Enkuklopadeia

Cogito, ergo sum

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notebooks:peclet_number [2025/02/14 10:41] – rishabhsteinnotebooks:peclet_number [Unknown date] (current) – external edit (Unknown date) 127.0.0.1
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 \text{Pe} = \frac{\tau_D}{\tau_A} = \frac{v_0 l_0}{D} \text{Pe} = \frac{\tau_D}{\tau_A} = \frac{v_0 l_0}{D}
 \end{equation} \end{equation}
-For larger length scales ($\text{Pe} \gg 1$), flow in the system is naturally advection-dominated, while for smaller $l_0$,  $\text{Pe}$ is $\ll1$; therefore, diffusion dominates the transport phenomenon. [[hatisthis]]+For larger length scales ($\text{Pe} \gg 1$), flow in the system is naturally advection-dominated, while for smaller $l_0$,  $\text{Pe}$ is $\ll1$; therefore, diffusion dominates the transport phenomenon.