Vector Analysis And the Theory of Relativity

Cover Vector Analysis And the Theory of Relativity
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In ordinary space, i.e., where the a;'s are rectangular Cartesian coordinates and where the y's are orthogonal co- ordinates, /ii = in-' a result which is sometimes useful in the calculation of the coefficients /n, /22, /as • • • of the form (ds)^ in the curvilinear coordinates y.
3. Resolution of tensors If we consider any comriant tensor Xr of rank one and take the inner product of this into a direction tensor Z^""^ we derive the invariant Xrl^^^ (r umbral; Rule (d)). This we call the resolve
...d part of the co variant tensor along the direction l^''\ Let us now make a transformation of coordinates from x to y and consider the .coordinate line y^'\ The n components of the direction tensor for this curve are proportional to a^) ir=h--:n) To determine the actual values of these components we must divide through by the positive square root of ^""a^aT^ am umbral) and this is equivalent to A^.
58 VECTOR ANALYSIS AND RELATIVITY The equations defining the covariant correspondence for a tensor of the first rank are Yi = -X'r^ (l = I, ■ ■ ■ , n; r umbral) = A^ times the resolved part of the tensor Xr along the co- ordinate direction y^^^ Example Space polar coordinates y in ordinary space of three dimensions.


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