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- W1590686199 abstract "In this chapter some of the mathematical ideas of classical potential theory are introduced, under simplifying assumptions. The basic space is Euclidean N space ℝ N . For a ball B( (xi ,delta ) ) in ℝ N $$ begin{gathered} {{l}_{{N - 1}}}(partial B(xi ,delta )) = {{pi }_{N}}{{delta }^{{N - 1}}},quad {{pi }_{N}} = 2{{pi }^{{N/2}}}Gamma {{left( {frac{N}{2}} right)}^{{ - 1}}} hfill {{l}_{N}}(B(xi ,delta )) = frac{{{{pi }_{N}}{{delta }^{N}}}}{N}. hfill end{gathered} $$ (1.1)." @default.
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- W1590686199 date "1984-01-01" @default.
- W1590686199 modified "2023-09-27" @default.
- W1590686199 title "Introduction to the Mathematical Background of Classical Potential Theory" @default.
- W1590686199 doi "https://doi.org/10.1007/978-1-4612-5208-5_1" @default.
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