Transactions of the Cambridge Philosophical SocietyUniversity Press, 1830 |
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الصفحة 246
... pipe , length = 2na + s , n being any whole number . Let now the secondary interval = 2a - s , a similar process ... pipe ( s ) to reed ( a ) , the same will be produced by a pipe 2nas . No. 8 . ea o o a e a o o a e a o Hence if a given ...
... pipe , length = 2na + s , n being any whole number . Let now the secondary interval = 2a - s , a similar process ... pipe ( s ) to reed ( a ) , the same will be produced by a pipe 2nas . No. 8 . ea o o a e a o o a e a o Hence if a given ...
الصفحة 254
... pipe will vibrate in the well known manner of a common organ - pipe . We should obtain a similar result if the pipe had been taken equal to any multiple of the wave . 1 1 But if B be open , the alternate portions BB , BB , & c . will be ...
... pipe will vibrate in the well known manner of a common organ - pipe . We should obtain a similar result if the pipe had been taken equal to any multiple of the wave . 1 1 But if B be open , the alternate portions BB , BB , & c . will be ...
الصفحة 260
Cambridge Philosophical Society. of density , at different parts of the pipe . We have seen , that when the pipe was equal to the half wave , or its odd multiples , that the variation of density took place as in a common organ- pipe ...
Cambridge Philosophical Society. of density , at different parts of the pipe . We have seen , that when the pipe was equal to the half wave , or its odd multiples , that the variation of density took place as in a common organ- pipe ...
المحتوى
by THOMAS JARRETT Esq B A | 65 |
Theory of Escapements by G B AIRY Esq M A | 105 |
On the Pressure produced on a flat Plate when opposed to a Stream | 129 |
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