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Basic Photometric Quantities

In spectroscopic applications of light sources it is very useful to define some characteristic quantities of the emitted and absorbed radiation. This allows a proper comparison of different light sources and detectors, and enables one to make an appropriate choice of apparatus for a particular experiment. [Pg.15]

The radiant energy W (measured in joules) refers to the total amount of energy emitted by a light source, transferred through a surface, or collected by a detector. The radiant power or radiant flux O [W] is the radiant [Pg.17]

The above three quantities refer to the total radiation integrated over the whole spectrum. Their spectral versions W (v), 3 (v), and p (v) are called the spectral densities and are defined as the amounts of W, O, or p within the unit frequency interval dv = 1 s around the frequency v. [Pg.17]

Consider a unit surface element dA = l m of a light source (Fig.2.6). The [Pg.18]

An important quantity is the radiant intensity I = / L dA of the source. This represents the flux per unit solid angle from the entire source [W ster ]. The total flux is then [Pg.18]

All samples in this chapter are assumed to consist of multiple scattering and fluorescent planar layers of arbitrary thickness d. One surface of the layer is irradiated monochromatically at A with parallel light ofintensity /o (per unit area perpendicular to the direction of propagation) under the angle ao relative to the normal of the surface [Pg.224]


See other pages where Basic Photometric Quantities is mentioned: [Pg.224]    [Pg.16]    [Pg.17]    [Pg.19]    [Pg.16]    [Pg.17]    [Pg.19]    [Pg.15]    [Pg.16]    [Pg.17]    [Pg.19]    [Pg.15]    [Pg.17]    [Pg.224]    [Pg.16]    [Pg.17]    [Pg.19]    [Pg.16]    [Pg.17]    [Pg.19]    [Pg.15]    [Pg.16]    [Pg.17]    [Pg.19]    [Pg.15]    [Pg.17]    [Pg.78]    [Pg.203]    [Pg.214]    [Pg.149]   


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Photometric

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