CHAPTER IV.
(Supplementary to Chapter II.)
concerning the differential and integral calculus of vectors.
169. If is a vector having continuously varying values in space, and the vector determining the position of a point, we may set
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and regard as a function of or of and Then,
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that is,
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If we set
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Here stands for
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exactly as in No. 52, except that it is here applied to a vector and produces a dyadic, while in the former case it was applied to a scalar and produced a vector. The dyadic represents the nine differential coefficients of the three components of w with respect to and just as the vector (where is a scalar function of ) represents the three differential coefficients of the scalar with respect to and
It is evident that the expressions and already defined (No. 54) are equivalent to and
160. An important case is that in which the vector operated on is of the form We have then
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where
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This dyadic, which is evidently self-conjugate, represents the six