[MITgcm-devel] seaice
Alistair Adcroft
adcroft at mit.edu
Tue Feb 14 10:26:44 EST 2006
Martin,
The code below doesn't look right - the divergence of fluxes should be
split into separate loops and applied consecutively otherwise the scheme
will not be monotonic. Also, be sure to use "forward" time-stepping with
dst2/3. I'm not sure what code you based this on but I hope it wasn't
from gad...
A.
Martin Losch wrote:
> GAD:
>
> I have tried using dst3fl (withoug any explicit diffusion). It runs
> stably for 20 years now, but now my ice (instead of being too little)
> is growing endlessly (37 m in the western Weddell Sea), so I have the
> suspicion that I am make severe mistakes: Could someone who
> understand gad_calc_rhs have a look at the attached routine and tell
> me, if I have done things right? In particular in the update of HEFF,
> is it correct to have advFac=1?:
>
>> DO j=1-Oly,sNy+Oly-1
>> DO i=1-Olx,sNx+Olx-1
>> HEFF(i,j,1,bi,bj)=HEFF(i,j,3,bi,bj) + DELTT *
>> & maskC(i,j,kSurface,bi,bj)*recip_rA(i,j,bi,bj)
>> & *( (fZon(i+1,j)-fZon(i,j))
>> & +(fMer(i,j+1)-fMer(i,j))
>> & -localT(i,j)*( (uTrans(i+1,j)-uTrans(i,j))
>> & +(vTrans(i,j+1)-vTrans(i,j))
>> & )*advFac
>> & )
>
>
> Martin
>
>
>
> On Feb 14, 2006, at 3:57 PM, chris hill wrote:
>
>> Martin,
>>
>> These all sound good.
>> Technically it should be possible to use gad to do the explicit
>> part of ice advection. Jinlun may have comments on whether this
>> makes sense algorithmically and on interactions with the implicit
>> parts of the ice dynamics.
>>
>> Chris
>> Martin Losch wrote:
>>
>>> Hi Dimitris,
>>> I am probably playing too much with the seaice model right now,
>>> but here are a few points that I'd like to make (and maybe check
>>> them in, even if they break lab_sea):
>>> 1. I am now sure that there is a bug in advect.F that does NOT
>>> affect lat-lon-grid simulations, but WILL affect cubed-sphere
>>> simulations and all other irregular grid simulations. It's
>>> basically an idexing error (see my previous email). I think I will
>>> just fix that.
>>> 2. I would like to replace all DXTICE DYTICE SINEICE CSTICE etc
>>> with the proper combination of variables dxF,dxG, etc. from
>>> GRID.h. This will --- at least as far as I can see --- make sure
>>> that the grid information is correct and the same grid parameters
>>> that are used for the ocean are used for seacie.
>>> Since I want to use the seaice model on a cubed sphere grid, I do
>>> care about this. However, this will change the lab_sea and very
>>> like (more dramatically) any cubed sphere set-up that you may have
>>> (I am currently currently playing with global_ocean.cs32x15 +
>>> seaice). Will I get your OK?
>>> 3. Advection schemes: for properties such as volume and fractional
>>> area, the advection scheme should not produce negative (or
>>> positve) overshoots. A 2nd order central difference scheme does
>>> that (eg., can produce negative thicknesses). The scheme in
>>> advect.F is 2nd order central difference, but I don't understand
>>> the time stepping scheme, so it may be OK. Nevertheless, I naively
>>> think, a positive scheme may be better, but it is no longer
>>> conservative, eg. 2n-order with flux limiter (e.g, Hunke's CSIM5
>>> uses MPDATA) or DST3FL that I use routinely for geochemical
>>> tracers. The nice thing is, that all of these schemes are there
>>> (in generic_advdiff), one just needs to pick one. I have tried
>>> dst3fl, but again, I do not understand the time stepping in
>>> advect.F (nor do I understand fully how gad_calc_rhs works): I
>>> have tried dst3fl and I even got it to work, but only halfway. If
>>> I am not mistaken, the DST schemes look as if they are explicit in
>>> time, that is, h(n+1) = h(n) + gh(n)*deltaT. I can compute gh (n),
>>> but for that I need to know what the different time levels are, eg.,
>>> HEFF(:,:,1,:,:) = current time level?
>>> HEFF(:,:,2,:,:) = do I need these?
>>> HEFF(:,:,3,:,:) = ?
>>> Or do I just update HEFF(:,:,1,:,:) in advect.F?
>>> Martin
>>> On Feb 14, 2006, at 2:07 PM, Dimitris Menemenlis wrote:
>>>
>>>> Martin and Jinlun, I am out of my depth when it comes to
>>>> advection schemes. Is there a reason for changing the scheme
>>>> that is there already in pkg/seaice?
>>>>
>>>> For cubed-sphere grid right now, I assumed that grid is
>>>> rectangular near the Poles (CS*ICE=1, TNG*ICE=0). This was a
>>>> quick fix to get going but it is not exact. So maybe that
>>>> explains why you get different numerical values?
>>>>
>>>> Regarding coastal sflux from seaice. One does expect coastal
>>>> regions around Antarctica to be ice/salt factories, but maybe too
>>>> much salt is being rejected. Carl recently send me some slides
>>>> and Ph.D. thesis from Dirk Notz:
>>>> http://ecco.jpl.nasa.gov/~dimitri/Notz/talk_MPI16112005.pdf
>>>> http://ecco.jpl.nasa.gov/~dimitri/Notz/PhD_thesis_Dirk.pdf
>>>> suggesting there is considerable uncertainty regarding how much
>>>> salt is rejected during sea ice creation.
>>>>
>>>> Dimitris
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>>>
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>>
>>
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