On the Undulatory Theory of Optics: Designed for the Use of Students in the UniversityMacmillan, 1866 - 159 σελίδες |
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Σελίδα 5
... side we have ( x , t ) = ( x , t ) + d . ( x , t ) dx d . ( x , t ) vt ' + t ' + & c . , dt d.p ( x , t ) , d . ( x , t ) or v + 4 -0 , dx dt the general solution of which gives い( x , t ) = ( vtx ) * . $ 7. This expression however is ...
... side we have ( x , t ) = ( x , t ) + d . ( x , t ) dx d . ( x , t ) vt ' + t ' + & c . , dt d.p ( x , t ) , d . ( x , t ) or v + 4 -0 , dx dt the general solution of which gives い( x , t ) = ( vtx ) * . $ 7. This expression however is ...
Σελίδα 18
... side AB towards CD : and suppose that the line EF passes through a number of points which are simultaneously in the same phase : then EF is a front of a wave . If at the same time GH be another line passing through a number of points ...
... side AB towards CD : and suppose that the line EF passes through a number of points which are simultaneously in the same phase : then EF is a front of a wave . If at the same time GH be another line passing through a number of points ...
Σελίδα 27
... side ) to spread through the room in the same manner as a sound coming in the same direction and through the same hole . The answer appears in the results of the last investigation the length of the waves of air is much greater than the ...
... side ) to spread through the room in the same manner as a sound coming in the same direction and through the same hole . The answer appears in the results of the last investigation the length of the waves of air is much greater than the ...
Σελίδα 29
... sides were dx , dy , dz , now occupies the parallelopiped , nearly rectangular , whose sides are dx ( 1 + dx ) , dy ( 1 + 1 ) , 81⁄2 ( 1 + dz ) . δε And if the elasticity ( represented by the pressure upon a unit of surface ) was ...
... sides were dx , dy , dz , now occupies the parallelopiped , nearly rectangular , whose sides are dx ( 1 + dx ) , dy ( 1 + 1 ) , 81⁄2 ( 1 + dz ) . δε And if the elasticity ( represented by the pressure upon a unit of surface ) was ...
Σελίδα 31
... side of the perpendicular : and the front of the wave will be B'C'D ' , making with the wall the same angle as BCD , but on the opposite side : the extent of vibration & c . remaining as be- fore . And this appears to justify us ...
... side of the perpendicular : and the front of the wave will be B'C'D ' , making with the wall the same angle as BCD , but on the opposite side : the extent of vibration & c . remaining as be- fore . And this appears to justify us ...
Άλλες εκδόσεις - Προβολή όλων
Συχνά εμφανιζόμενοι όροι και φράσεις
2π λ a² cos² Algebra analyzing plate angle of incidence aperture axis BROOKE FOSS WESTCOTT Cambridge cloth coefficient common light Consequently Crown 8vo dicular different colours direction displacement distance disturbance double refraction ELEMENTARY TREATISE elliptically polarized English equal equation ether explain expression Extra fcap extraordinary ray fcap find the intensity Fresnel's rhomb front glass Iceland spar integral intensity of light investigation Latin length Mathematical motion nearly Newton's rings ordinary ray original particles pencil perpen perpendicular phænomena plane of incidence plane of polarization plane of reflection polarized light position principal plane prism produced Professor PROP proportion radius reflected ray represented retardation rhombohedron Schools screen Second Edition seen shews similar sin² suppose surface tion tourmaline undulation uniaxal crystal velocity vibration vibrations perpendicular vt-x λ 2π λό όλ
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