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| author | Prefetch | 2022-09-27 21:20:05 +0200 |
|---|---|---|
| committer | Prefetch | 2022-09-28 20:51:35 +0200 |
| commit | 03accd13c0a6ec4de2d8001edf3ce7553f831160 (patch) | |
| tree | 59840d0c443752c6fef87f74597e032db91cd219 /content/know/concept/rutherford-scattering/index.pdc | |
| parent | 7e0b6df586da7c79df3853ba0bdc9f98c10af839 (diff) | |
Clean up CSS, minor design changes
Diffstat (limited to 'content/know/concept/rutherford-scattering/index.pdc')
| -rw-r--r-- | content/know/concept/rutherford-scattering/index.pdc | 4 |
1 files changed, 2 insertions, 2 deletions
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 $\vb{r}$, |