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Standard representation of the single-layer potential is as follows: (formula presented), where (formula presented) is an arbitrary function and (formula presented). The function (formula presented) and its derivatives tangential to, are continuous on the surface while its normal derivative has discontinuety: (formula presented). For details see, e.g., G. A. Korn and T. M. Korn, (McGraw-Hill New York, 1968), Chap. 15.6
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Standard representation of the single-layer potential is as follows: (formula presented), where (formula presented) is an arbitrary function and (formula presented). The function (formula presented) and its derivatives tangential to S are continuous on the surface while its normal derivative has discontinuety: (formula presented). For details see, e.g., G. A. Korn and T. M. Korn, Mathematical Handbook for Scientists and Engineers (McGraw-Hill New York, 1968), Chap. 15.6.
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This relation was presented for the first time in Ref., (a), however, with incorrect degree of (formula presented); it is corrected in Ref., (b)
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