Question #41684

show that the curvilnear coordinate system defined by the following equations is orthogonal. x=uvcosØ,
y=uvsinØ, z=1/2(u^2-v^2)

Expert's answer

Answer on Question #41684 – Math – Analytic Geometry


r⃗=(Xyz)=(uvcos⁡(α)uvsin⁡(α)12(u2−v2))\vec{r} = \begin{pmatrix} X \\ y \\ z \end{pmatrix} = \begin{pmatrix} uv\cos(\alpha) \\ uv\sin(\alpha) \\ \frac{1}{2}(u^2 - v^2) \end{pmatrix}


Derivatives of the radius vector:


r⃗u=(xuyuzu)=(vcos⁡(α)vsin⁡(α)u);r⃗v=(xvyvzv)=(ucos⁡(α)usin⁡(α)−v);r⃗α=(xαyαzα)=(−uvsin⁡(α)uvcos⁡(α)0);\vec{r}_u = \begin{pmatrix} x_u \\ y_u \\ z_u \end{pmatrix} = \begin{pmatrix} v\cos(\alpha) \\ v\sin(\alpha) \\ u \end{pmatrix}; \vec{r}_v = \begin{pmatrix} x_v \\ y_v \\ z_v \end{pmatrix} = \begin{pmatrix} u\cos(\alpha) \\ u\sin(\alpha) \\ -v \end{pmatrix}; \vec{r}_\alpha = \begin{pmatrix} x_\alpha \\ y_\alpha \\ z_\alpha \end{pmatrix} = \begin{pmatrix} -uv\sin(\alpha) \\ uv\cos(\alpha) \\ 0 \end{pmatrix};


Scalar products:


r⃗u⋅r⃗v=uvcos⁡2(α)+uvsin⁡2(α)−uv=0\vec{r}_u \cdot \vec{r}_v = uv\cos^2(\alpha) + uv\sin^2(\alpha) - uv = 0r⃗u⋅r⃗α=−uv2cos⁡(α)sin⁡(α)+uv2cos⁡(α)sin⁡(α)=0\vec{r}_u \cdot \vec{r}_\alpha = -uv^2\cos(\alpha)\sin(\alpha) + uv^2\cos(\alpha)\sin(\alpha) = 0r⃗v⋅r⃗α=−u2vcos⁡(α)sin⁡(α)+u2vcos⁡(α)sin⁡(α)=0\vec{r}_v \cdot \vec{r}_\alpha = -u^2v\cos(\alpha)\sin(\alpha) + u^2v\cos(\alpha)\sin(\alpha) = 0


It means that r⃗u,r⃗v\vec{r}_u, \vec{r}_v and r⃗α\vec{r}_\alpha can be chosen as a basis and these vectors are orthogonal.

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