Transactions of the Cambridge Philosophical SocietyUniversity Press, 1842 |
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النتائج 1-3 من 17
الصفحة 420
... velocity of propagation in general depends on the length of the wave . In vacuum however C = 0 , and therefore the velocity of propagation does not depend on the length of the wave . Hence the direct action of the particles of matter ...
... velocity of propagation in general depends on the length of the wave . In vacuum however C = 0 , and therefore the velocity of propagation does not depend on the length of the wave . Hence the direct action of the particles of matter ...
الصفحة 426
... propagated with a constant velocity in transparent bodies ; for I have proved that if the velocity be constant , the particles must necessarily vibrate according to the cycloidal law . What the velocity of propagation is , must de- pend ...
... propagated with a constant velocity in transparent bodies ; for I have proved that if the velocity be constant , the particles must necessarily vibrate according to the cycloidal law . What the velocity of propagation is , must de- pend ...
الصفحة 427
... velocity of propagation of a wave spreading from A when it arrives at B , v ' the velocity of propagation of a wave spreading from B when it arrives at C , it is evident that we have ultimately , time of describing EB ' = EB ' v = 8 ...
... velocity of propagation of a wave spreading from A when it arrives at B , v ' the velocity of propagation of a wave spreading from B when it arrives at C , it is evident that we have ultimately , time of describing EB ' = EB ' v = 8 ...
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action algebra angle apse attraction axis bone caloric cause centre co-ordinates coefficients consequently curves cycloidal D'Alembert's Principle density direction distance dp² dt dt dv dw dx dx dx dy dx dy dz dx dz dx² dy dx dy dy dy dz dz dx e-al effect engine equilibrium evident exact differential fluid function Hence hypothesis integral lever-frame light line of motion luminiferous ether material particles medium molecular force obtained optic axes parallel parametric surface perpendicular plane position pressure produce propagation radius refraction respect result Rhynchosaur shew shewn substituting suppose surface of displacement symbol transversal U₁ variation velocity velocity of propagation vibrations wave weight wheels zero αφ аф аф аф