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By A V Balakrishnan

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Extra info for Advances in communication systems : theory and applications. Volume 2

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In addition, the intensity grows as a result of scattering from other directions into the desired direction at points along the line AB. In constructing a numerical solution, we determine the intensity at multiples of a time increment At. The solution at the previous time increment is used to calculate the contribution at B in Fig. 10. The integral along AB is approximated by a two-point quadrature formula using the known values of the intensity at point B and the unknown values of the intensity at point A.

0, receiver at base of cloud). power. In addition, the total response contains the unscattered radiation and the multiple-scattered radiation. In order to determine the rise characteristics of the total response, a special simulation of the transport equation was made. This simulation placed special stress on the rise characteristics of the scattered radiation. 160 FIG. 21. 3 from base of cloud). 160 FIG. 22. 9 from base of cloud). interval Co < τ < Co/cos Θ (56) which is the same interval as the single-scattered intensity.

17. F. Jenkins and H. White, "Fundamentals of Optics," p. 255. McGraw-Hill, New York, 1957. Stochastic Approximation: A Recursive Method for Solving Regression Problems1 DAVID J. SAKRISON Department of Electrical Engineering, University of California Berkeley, California I. Introduction 51 A. Scope and Advantages of Stochastic Approximation Methods 51 B. Notation and Description of the Methods 53 II. Stochastic Approximation: Mathematical Foundation and Background . . 55 A. The Robbins-Monro Method 56 B.

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