From 7c594db2d2561679b257dbcf6780070f91fa4bb4 Mon Sep 17 00:00:00 2001
From: "T. van der Sar" <t.vandersar@tudelft.nl>
Date: Mon, 4 Feb 2019 15:04:52 +0000
Subject: [PATCH] Update 3_drude_model.md

---
 src/3_drude_model.md | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

diff --git a/src/3_drude_model.md b/src/3_drude_model.md
index c335735b..e596f6ff 100644
--- a/src/3_drude_model.md
+++ b/src/3_drude_model.md
@@ -85,7 +85,7 @@ where $R_{\rm H}=-\frac{1}{ne}$ is the _Hall coefficient. So by measuring the Ha
 While most materials have $R_{\rm H}>0$, interestingly some materials are found to have $R_{\rm H}<0$. This would imply that the charge carriers either have a positive charge, or a negative mass. We will see later (chapter 17) how to interpret this.
 
 ## Exercises
-### Exercise 1
+### Exercise 1: Extracting quantities from basic Hall measurements
 We apply a magnetic field $\bf B$ perpendicular to a planar sample that sits in the $xy$ plane. The sample has width $W$ in the $y$-direction, length $L$ in the $x$-direction and we apply a current $I$ along $x$.
 
   1. Suppose we measure a Hall voltage $V_H$. Express the Hall resistance $R_{xy} = V_H/I$ in terms of the Hall resistivity $\rho_{xy}$. Also express $R_{xy}$ in terms of the Hall coefficient $R_H$.
-- 
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