From 03accd13c0a6ec4de2d8001edf3ce7553f831160 Mon Sep 17 00:00:00 2001
From: Prefetch
Date: Tue, 27 Sep 2022 21:20:05 +0200
Subject: Clean up CSS, minor design changes

---
 content/know/concept/rutherford-scattering/index.pdc | 4 ++--
 1 file changed, 2 insertions(+), 2 deletions(-)

(limited to 'content/know/concept/rutherford-scattering/index.pdc')

diff --git a/content/know/concept/rutherford-scattering/index.pdc b/content/know/concept/rutherford-scattering/index.pdc
index c89b477..d91ae40 100644
--- a/content/know/concept/rutherford-scattering/index.pdc
+++ b/content/know/concept/rutherford-scattering/index.pdc
@@ -25,7 +25,7 @@ Coulomb repulsion causes 1 to deflect by an angle $\theta$,
 and pushes 2 away in the process:
 
 <a href="two-body.png">
-<img src="two-body.png" style="width:50%;display:block;margin:auto;">
+<img src="two-body.png" style="width:50%">
 </a>
 
 Here, $b$ is called the **impact parameter**.
@@ -75,7 +75,7 @@ we can see that $v_x$ is unchanged for any given $\pm t$,
 while $v_y$ simply changes sign:
 
 <a href="one-body.png">
-<img src="one-body.png" style="width:60%;display:block;margin:auto;">
+<img src="one-body.png" style="width:60%">
 </a>
 
 From our expression for $\vb{r}$,
-- 
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