − 1 ) a + } ' - ( n > 1 , − } < n < } ) - given by Sonine * . Our formulae are valid provided only m > 1 and the integral is con ...
... formula sin απ . . ( 8 ) , COS aπ ... .. ( 9 ) . So x Ja ( x ) sin mx dx = - 2a√πT г ( } − a ) ( m2 − 1 ) a + } ' - ( n > 1 , − } < n < } ) - given by Sonine * . Our formulae are valid provided only m > 1 and the integral is con ...
الصفحة 12
... formula of Euler's from it t 00 [ * ° * ° Ja ( mx ) e ̄ * æodx * We note that = - a + 1 , − m2 ) ... ( 12 ) , 2 We have only to replace Ja ( ma ) by its expression as a series This formula fails us for small values of 7 , but , by the ...
... formula of Euler's from it t 00 [ * ° * ° Ja ( mx ) e ̄ * æodx * We note that = - a + 1 , − m2 ) ... ( 12 ) , 2 We have only to replace Ja ( ma ) by its expression as a series This formula fails us for small values of 7 , but , by the ...
الصفحة 12
... formula holds for a + p > -1 . If also p < the integral is convergent in the ordinary sense * . §14 . Now let us , in the general integral suppose and Then G [ * $ ( x ) F ( x ) dr . F = Σar " , ( r ) = Ja ( mx ) xo . ¥ ( 7 ) ...
... formula holds for a + p > -1 . If also p < the integral is convergent in the ordinary sense * . §14 . Now let us , in the general integral suppose and Then G [ * $ ( x ) F ( x ) dr . F = Σar " , ( r ) = Ja ( mx ) xo . ¥ ( 7 ) ...
الصفحة 13
Cambridge Philosophical Society. Our proof a formula which contains a very large number of interesting particular cases . involves only that the integral should be convergent at the lower limit , i.e. that a > 0 . If y - a - B > -1 the ...
Cambridge Philosophical Society. Our proof a formula which contains a very large number of interesting particular cases . involves only that the integral should be convergent at the lower limit , i.e. that a > 0 . If y - a - B > -1 the ...
الصفحة 19
... formula which we obtain by integrating [ F ( x ) mix dx ( n > 0 ) round the contour formed by the positive parts of the real and imaginary axes and a very large quadrant of a circle , supposing the integrals along the axes convergent in ...
... formula which we obtain by integrating [ F ( x ) mix dx ( n > 0 ) round the contour formed by the positive parts of the real and imaginary axes and a very large quadrant of a circle , supposing the integrals along the axes convergent in ...
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عبارات ومصطلحات مألوفة
a₁ absolutely convergent applied asymptotic B₁ bounded function bracket C₂ CAMBRIDGE concomitant consider continuous function convergent corresponding cos² curve denote differential coefficient differential equation dx² elastic equal expression factor finite follows formula ƒ x Hence impact infinite integrand irreducible k₁ Lebesgue integral Lemma linear monotone monotone function obtain operator oscillation P₁ plastic positive pressure prove R₁ reciprocant repeated integrals respect result s₁ satisfied sequence shew solution summable suppose symbols theorem theory transformation U₂ uniformly uniformly convergent unique limit upper V₁ values variables velocity W. H. Young w₁ zero α₁ ах дг ди др ду дх მყ
مقاطع مشهورة
الصفحة 280 - We know, however, that this integral is also equal to the sum of the residues at the poles of the integrand /
الصفحة 286 - The sum of the residues at the poles of the last factor, which occurs in (13.18) is therefore equal to minus the sum of the residues at the poles of the other factors.
الصفحة 358 - Since the modulus of a sum is not greater than the sum of the moduli...
الصفحة 96 - In support of such an hypothesis we may remark that as the crystalline grains are built up from their various centres, there will in general be a certain number of molecules to spare between their surfaces ; and these molecules will evidently be distributed in the spaces between the grains with relatively small density, ie, in such a fluid or serai-fluid condition, as would just account for the viscous reaction required.
الصفحة 140 - ... the same properties as the forms upon which they effectively operate, and that the forms which are invariant and the operators are properly to be regarded as one system of forms possessing the same properties.
الصفحة 312 - A geometrical progression is a series in which the ratio of any term to the preceding term is the same for all terms of the series.
الصفحة 126 - Plemelj's canonical form for the principal part of the solving function of an integral equation of the second kind in the neighbour hood of a pole.
الصفحة 48 - would prove independent of the length of the rods, provided the velocity and other conditions of the impact were kept unchanged. This was found to be the case, so that, by plotting duration of impact against length of rods, a straight line was obtained, whose slope gave the required value of the wave-velocity. * " On the Effects of Momentary Stresses in Metals,
الصفحة 348 - Rules for determining when the process of reversing the order of integration in a repeated integral is allowable.
الصفحة 100 - We are concerned here with the variation of integral forms, or more specially with their invariance, under the action of an operator which is an extension of the hydrodynamical operator in Enler's equations.