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 $\vb{r}$, -- cgit v1.2.3