Mathematical and Physical Papers, Volume 2University Press, 1883 - Hydrodynamics |
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Page 6
... N draw a plane A perpendicular to PN , and project w on this plane by a circum- scribing cylindrical surface . Suppose h greater than the radius r of the sphere of activity of the molecular forces , 6 NOTES ON HYDRODYNAMICS .
... N draw a plane A perpendicular to PN , and project w on this plane by a circum- scribing cylindrical surface . Suppose h greater than the radius r of the sphere of activity of the molecular forces , 6 NOTES ON HYDRODYNAMICS .
Page 13
... greater . This is just the conclusion to which we are led quite independently , from dynamical principles of the greatest generality , combined with the observed phenomena of optics * . * See the introduction to an admirable memoir by ...
... greater . This is just the conclusion to which we are led quite independently , from dynamical principles of the greatest generality , combined with the observed phenomena of optics * . * See the introduction to an admirable memoir by ...
Page 25
... greater than the focal length when the luminous point is not very distant . Let C be a point in the object - glass , situated in the middle of the interval between the two streams , and let the intensity be required at a point M , near ...
... greater than the focal length when the luminous point is not very distant . Let C be a point in the object - glass , situated in the middle of the interval between the two streams , and let the intensity be required at a point M , near ...
Page 32
... greater as T is more nearly equal to To , for which particular value the minima are absolutely black . ❤ Secondly , suppose the breadths h , k of the two streams to be equal as before , but suppose the streams separated by an interval ...
... greater as T is more nearly equal to To , for which particular value the minima are absolutely black . ❤ Secondly , suppose the breadths h , k of the two streams to be equal as before , but suppose the streams separated by an interval ...
Page 33
... greater of the two , h , k . As T increases to 2T - T ,, the vividness of the bands remains unchanged ; and as T increases from 27 - T1 to 2T - T ,, the vividness decreases by the same steps as it before in- creased . When T - 2T - T ...
... greater of the two , h , k . As T increases to 2T - T ,, the vividness of the bands remains unchanged ; and as T increases from 27 - T1 to 2T - T ,, the vividness decreases by the same steps as it before in- creased . When T - 2T - T ...
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17 Paternoster Row angle of incidence aperture arbitrary constants astigmatic attraction axis bands bridge calculated centre Clairaut's Theorem coefficient College considered cos² Demy 8vo denote density determined direction displacement distance disturbance earth edition equal equation error exact differential experiments expression finite fluid force formula function given glass gravity grooved face Hence incident light integral intensity limits luminiferous ether mass medium motion nearly negative Newton's Rings observed obtained particle perpendicular plane of diffraction plane of incidence plane of polarization plate portion positive prism Professor quantity radius vector reflected refraction refractive index regard respect result sensible shew sin² spectrum St John's College suppose supposition surface of equilibrium T₁ theorem theory tion University of Cambridge vanishes velocity of propagation vertical vibrations vis viva zero
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