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Huygens-Fresnel principle

As one can see from relation (13.112), the wavefield at the point r D may be viewed at the moment of time t as the sum of elementary fields of point and dipole sources distributed over the surface S with densities dP r,t)/dn and P r,t) respectively. The interference of these fields beyond the domain D results in complete suppression of the total wavefield. Thus, the Kirchhoff integral formula can be treated as the mathematical formulation of the classical physical Huygens-Fresnel principle. [Pg.417]

Huygens-Fresnel principle Every point on a primary wavefront serves as the source of secondary wavelets such that the wavefront at some later time is the envelope of these wavelets. [Pg.230]

Of interest is the light intensity measured on plane II, located a distance / from plane I. Huygen s principle simply states that the field at plane II is the sum of spherical waves emanating from all points in plane I. However, the field at point A will be primarily influenced by the spherical wave at point A, with a similar relationship between the fields at points B and B. Fresnel s extension of Huygen s principle quantifies this statement. The spherical wave emanating from a differential area, dS, located at point A is... [Pg.68]

We can use Huygens principle to explain qualitatively the essential features of diffraction, but a quantitative treatment involves casting Huygens principle into a precise mathematical form, the Fresnel-Kirchhoff formula ... [Pg.13]


See other pages where Huygens-Fresnel principle is mentioned: [Pg.508]    [Pg.74]    [Pg.391]    [Pg.230]    [Pg.231]    [Pg.378]    [Pg.508]    [Pg.74]    [Pg.391]    [Pg.230]    [Pg.231]    [Pg.378]    [Pg.67]    [Pg.159]    [Pg.74]    [Pg.78]    [Pg.16]    [Pg.16]    [Pg.230]    [Pg.248]    [Pg.356]   
See also in sourсe #XX -- [ Pg.417 ]

See also in sourсe #XX -- [ Pg.74 , Pg.78 ]

See also in sourсe #XX -- [ Pg.391 ]




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