X-Git-Url: https://hackdaworld.org/gitweb/?p=lectures%2Flatex.git;a=blobdiff_plain;f=physics_compact%2Fmath_app.tex;fp=physics_compact%2Fmath_app.tex;h=ec21dae694d53792baf78ca3b974897cb3a1dacd;hp=f1ac777ea2a51d8168b426991d5fca0a05b3e8c1;hb=8e76f77bf1d7e1428796a7cb524a76fd57ca055d;hpb=dc92faa0cd4395778583bf127f5246ae8df275b4

diff --git a/physics_compact/math_app.tex b/physics_compact/math_app.tex
index f1ac777..ec21dae 100644
--- a/physics_compact/math_app.tex
+++ b/physics_compact/math_app.tex
@@ -165,7 +165,7 @@ u_mv_1^* & u_mv_2^* & \cdots & u_mv_n^*\\
 \right)
 \text{ ,}
 \end{equation}
-which can be equivalently obtained by the rulrs of matrix multiplication
+which can be equivalently obtained by the rules of matrix multiplication
 \begin{equation}
 \vec{u}\otimes\vec{v}=\vec{u}\vec{v}^{\dagger} \text{ ,}
 \end{equation}
@@ -180,5 +180,47 @@ holds.
 
 \section{Spherical coordinates}
 
+Cartesian coordinates $\vec{r}(x,y,z)$ are related to spherical coordinates $\vec{r}(r,\theta,\phi)$ by
+\begin{eqnarray}
+x&=&r\sin\theta\cos\phi\textrm{ ,}\\
+y&=&r\sin\theta\sin\phi\textrm{ ,}\\
+z&=&r\cos\theta\textrm{ .}
+\end{eqnarray}
+Infinitesimal translations $dq_i$ and $dq'_i$ of the two coordinate systems are related by the partial derivatives.
+\begin{equation}
+dq_i=\sum_j \frac{\partial q_i}{\partial q'_j}dq'_j
+\end{equation}
+\begin{definition}[Jacobi matrix]
+The matrix J with components
+\begin{equation}
+J_{ij}=\frac{\partial q_i}{\partial q'_j}
+\end{equation}
+is called the Jacobi matrix.
+\end{definition}
+
+For cartesian and spherical coordinates the relation of the translations are presented in detail
+\begin{eqnarray}
+dx&=&\frac{\partial x}{\partial r}dr +
+     \frac{\partial x}{\partial \theta}d\theta +
+     \frac{\partial x}{\partial \phi}d\phi\\
+dy&=&\frac{\partial y}{\partial r}dr +
+     \frac{\partial y}{\partial \theta}d\theta +
+     \frac{\partial y}{\partial \phi}d\phi\\
+dz&=&\frac{\partial z}{\partial r}dr +
+     \frac{\partial z}{\partial \theta}d\theta +
+     \frac{\partial z}{\partial \phi}d\phi\\
+\end{eqnarray}
+and the vector consisting of all or using the Jacobi matrix
+
+
+\begin{equation}
+   =\sin\theta\cos\phi dr + \\
+\end{equation}
+
+To obtain infinitesimal 
+\begin{definition}[Jacobi matrix]
+
+\end{definition}
+
 \section{Fourier integrals}