Page 47 - Intro to Tensor Calculus
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               EXAMPLE 1.2.2. (Spherical Coordinates) (ρ, θ, φ)
                   Consider the transformation


                         x = x(ρ, θ, φ)= ρ sin θ cos φ  y = y(ρ, θ, φ)= ρ sin θ sin φ  z = z(ρ, θ, φ)= ρ cosθ

               from rectangular coordinates (x, y, z) to spherical coordinates (ρ, θ, φ). By letting


                                                        3
                                                 2
                                          1
                                                                               3
                                                                        2
                                                                 1
                                         y = x, y = y, y = z    x = ρ, x = θ, x = φ
               the above set of equations has the form found in equation (1.2.8) with u = ρ, v = θ, w = φ the generalized
               coordinates. One could place bars over the x s in this example in order to distinguish these coordinates from
                                                      0
               the x s of the previous example. The spherical coordinates (ρ, θ, φ) are illustrated in the figure 1.2-3.
                    0


















                                               Figure 1.2-3. Spherical coordinates.






               Scalar Functions and Invariance

                   We are now at a point where we can begin to define what tensor quantities are. The first definition is
               for a scalar invariant or tensor of order zero.
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