Transactions of the Cambridge Philosophical SocietyUniversity Press, 1842 |
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النتائج 1-3 من 83
الصفحة 345
... obtain , kams kamd r ( 1 + d ) 2 + r ( 1 + 8 ) * + - 약 . ( 1-8 ) . Substituting now this value in the approximate expression for we get d3 x g dx 1-8 + i'dt 1 + d = - df ghað ̧ ( 1–3 ) e ̄ * , e ̄ ‚ rl dt * I have already obtained this ...
... obtain , kams kamd r ( 1 + d ) 2 + r ( 1 + 8 ) * + - 약 . ( 1-8 ) . Substituting now this value in the approximate expression for we get d3 x g dx 1-8 + i'dt 1 + d = - df ghað ̧ ( 1–3 ) e ̄ * , e ̄ ‚ rl dt * I have already obtained this ...
الصفحة 382
... obtained when udx + vdy + wdz is an exact differential , as it manifestly ought to be . The general expression for inclusive of all the cases in which that differential is exact , would be obtained by integrating the equation , аф dt + ...
... obtained when udx + vdy + wdz is an exact differential , as it manifestly ought to be . The general expression for inclusive of all the cases in which that differential is exact , would be obtained by integrating the equation , аф dt + ...
الصفحة 431
... obtained from the equations sin 4 = μ2 sin $ 2 , sin sin y2 = sin 2 sin ( i − 2 ) ' -- will be the greatest angle at which the light emerges from the prism . M - Thus we may obtain - , which will be the whole dispersion produced by the ...
... obtained from the equations sin 4 = μ2 sin $ 2 , sin sin y2 = sin 2 sin ( i − 2 ) ' -- will be the greatest angle at which the light emerges from the prism . M - Thus we may obtain - , which will be the whole dispersion produced by the ...
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