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author | Prefetch | 2021-05-27 20:46:01 +0200 |
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committer | Prefetch | 2021-05-27 20:46:01 +0200 |
commit | 4780106a4f191c41d3b82ca9d1327a1c95a72055 (patch) | |
tree | c6a2bd91c5ab9721a008078cafd9e36e608395a0 /content/know/concept/stokes-law/index.pdc | |
parent | d3b96730bd01263098bbb96c15148878e5633a04 (diff) |
Expand knowledge base
Diffstat (limited to 'content/know/concept/stokes-law/index.pdc')
-rw-r--r-- | content/know/concept/stokes-law/index.pdc | 6 |
1 files changed, 4 insertions, 2 deletions
diff --git a/content/know/concept/stokes-law/index.pdc b/content/know/concept/stokes-law/index.pdc index acc98af..dee40d6 100644 --- a/content/know/concept/stokes-law/index.pdc +++ b/content/know/concept/stokes-law/index.pdc @@ -356,8 +356,10 @@ This is an equation for the **terminal velocity** $U_t$, which we find to be as follows: $$\begin{aligned} - U_t - = \frac{2 a^2 (\rho_s - \rho_f) g_0}{9 \eta} + \boxed{ + U_t + = \frac{2 a^2 (\rho_s - \rho_f) g_0}{9 \eta} + } \end{aligned}$$ The falling sphere will accelerate until $U_t$, |