Download Handbook of Optics, Third Edition Volume V: Atmospheric by Michael Bass, Casimer DeCusatis, Jay Enoch, Vasudevan PDF
By Michael Bass, Casimer DeCusatis, Jay Enoch, Vasudevan Lakshminarayanan, Guifang Li, Carolyn MacDonald, Virendra Mahajan, Eric Van Stryland
The main finished and up to date optics source to be had ready less than the auspices of the Optical Society of the United States, the 5 conscientiously architected and cross-referenced volumes of the guide of Optics, 3rd version, comprise every little thing a scholar, scientist, or engineer calls for to actively paintings within the box. From the layout of advanced optical structures to world-class learn and improvement equipment, this definitive book offers extraordinary entry to the basics of the self-discipline and its maximum minds. person chapters are written via the world's most famed specialists who clarify, illustrate, and remedy the whole box of optics. each one quantity includes a entire bankruptcy directory for the total guide, vast bankruptcy glossaries, and a wealth of references. This pioneering paintings deals exceptional assurance of optics info, concepts, and purposes. quantity V covers atmospheric optics, modulators, fiber optics, and x-ray and neutron optics.
Read or Download Handbook of Optics, Third Edition Volume V: Atmospheric Optics, Modulators, Fiber Optics, X-Ray and Neutron Optics PDF
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Extra resources for Handbook of Optics, Third Edition Volume V: Atmospheric Optics, Modulators, Fiber Optics, X-Ray and Neutron Optics
This ratio (not the front aperture/sample distance) determines the solid angle of this receiver configuration. The FOV is determined by the clear aperture of the lens, which must be kept larger than the illuminated spot on the sample. The Fig. 3b design is unsuitable for near specular measurement because the relatively broad collimated specular beam will scatter from the receiver lens for several degrees from specular. It is also limited in measuring large incident angle situations where the elongated spot may exceed the FOV.
There are three obvious choices for making wavelength scans. Filters (variable or discrete) can be employed at the source or receiver. 20 Details of these techniques are beyond the scope of this discussion; however, a couple of generalities will be mentioned. Even though these measurements often involve relatively large bandwidths at a given wavelength (compared to a laser), the NEBSDF is often larger by a few orders because of the smaller incident power. Further, because the bandwidths change differently between the various source types given above, meaningful measurement comparisons between instruments are often difficult to make.
The geometry is shown in Fig. 1. The value qs is the polar angle in the scatter direction measured from reflector normal and Ω is the differential solid angle (in steradians) through which dPs (watts) scatters when Pi (watts) is incident on the reflector. The cosine comes from the definition of radiance and may be viewed as a correction from the actual size of the scatter source to the apparent size (or projected area) as the viewer rotates away from surface normal. The details of the derivation do not impact scatter instrumentation, but the initial assumptions and the form of the result do.