From 319e4346b1575370fc8b3557d3f13ed9671e1a92 Mon Sep 17 00:00:00 2001
From: Marcello Seri <marcello.seri@gmail.com>
Date: Wed, 10 Feb 2021 14:56:15 +0100
Subject: [PATCH] Fix typo

Signed-off-by: Marcello Seri <marcello.seri@gmail.com>
---
 hm.tex | 12 ++++++------
 1 file changed, 6 insertions(+), 6 deletions(-)

diff --git a/hm.tex b/hm.tex
index 120f284..f0a4dc0 100644
--- a/hm.tex
+++ b/hm.tex
@@ -136,7 +136,7 @@
 \thispagestyle{empty}
 \null\vfill
 \begin{center}
-    Version 1.3.2\\
+    Version 1.3.3\\
     \today
 \end{center}
 \vfill
@@ -177,7 +177,7 @@ \chapter*{Preface}
 
 Please don't be afraid to send me comments to improve the course or the text and to fix the many typos that will surely be in this first draft. They will be very appreciated.
 
-I am extremely grateful to Anouk Pelzer, Robbert Scholtens and Albert \v{S}ilvans for their careful reading of the notes and their useful comments and corrections.
+I am extremely grateful to Riccardo Bonetto, Anouk Pelzer, Robbert Scholtens and Albert \v{S}ilvans for their careful reading of the notes and their useful comments and corrections.
 
 \chapter{Classical mechanics, from Newton to Lagrange and back}
 
@@ -266,7 +266,7 @@ \subsection{Motion in one degree of freedom}
     Clearly, once we know the initial conditions, the full evolution of the solution $x(t)$ is known, in agreement with Newton's principle of determinacy.
 
     \begin{figure}[ht!]
-        \includegraphics[width=\linewidth]{images/{HM-1.2}.pdf}
+        \includegraphics[width=.9\linewidth]{{images/HM-1.2}.pdf}
     \end{figure}
 
     Consider, now, a point particle of mass $m$ attached to a pivot on the ceiling via a rigid rod of length $l$.
@@ -668,7 +668,7 @@ \subsection{Dynamics of point particles: from Lagrange back to Newton}\label{sec
     \begin{equation}
         \bm{F}_k = -\sum_{j\neq k} \bm{F}_j.
     \end{equation}
-    (Hint: use the invariance with respect to spacial translations.)
+    (Hint: use the invariance with respect to spatial translations.)
 \end{exercise}
 
 \begin{remark}
@@ -910,7 +910,7 @@ \section{Euler-Lagrange equations on smooth manifolds}\label{sec:lagrangianonman
     \end{equation}
     have the form
     \begin{equation}\label{eq:geodesic}
-        \ddot q^k = \Gamma_{ij}^k(q) \dot q^i \dot q^j, \quad k=1,\ldots, n,
+        \ddot q^k + \Gamma_{ij}^k(q) \dot q^i \dot q^j = 0, \quad k=1,\ldots, n,
     \end{equation}
     where $\Gamma_{ij}^k(q)$ are the Christoffel symbols of the Levi-Civita connection associated with the metric $\d s^2$:
     \begin{equation}
@@ -1334,7 +1334,7 @@ \subsection{Back to one degree of freedom, again}\label{sec:1deg-again}
 \begin{figure}[ht]
     \centering
     \includegraphics[width=.75\linewidth,trim={0 50pt 0 50pt},clip]{images/lissajous.pdf}
-    \caption{Some casually selected Lissajous figures. The top right example is a degenerate ellipse squeezed to a line, i.e., a closed curve.}
+    \caption{Some casually selected Lissajous figures. The top right example (in orange) and the one in the center at the bottom (in purple) are degenerate closed curves squeezed to a line.}
     \label{img:lissajous}
 \end{figure}