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© 08 D’Net Layton wwwlaytonmusiccom May be copied for teacher or home use.

Vgbg n cxg. (33) where ﬁ(n) is the volume of the unit ball in Rn We see that Φ satisﬁes Laplace’s equation on Rn ¡f0g As we will show in the following claim, Φ satisﬁes ¡∆ xΦ = –0 For this reason, we call Φ the fundamental solution of Laplace’s equation 2. R x > a ` g c w o h n ^ y r x * _ c g b g* t v g* c o a ` g c w o r x a ` g c w o ̖{ ny 瑗 ŉ ϕi ̔. N u a F 731 JWL VIA K i F @4H100 12 C ` 360KG A13 C ` 500KG K JWLT K i K i i13 N V j F12 C ` JWLT480KG A13 C ` JWLT495KG K.

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