Download Light Scattering Reviews 5: Single Light Scattering and by Alexander A. Kokhanovsky PDF

By Alexander A. Kokhanovsky

Concentrating on radiative move and optics of hugely reflective items, this quantity provides an up to date evaluate of recent mild scattering thought. Numerical strategies in unmarried and a number of gentle scattering are coated, in addition to theoretical experiments.

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Light Scattering Reviews 5: Single Light Scattering and Radiative Transfer (Springer Praxis Books Environmental Sciences)

Concentrating on radiative move and optics of hugely reflective items, this quantity offers an up to date assessment of contemporary gentle scattering idea. Numerical thoughts in unmarried and a number of gentle scattering are lined, in addition to theoretical experiments.

Additional info for Light Scattering Reviews 5: Single Light Scattering and Radiative Transfer (Springer Praxis Books Environmental Sciences)

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However, results are obtained for a single orientation, not random orientation averaging. We consider that these deviations may be caused by specific alignment of monomers for a single orientation, and may disappear for random orientation averaging. We obtained the regression of the relations between N and efficiency values (Qabs and Qsca ). 7. 7. 24 Y. Okada 10 10 10 50 (a) 30 -1 Silicate Pyroxene Amorphous carbon -3 64 256 Silicate Pyroxene Amorphous carbon 10 5 -2 10 (b) 0 Qsca Qabs 10 1 1024 Number of monomers 2 4096 64 256 1024 Number of monomers 4096 Fig.

Curves with different styles correspond to results with different N . 12) show the following two impacts of N : Forward scattering amplitudes at scattering angle of 0◦ for the BPCA and BCCA increase with N . The BCCA shows a larger increase of the amplitudes with N compared with that of the BPCA. , 256–1024). The scattering angle of the bump shifts from 20◦ to 10◦ as N increases. Also the bump becomes sharper for the BPCA with increased N . In the case of the BCCA, the bump is not seen even with N = 1024.

2) The composing particles of an aggregate are called monomers. The size of the monomer is described by the size parameter of the monomer xm (= 2πrm /λ) where rm is the monomer radius, and λ the wavelength of incident light. , μm or nm). 1 Numerical simulations of light scattering 5 The number of monomers composing the aggregate is defined with N . 1 for the equation). The material composition of the aggregate is described by the complex refractive index m = n+ik. k is related to the absorption coefficients of the aggregate defined as 4πk/λ (see Eq.

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