On the Undulatory Theory of Optics: Designed for the Use of Students in the University |
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... reflected and refracted rays , & c . , though generally probable , I conceive to be far from certain . " The plan of this Tract has therefore been to include those phænomena only which admit of calculation . Many subjects are thus ...
... reflected and refracted rays , & c . , though generally probable , I conceive to be far from certain . " The plan of this Tract has therefore been to include those phænomena only which admit of calculation . Many subjects are thus ...
Page
... reflected and refracted rays , & c . , though generally probable , I conceive to be far from certain . " The plan of this Tract has therefore been to include those phænomena only which admit of calculation . Many subjects are thus ...
... reflected and refracted rays , & c . , though generally probable , I conceive to be far from certain . " The plan of this Tract has therefore been to include those phænomena only which admit of calculation . Many subjects are thus ...
Page 27
... reflected from a large surface ( which amounts nearly to the same thing ) it is hardly sensible except in front of the open- ing , or in the direction of reflection . 29. Our conclusion with regard to light is also important as removing ...
... reflected from a large surface ( which amounts nearly to the same thing ) it is hardly sensible except in front of the open- ing , or in the direction of reflection . 29. Our conclusion with regard to light is also important as removing ...
Page 28
... not plane . PROP . 9. To explain the reflection of light on the undu- latory theory . 31. We shall again refer to the motion of sound for an analogical illustration of this point . In fig . 7 28 UNDULATORY THEORY OF OPTICS .
... not plane . PROP . 9. To explain the reflection of light on the undu- latory theory . 31. We shall again refer to the motion of sound for an analogical illustration of this point . In fig . 7 28 UNDULATORY THEORY OF OPTICS .
Page 29
... whose sides were h , k , l , the excess of pressure which urges it on in the direction of x is -P d 2 ( 1 -m dx = mPhkl dX dY dz - m dx dy m h.kl dz d / dx dY dz + + dx dx dy dz any part of this wave , as BCD , has REFLECTION OF LIGHT . 29.
... whose sides were h , k , l , the excess of pressure which urges it on in the direction of x is -P d 2 ( 1 -m dx = mPhkl dX dY dz - m dx dy m h.kl dz d / dx dY dz + + dx dx dy dz any part of this wave , as BCD , has REFLECTION OF LIGHT . 29.
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Common terms and phrases
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 dx dy ELEMENTARY TREATISE elliptically polarized English equal equation ether explain expression Extra fcap extraordinary ray fcap 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 velocity vibration vibrations perpendicular vt-x λατ λό όλ
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