From: hackbard <hackbard@hackdaworld.org>
Date: Wed, 30 May 2012 07:37:04 +0000 (+0200)
Subject: new stuff
X-Git-Url: https://hackdaworld.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=8e76f77bf1d7e1428796a7cb524a76fd57ca055d;p=lectures%2Flatex.git

new stuff
---

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}
 
diff --git a/physics_compact/mech.tex b/physics_compact/mech.tex
index e67554c..92f85f0 100644
--- a/physics_compact/mech.tex
+++ b/physics_compact/mech.tex
@@ -1,2 +1,8 @@
 \part{Classical mechanics}
 
+\chapter{Lagrangian mechanics}
+
+\section{Variational principle}
+
+\chapter{Theory of relativity}
+
diff --git a/physics_compact/phys_comp.tex b/physics_compact/phys_comp.tex
index 674c88e..7a7d0b2 100644
--- a/physics_compact/phys_comp.tex
+++ b/physics_compact/phys_comp.tex
@@ -38,7 +38,7 @@
 \usepackage{miller}
 
 % in use?
-\usepackage{slashbox}
+%\usepackage{slashbox}
 
 % smaller captions ...
 \usepackage[small,bf]{caption}
diff --git a/physics_compact/qm.tex b/physics_compact/qm.tex
index bf8b2ee..6b8c6c4 100644
--- a/physics_compact/qm.tex
+++ b/physics_compact/qm.tex
@@ -49,3 +49,9 @@ Moreover, equality in \eqref{sec:vm_f} is only achieved if $|\tilde 0\rangle$ co
 
 \chapter{Quantum dynamics}
 
+\chapter{Relativistic quantum mechanics}
+
+285 Schulten
+
+
+