A Treatise on Physical OpticsDeighton, Bell, 1892 - 411 páginas |
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Página xiii
... parallel to the axis 136. When the axis is neither parallel nor perpendicular to the plate , the isochromatic curves are curves of the fourth degree 137. Rings produced by two plates cut parallel to the axis , which are superposed ...
... parallel to the axis 136. When the axis is neither parallel nor perpendicular to the plate , the isochromatic curves are curves of the fourth degree 137. Rings produced by two plates cut parallel to the axis , which are superposed ...
Página xvii
... parallel to the plane of polarization · • 253. Crystalline reflection and refraction . Failure of Green's theory to satisfactorily explain this phenomenon 254. Criticisms on Green's theory 255. Suggestion of a theory , which would ...
... parallel to the plane of polarization · • 253. Crystalline reflection and refraction . Failure of Green's theory to satisfactorily explain this phenomenon 254. Criticisms on Green's theory 255. Suggestion of a theory , which would ...
Página xxii
... parallel to the reflector 386 457. Description of the arrangements employed 387 458. Experimental results 387 459. Summary of the experimental results 388 460. Further experiments , giving negative results 388 461. Hall's experiments on ...
... parallel to the reflector 386 457. Description of the arrangements employed 387 458. Experimental results 387 459. Summary of the experimental results 388 460. Further experiments , giving negative results 388 461. Hall's experiments on ...
Página xxiii
... and refraction , when the magnetization is parallel to the reflector 408 • • 485. Theoretical explanation of Kundt's experiments on reflection from glass . 408 486. Concluding remarks 411 ERRATA . Page 33 lines 7 and 8 , read.
... and refraction , when the magnetization is parallel to the reflector 408 • • 485. Theoretical explanation of Kundt's experiments on reflection from glass . 408 486. Concluding remarks 411 ERRATA . Page 33 lines 7 and 8 , read.
Página 10
... parallel to the ray , the properties of a ray would be the same on every side of it ; if however the vibrations were parallel to the wave front , and therefore perpendi- cular to the ray , we should anticipate that the properties of a ...
... parallel to the ray , the properties of a ray would be the same on every side of it ; if however the vibrations were parallel to the wave front , and therefore perpendi- cular to the ray , we should anticipate that the properties of a ...
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Términos y frases comunes
A₁ accordingly amplitude angle of incidence aperture axis bands biaxal crystal centre change of phase circularly polarized colours cos² critical angle diffraction direction of vibration displacement dx dy elastic ellipsoid elliptically polarized equal equations of motion ether extraordinary ray extraordinary wave follows formulæ Fresnel's glass Hence Iceland spar incident light index of refraction integral intensity light is incident light is polarized Lord Rayleigh medium Nicol normal obtain optic axes parallel perpendicular plane of incidence plane of polarization plate of quartz polarized light polarized perpendicularly polarizing angle prism produced quantity quartz reflected and refracted reflected light refracted wave rhomb right-handed rings rotation sin² spectrum suppose surface theory thickness transmitted transparent U₁ uniaxal crystal V₁ values velocity of propagation wave-front wave-length wave-surface whence whilst μ²
Pasajes populares
Página 372 - Nicol's prism turned in any way. [Shown.] (5) The spectrum of the reflected light is frequently found to consist almost entirely of a comparatively narrow band. When the angle of incidence is increased, the band moves in the direction of increasing refrangibility, and at the same time increases rapidly in width. In many cases the reflection appears to be almost total.
Página 356 - The difference between these numbers is greater than can be accounted for by errors of observation, and shows that our theories of the structure of bodies must be much improved before we can deduce their optical from their electrical properties. At the same time, I think that the agreement of the numbers is such that if no greater discrepancy were found between the numbers derived from the optical and...
Página 347 - To fill all space with a new medium whenever any new phenomenon is to be explained is by no means philosophical, but if the study of two different branches of science has independently suggested the idea of a medium, and if the properties which must be attributed to the medium in order to account for electromagnetic phenomena are of the same kind as those which, we attribute to the luminiferous medium in order to account for the phenomena of light, the evidence for the physical existence of the medium...
Página 347 - But the properties of bodies are capable of quantitative measurement. We therefore obtain the numerical value of some property of the medium, such as the velocity with which a disturbance is propagated through it, which can be calculated from electromagnetic experiments, and also observed directly in the case of light. If it should be found that the velocity of propagation of electromagnetic disturbances is the same as the velocity of light, and this not only in air, but in other transparent media,...