From 27f1ce55f8b561618dbf493b2bc7b213c23c0d31 Mon Sep 17 00:00:00 2001
From: Joris van Winden <j.vanwinden@student.tudelft.nl>
Date: Sun, 7 Feb 2021 15:00:17 +0000
Subject: [PATCH] Apply 1 suggestion(s) to 1 file(s)
---
src/3_drude_model_solutions.md | 2 +-
1 file changed, 1 insertion(+), 1 deletion(-)
diff --git a/src/3_drude_model_solutions.md b/src/3_drude_model_solutions.md
index b3f5c722..c8561190 100644
--- a/src/3_drude_model_solutions.md
+++ b/src/3_drude_model_solutions.md
@@ -19,7 +19,7 @@ $R_{xy}$ = $-\frac{B}{ne}$, so it does not depend on the sample geometry.
If hall resistance and magnetic field are known, the charge density is calculated from $R_{xy} = -\frac{B}{ne}$.
-As $V_x = -\frac{I_x}{ne}B$, a stronger field makes large Hall voltages easier to measure.
+As $V_x = -\frac{I_x}{ne}B$, a stronger field makes Hall voltages easier to measure.
3.
--
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