diff --git a/src/3_drude_model_solutions.md b/src/3_drude_model_solutions.md
index b3f5c722de9810ffa3732b209a6639c816eab485..c8561190d7428ea1cc494bdf5d6bed348da88195 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.