Physical Optics, Part II., Part 2 |
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Page vii
... Velocity of a luminiferous molecule after reflexion , 4 ; of a refracted molecule , 5 ; impulsive forces at the refracting surface - coeffici- ents investigated , 5 ; forms of the luminiferous surfaces in uniaxal crystals , 6 ; ordinary ...
... Velocity of a luminiferous molecule after reflexion , 4 ; of a refracted molecule , 5 ; impulsive forces at the refracting surface - coeffici- ents investigated , 5 ; forms of the luminiferous surfaces in uniaxal crystals , 6 ; ordinary ...
Page viii
... velocity of light in glass from expe- riment , 48 ; radii of Newton's rings , 49 ; when the light is ob- liquely incident , 51 ; interference near the shadow of a body , or diffraction , 52 ; law of the fringes , 53 ; interference ...
... velocity of light in glass from expe- riment , 48 ; radii of Newton's rings , 49 ; when the light is ob- liquely incident , 51 ; interference near the shadow of a body , or diffraction , 52 ; law of the fringes , 53 ; interference ...
Page 3
... velocity of the reflected ray equals that of the incident ray . For a luminiferous molecule which is reflected , we suppose the component of the velocity before incidence parallel to the reflecting surface , equals that after reflexion ...
... velocity of the reflected ray equals that of the incident ray . For a luminiferous molecule which is reflected , we suppose the component of the velocity before incidence parallel to the reflecting surface , equals that after reflexion ...
Page 4
Richard Potter. Letv be the velocity of a luminiferous molecule in the SA , u the velocity of it in the reflected ray AR . ray Then from the above relation of the parallel and perpendicular components we have u sin i ' = v sin i , u cos ...
Richard Potter. Letv be the velocity of a luminiferous molecule in the SA , u the velocity of it in the reflected ray AR . ray Then from the above relation of the parallel and perpendicular components we have u sin i ' = v sin i , u cos ...
Page 5
... velocity of the in- cident molecule , u that of the refracted molecule ; we have sin i = μ sini ' , v = μu . With these data we require to find how the impulsive forces act in directions parallel and perpendicular to the refracting ...
... velocity of the in- cident molecule , u that of the refracted molecule ; we have sin i = μ sini ' , v = μu . With these data we require to find how the impulsive forces act in directions parallel and perpendicular to the refracting ...
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Common terms and phrases
2nd Edit 4th Edit angle of incidence aperture asymptote axis biaxal crystals caustic co-ordinates colours cos³ Crown 8vo curves dark Differential Calculus diffraction distance edge Elementary Treatise elliptically polarized emergent ray English equal equation experiments extraordinary ray F. A. Paley Fcap 8vo figure formula Geometrical Greek hyperbola incident ray integer intensity interference J. W. Donaldson Latin luminiferous molecule luminiferous surface luminous point M.A. 3rd Edition M.A. Fcap maxima nearly Newton's rings object-glass optic axes ordinary ray original polarization outer sheet parallel parallelogram perpendicular plane of analyzation plane of incidence plane of polarization plane of xz plate Post 8vo principal plane PROP reflected light reflecting surface reflexion refracted ray refractive index retardation right angles rings shewn sin² sin³ speculum metal tan² u² cos² undulatory theory uniaxal crystal values velocity whilst μ²
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