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authorPrefetch2022-01-30 11:27:00 +0100
committerPrefetch2022-01-30 11:27:00 +0100
commit88537b82784f71104c3a2771330c9e492f57fb03 (patch)
tree0d5ddb6adaf9e55892f4e7b79adf1e22cf0aee10 /content/know/concept/lubrication-theory/index.pdc
parent8a9fb5fef2a97af3274290e512816e1a4cac0c02 (diff)
Expand knowledge base, remove comments
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diff --git a/content/know/concept/lubrication-theory/index.pdc b/content/know/concept/lubrication-theory/index.pdc
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+++ b/content/know/concept/lubrication-theory/index.pdc
@@ -124,8 +124,6 @@ Then we insert this into our earlier expression for $v_x$, yielding:
$$\begin{aligned}
v_x
&= 3 y (y - h) \Big( \frac{U}{h^2} - \frac{2 Q}{h^3} \Big) - \frac{U h}{h^2} y + \frac{U h^2}{h^2}
- %\\
- %&= U \frac{3 y (y - h) - h y + h^2}{h^2} - Q \frac{6 y (y - h)}{h^3}
\end{aligned}$$
Which, after some rearranging, can be written in the following form: