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With these timescale groupings and subsystems defined, we can proceed to analyze the mechanisms underlying the SS solutions.
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These timescales depend on the disk structure.
The definitions of these timescales are described later.
These timescales are small compared to the cooling timescale of a molten layer.
The ratio of these timescales gives us a small dimensionless parameter.
These timescales extend beyond those achievable by laboratory experiments or industrial experience.
Connectivity is dynamic on timescales of a day to a flow season (6 12 weeks), as streamflow varies over these timescales.
We estimate these timescales just in the Stokes law regime because the lift force in other regimes is uncertain.
By comparing these timescales, we obtain the parameter space where the lift force can act on the spinning dust grains.
These timescales range from decades for significant human health risk to 0.5 Myr for D. radiodurans lethality.
Diffusion necessarily exists and one could argue that imposing the FF-hypothesis constraint is not a valid approach at these timescales.
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