Schwere, Elektricität und Magnetismus:387
Vorlage:Bernhard Riemann - Schwere, Elektricität und Magnetismus Vorlage:PageDef2
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Vorlage:IdtIf we suppose the quantities occurring in the six equations of the last section to be functions of a scalar , we may substitute for in those equations since this is only to divide all
terms by the scalar .
Vorlage:Idt47. Successive differentiations.—The differential coefficient of a vector with respect to a scalar is of course a finite vector, of which we may take the differential, or the differential coefficient with respect to the same or any other scalar. We thus obtain differential coefficients of the higher orders, which are indicated as in the scalar calculus.
Vorlage:IdtA few examples will serve for illustration.
Vorlage:IdtIf is the vector drawn from a fixed origin to a moving point at any time , will be the vector representing the velocity of the point, and the vector representing its acceleration.
Vorlage:IdtIf is the vector drawn from a fixed origin to any point on a curve, and the distance of that point measured on the curve from any fixed point, is a unit vector, tangent to the curve and having the direction in which increases: is a vector directed from a point on the curve to the center of curvature, and equal to the curvature: is the normal to the osculating plane, directed to the side on which the curve appears described counter-clock-wise about the center of curvature, and equal to the curvature. The tortuosity (or rate of rotation of the osculating plane, considered as positive when the rotation appears counter-clock-wise as seen from the direction in which increases,) is represented by
Vorlage:Idt48. Integration of an equation between differentials.—If and are two single-valued continuous scalar functions of any number of scalar or vector variables, and
where is a scalar constant.
Vorlage:References
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