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This does look wrong to me. The stability function plot also makes it clear that the fluxes should decrease if the stability parameter increases. Something that is missing is a plot of the stability parameter that comes out of the flux computation. That might be one place to start for figuring out what's going wrong here... |
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Thanks for reporting this @mmr0 and sorry that it took me some time to address this. Uᴳ = β * cbrt(Jᵇ * h_bℓ)In the above, U = sqrt(Δu^2 + Δv^2 + Uᴳ^2))so even when there is no large-scale velocity difference between the ocean and the atmosphere, there is always a small scale (turbulent) velocity that generates turbulent exchange of heat and vapor. I have opened an issue from this discussion which is definitely a bug. |
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Awesome thanks @simone-silvestri for looking into this - the new plot in #748 looks much better! |
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Hi,
I have been reading the awesome docs on interface fluxes, but am perplexed by the bottom panel of this figure figure:

As far as I understand the example, the atmosphere specific humidity is set to be equal to the surface saturation humidity, so there should be no vapor fluxes. So I would expect the sign of the air-sea temperature difference ΔT to set the sign of the buoyancy flux. Also as per my understanding and also the text:
So I'm confused as to why a large positive ΔT of 20K corresponding to a stabilising buoyancy flux would lead to an increased drag coefficient?
Thanks in advance for any comments/clarifications!
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