Hi all,

Here, a few articles about cloudiness changes over the Arctic and Northern
Eurasia (in addition to Schweiger, GRL, 2004):

http://journals.ametsoc.org/doi/abs/10.1175/JCLI3439.1
http://www.agu.org/pubs/crossref/2007/2007GL030042.shtml
http://journals.ametsoc.org/doi/abs/10.1175/2010JCLI3492.1
http://iopscience.iop.org/1748-9326/6/3/035202/


Actually, there is a strong contradiction among different datasets on
cloudiness trend over this region.


2011/10/17 John Nissen <[email protected]>

> Hi all,
>
> This email from 21st September (see below) seems relevant to our
> discussions at the workshop.  Cloud effects are extremely important to SRM
> geoengineering and its application to cooling the Arctic, which we discussed
> on the second day of the workshop.  Therefore I hope the geoengineering list
> moderator will allow me to post this message to the group.
>
> Fortunately we did have a cloud expert at the meeting - Jon Egill
> Kristjansson.  He told us that there was up to 90% cloud cover over the
> Arctic in summer.  This is important for calculating the overall heat flux
> that the SRM geoengineering has to oppose in achieving an overall cooling of
> the Arctic.  A central purpose of the workshop was to provide an estimate of
> the SRM negative flux (i.e. cooling effect) to be achieved - but the
> estimate does not have to be accurate - only sufficiently accurate in the
> upper end of the range of values for engineering purposes.
>
> If the cloud cover has increased since pre-industrial times, then the total
> heat flux change calculation could be affected by this increase.  The cloud
> in summer is likely to have an cooling effect, whereas cloud in winter is
> certainly having a warming effect.  What is the overall effect? This needs
> investigation.  Does anybody have an idea on this?  Note that any cooling
> effect of the cloud, giving a negative feedback effect at certain times of
> the year, would be important if we could enhance it.
>
> At the meeting we looked at the graphs of sea ice extent.  We noticed a
> definite bounce effect on sea ice extent: after years of larger downturn in
> sea ice extent, there was an upturn in the following year, and vice versa.
>  This could perhaps be explained by an overall negative feedback effect of
> cloud: in years of greater sea ice retreat (downturn in sea ice extent),
> there would be more cooling at the end of the summer as more open water was
> exposed to evaporation - and this cooling would allow a greater volume of
> sea ice to form for the following year.
>
> However the alternative explanation for the bounce effect is that the
> negative feedback comes from black body radiation: as the sea ice retreats
> there is better radiative transfer of heat into space, because the water is
> warmer than the ice.  This was the preferred explanation at the meeting.
>
> Now let's go back to heat flux calculation.  If, on average over the year,
> the cloud is having an overall positive feedback effect, it increases the
> amount of flux that is going to be required by the SRM geoengineering to
> cool the Arctic.  So this one important thing to know from the engineer's
> viewpoint.
>
> Another thing to know is that the increased cloud has different
> significance depending on the SRM technique.  With stratospheric aerosols,
> the cloud cover factor should cancel out - the reduction in SRM effect by
> the cloud is balanced by the reduction in insolation from the sun.  Or
> looking at it another way, the aerosols are high up, so their sunshade
> cooling effect is equally over the whole area below them, whether there are
> clouds there or not.  For cloud brightening techniques, it is simply good
> news to have more clouds to brighten!  What proportion of summer clouds in
> the Arctic can be brightened?  It would be useful to know.
>
> We discussed both cloud brightening and cloud removal techniques.  One of
> the nice things about cloud removal is that it more directly opposes the
> thermal radiation trapping effect of increased CO2.  Jon Egill had done
> modelling in exploring the balance of the two techniques.  I shall put
> copies of his and other presentations into the [arctic-methane] yahoo group
> as a file.
>
> Again for cloud removal we need to know the proportion of clouds that could
> be removed by the technique, especially in winter.
>
> Cheers,
>
> John
>
> ---
>
> On 21/09/2011 12:54, John Nissen wrote:
>
>>
>> Hi Stephen,
>>
>> It's good news that you can do the brightening so far north.  But I'm
>> quite worried about the warming effect of clouds in autumn and winter.  As
>> the sea ice is retreating, there is more open water for evaporation, water
>> vapour production and cloud formation for the autumn, slowing the
>> reformation of the sea ice.  As the sun lowers, the heat trapping of clouds
>> becomes more important than the reflection of insolation.  Could David
>> Mitchell's idea of cloud dispersal have some merit at this time of year?
>>
>> So I am wondering whether we should invite a cloud expert to the workshop.
>>  According to this [1], the cloud cover has been increasing - and
>> approximately linearly up to the last date of measurement they show, 2005 -
>> but hardly at all in the North Atlantic where currents flow into the Arctic
>> ocean.  The trends are provided by Axel Schweiger, of the Washington Polar
>> Science Center [2], who is currently investigating the effect of sea ice
>> changes on cloud cover.  (I am therefore copying this email to him.)
>>
>> According to [3] the water vapour heat-trapping effect may be more
>> important than the overall effect of cloud cover changes.  To quote: "Here
>> we show that the Arctic warming is strongest at the surface during most of
>> the year and is primarily consistent with reductions in sea ice cover.
>> Changes in cloud cover, in contrast, have not contributed strongly to recent
>> warming. Increases in atmospheric water vapour content, partly in response
>> to reduced sea ice cover, may have enhanced warming in the lower part of the
>> atmosphere during summer and early autumn."
>>
>> Of course, as the Arctic warms, the atmosphere is capable of holding more
>> water vapour, so this is a positive feedback.  Does anybody have an idea of
>> the magnitude/significance of this, especially relative to the sea ice
>> albedo effect?
>>
>> BTW, the surface amplification of temperature graphs of [3] support a
>> polar amplification of two, whereas others are talking of Arctic temperature
>> increases commensurate with a polar amplification factor closer to six.
>>
>> Cheers,
>>
>> John
>>
>> [1] 
>> http://www.arctic.noaa.gov/**detect/climate-clouds.shtml<http://www.arctic.noaa.gov/detect/climate-clouds.shtml>
>>
>> [2] http://psc.apl.washington.edu/**wordpress/response-of-cloud-**
>> cover-to-changes-in-sea-ice/<http://psc.apl.washington.edu/wordpress/response-of-cloud-cover-to-changes-in-sea-ice/>
>>
>> [3] http://www.nature.com/nature/**journal/v464/n7293/full/**
>> nature09051.html<http://www.nature.com/nature/journal/v464/n7293/full/nature09051.html>
>>
>> ---
>>
>> On 17/09/2011 16:55, Stephen Salter wrote:
>>
>>>  John
>>>
>>> You say that you do not want to rely on cloud brightening because of
>>> effects on the gulf stream and affect Europe. I do not want to rely on any
>>> single tool.   But in the summer we can do cloud brightening north of the
>>> lattitude Novaya Zemlya without affecting  Europe.  The long hours of summer
>>> sunlight make the technique very powerful.  If we did need to operate south
>>> of this line we could limit the effect to sea temperatures to the values we
>>> had in happier times.   If there was another Pinatubo or if we over do it
>>> then we stop in a few days.
>>>
>>> Stephen
>>>
>>> Emeritus Professor of Engineering Design
>>> Institute for Energy Systems
>>> School of Engineering
>>> Mayfield Road
>>> University of Edinburgh EH9  3JL
>>> Scotland
>>> Tel +44 131 650 5704
>>> Mobile 07795 203 195
>>> www.see.ed.ac.uk/~shs
>>>
>>>
>>>  On 13/09/2011 20:26, John Nissen wrote:
>>>>
>>>>>
>>>>> Dear Stephen, Peter,
>>>>>
>>>>> 1. Meeting discussions
>>>>>
>>>>> Yes, please bring drawings, Stephen. We are meeting at my home, so it
>>>>> will be a fairly informal affair, to allow maximum brainstorming and
>>>>> discussion! Anything you can let me have beforehand would be appreciated,
>>>>> because I want to be able to steer the discussion sensibly. Also I want to
>>>>> draft a working paper before the meeting, and then be able to slot in
>>>>> contributions/decisions easily.
>>>>>
>>>>> Also bring stuff about the cloud brightening. I would also like to have
>>>>> somebody to discuss stratospheric aerosols, because I think the 
>>>>> geographical
>>>>> distribution of the negative forcing effects is going to be crucial,
>>>>> especially to cool the ESAS where the methane seems to be in the most
>>>>> critical state. I'm copying this to Brian Launder, who worked on the RS
>>>>> report under John Shepherd, and might have some ideas. Your welcome to the
>>>>> workshop, Brian - 15-16 October - let me know if you're interested.
>>>>>
>>>>> I'd be very concerned to rely too much on cloud brightening, because to
>>>>> produce upwards of 1 petawatt cooling, you'd have to cool the Gulf Stream
>>>>> and North Atlantic currents by a significant amount - potentially 
>>>>> affecting
>>>>> weather in Europe perhaps - opening up a can of worms!
>>>>>
>>>>>
>>>>> 2. East Siberian Arctic Shelf (ESAS)
>>>>>
>>>>> This does seem to be the most critical area for the methane, with 50 Gt
>>>>> of the stuff that could be emitted at any time, e.g. as the result of an
>>>>> earthquake (and this is a real hazard).
>>>>>
>>>>> Just in case you've not got it, I attach the Shakhova and Semiletov
>>>>> paper, which describes the situation of the ESAS very graphically. Indeed,
>>>>> because the whole area was flooded/inundated as the sea level rose, from 
>>>>> its
>>>>> low level at the last glacial maximum (LGM) about 100-120 metres below
>>>>> current level, you can see what the seabed looks like! You can also see 
>>>>> the
>>>>> approximate sizes of the places where methane is coming out, etc.
>>>>>
>>>>> Note that the authors talk about 5 degrees warming in the region (air
>>>>> temperature presumably), and 3 degrees warming of the water! It's the
>>>>> warming of the water is particularly dangerous. I don't know how we can
>>>>> easily cool it. Can we do anything with local clouds? Could we try
>>>>> brightening the water with clouds of bubbles, as somebody suggested on the
>>>>> geoengineering list?
>>>>>
>>>>> BTW, it's amazing that people (who should know better) are still
>>>>> talking about polar amplification as a doubling of global warming. It's
>>>>> clear to me that Arctic warming is accelerating relative to global 
>>>>> warming,
>>>>> so the amplification factor is increasing all the time, and must be well
>>>>> over six by now. So Hadley models that put 16 degrees in the Arctic for 4
>>>>> degrees global warming are rubbish (- and anyway they ignore the 
>>>>> methane). I
>>>>> think it's basically the albedo flip that's doing the amplification now -
>>>>> the subject of my paper to the EGU in April, Stephen. Let's pray that
>>>>> there's not a methane excursion in the next few years and the sea ice
>>>>> doesn't retreat faster than PIOMAS trend!
>>>>>
>>>>>
>>>>> 3. Fluxes into Arctic and your comment
>>>>>
>>>>> Stephen, by "current TO" I assume you mean "turn over". This is what I
>>>>> was talking about, when I said:
>>>>>
>>>>>  * /Warming is driven by currents from the Atlantic and the albedo
>>>>>    effect/.
>>>>>
>>>>>
>>>>> The main driver turns out to be the albedo flip effect, which I've
>>>>> labelled 'F' in my calculations. In order to ascertain the forces we are 
>>>>> up
>>>>> against in geoengineering, I've tried to calculate the various heat 
>>>>> fluxes.
>>>>> 'S' is the extra heat flux from the Atlantic since pre-industrial times,
>>>>> taking into account that the flow into the Arctic is balanced by flow 
>>>>> coming
>>>>> out, in what is termed AMOC - the overturning circulation.
>>>>>
>>>>> I could have added the local greenhouse effect, 'C' to the warming
>>>>> effect. There is also a cooling effect, 'R', of thermal radiation from the
>>>>> open water as the sea ice retreats, but these are relative small fluxes 
>>>>> and
>>>>> roughly cancel out.
>>>>>
>>>>> And there are some other factors, I asked about recently: the extra
>>>>> water vapour from the open water (positive forcing), the extra cloud cover
>>>>> (positive forcing) and the extra snow to increase albedo (negative 
>>>>> forcing).
>>>>> I've so far neglected these other factors. And I've ignored atmospheric 
>>>>> heat
>>>>> transfer - water vapour transport into the Arctic could perhaps be a
>>>>> significant positive forcing. Otherwise I would expect the total 
>>>>> atmospheric
>>>>> heat transport if anything to diminish, since the Arctic has warmed 
>>>>> relative
>>>>> to the rest of the world.
>>>>>
>>>>> The rest of this email is copied from a previous email about the flux
>>>>> calculation. But I may have underestimated the albedo flip effect, F, 
>>>>> when I
>>>>> wrote it.
>>>>>
>>>>> --
>>>>>
>>>>> Let significant fluxes (extra since pre-industrial times) be identified
>>>>> as follows:
>>>>> S = Gulf Stream warming via North Atlantic Drift heat transport into
>>>>> Arctic [1];
>>>>> C = local warming - net effect of gases and aerosols, mainly CO2 at
>>>>> present;
>>>>> F = albedo Flip effect, where snow and ice has given way to land
>>>>> surface and sea;
>>>>> R = thermal Radiation into space as Arctic surfaces warm [2];
>>>>> L = Latent heat for melting ice;
>>>>> W = heat absorbed by land, water and atmosphere, as Arctic warms.
>>>>>
>>>>> The balance of input flux minus output flux goes into melting the ice
>>>>> and raising the Arctic temperature.
>>>>>
>>>>> Thus S + C + F - R = L + W
>>>>>
>>>>> The geoengineering negative forcing (aka cooling) has to counter S + C
>>>>> + F - R.
>>>>>
>>>>> S is difficult to estimate.But it is observed that the water entering
>>>>> the Fram Strait from the Atlantic has warmed by about 2 degrees C [3]. I 
>>>>> am
>>>>> not sure about the flow volume rate into the Arctic Ocean, but it could be
>>>>> about 6 Sv [4].Note that the paper [5] gives 2-3 Sv into Fram Strait and 
>>>>> 2-3
>>>>> Sv through the Barents Sea Opening (BSO).(1 Sv, or sverdrup, is a million
>>>>> cubic metres of water per second).This is small compared to the Gulf 
>>>>> Stream,
>>>>> at 55 Sv.
>>>>>
>>>>> The figure of 2 degrees warming, observed in [3], is not throughout the
>>>>> depth of the water, so cannot be used for calculating the heat flux.But
>>>>> fortunately there are some figures for the heat transfer from [5]: about 
>>>>> 20
>>>>> terawatts through the Fram Strait and 50 through BSO, giving a total of 70
>>>>> terawatts for a total current of 5 Sv.
>>>>>
>>>>> Now we’d expect the NADW from the Arctic to be the same flow as the
>>>>> flow into the Arctic, and this is given as just under 25 Sv in [6] (table
>>>>> 4).The Gulf Stream is 55 Sv [4], so it is reasonable that just under half
>>>>> goes towards the Arctic and returns as NADW.
>>>>>
>>>>> If 5 Sv is giving 70 terawatts from [5], but we have 25 Sv from [6],
>>>>> then the total warming, S, could be as much as 350 terawatts.
>>>>>
>>>>> In the formula S + C + F - R = L + W, I've estimated the parameters as
>>>>> follows:
>>>>>
>>>>> S = 70-350 terawatts, from Gulf Stream;
>>>>> C = 35 terawatts, from current greenhouse warming over Arctic;
>>>>> F* = 300-1000 terawatts, from the albedo flip when sea ice has gone;
>>>>> R = 34 terawatts, thermal radiation into space as Arctic warms (using
>>>>> [2]);
>>>>> L = 10 terawatts; and
>>>>> W is derivable from the other parameters.
>>>>>
>>>>> --
>>>>>
>>>>> Cheers,
>>>>>
>>>>> John
>>>>>
>>>>> [1] 
>>>>> http://www.sciencedaily.com/**releases/2011/01/110127141659.**htm<http://www.sciencedaily.com/releases/2011/01/110127141659.htm>
>>>>>
>>>>> [2] 
>>>>> http://en.wikipedia.org/wiki/**Stefan%E2%80%93Boltzmann_law<http://en.wikipedia.org/wiki/Stefan%E2%80%93Boltzmann_law>
>>>>>
>>>>> [3] http://instaar.colorado.edu/~**marchitt/reprints/**
>>>>> spielhagenscience11.pdf<http://instaar.colorado.edu/~marchitt/reprints/spielhagenscience11.pdf><
>>>>> http://instaar.colorado.edu/%**7Emarchitt/reprints/**
>>>>> spielhagenscience11.pdf<http://instaar.colorado.edu/%7Emarchitt/reprints/spielhagenscience11.pdf>>
>>>>>
>>>>>
>>>>> /These results reveal a rapid warming by ~2°C of uppermost AWin the FSB
>>>>> in the Arctic Gateway during the past ~120 years, consistent with the
>>>>> documented sea ice retreat in the Barents Sea (//5//), terrestrial
>>>>> Paleoclimate reference records (//6//, //19//) (Fig. 3, C to E), and
>>>>> atmospheric measurements./
>>>>>
>>>>> [4] http://www3.ncc.edu/faculty/**bio/fanellis/biosci119/**
>>>>> currents.html<http://www3.ncc.edu/faculty/bio/fanellis/biosci119/currents.html>
>>>>> This has excellent maps showing currents.
>>>>>
>>>>> [5] 
>>>>> ftp://ftp.npolar.no/ASOF/**library/pdf/Karcher_etal.pdf<ftp://ftp.npolar.no/ASOF/library/pdf/Karcher_etal.pdf>
>>>>>
>>>>> [6] 
>>>>> http://www.atmos.ucla.edu/~**hbrix/papers/brix03jgr.pdf<http://www.atmos.ucla.edu/~hbrix/papers/brix03jgr.pdf><
>>>>> http://www.atmos.ucla.edu/%**7Ehbrix/papers/brix03jgr.pdf<http://www.atmos.ucla.edu/%7Ehbrix/papers/brix03jgr.pdf>
>>>>> >
>>>>>
>>>>> [7] From 1975:
>>>>> http://www.sciencedirect.com/**science/article/pii/**0012821X76900728<http://www.sciencedirect.com/science/article/pii/0012821X76900728>
>>>>> “The rate of Atlantic bottom water formation is estimated at 18
>>>>> Sverdrups”
>>>>>
>>>>> ---
>>>>>
>>>>> On 13/09/2011 10:13, Stephen Salter wrote:
>>>>>
>>>>>> John
>>>>>>
>>>>>> I think that warming is driven by current TO not from the Arctic. All
>>>>>> the water that goes in must come out but the in flow is warmer than the 
>>>>>> out
>>>>>> flow.
>>>>>>
>>>>>> Do you want me to bring drawings and calculations about a scheme for
>>>>>> methane recovery?
>>>>>>
>>>>>> Stephen
>>>>>>
>>>>>>
>>>>>> Emeritus Professor of Engineering Design
>>>>>> Institute for Energy Systems
>>>>>> School of Engineering
>>>>>> Mayfield Road
>>>>>> University of Edinburgh EH9 3JL
>>>>>> Scotland
>>>>>> Tel +44 131 650 5704
>>>>>> Mobile 07795 203 195
>>>>>> www.see.ed.ac.uk/~shs
>>>>>>
>>>>>> On 12/09/2011 23:50, John Nissen wrote:
>>>>>>
>>>>>>>
>>>>>>> Dear all,
>>>>>>>
>>>>>>> I need to check figures - especially the 20 W/m-2 figures - before I
>>>>>>> send more widely. And I'd like to put petawatts against the methane, so 
>>>>>>> we
>>>>>>> have a total petawatt figure for geoengineering to counter! Anything 
>>>>>>> else
>>>>>>> missing?
>>>>>>>
>>>>>>> Any other comments? Should I consider 'considerations' at all for an
>>>>>>> agenda? Do the figures have to be justified here - or can I do that in a
>>>>>>> separate document, with references?
>>>>>>>
>>>>>>> Should I mention that any rise in methane emissions will affect the
>>>>>>> carbon budget for CO2 emissions reductions to meet the 2 (or now 1.5?)
>>>>>>> degree C global warming target limit?
>>>>>>>
>>>>>>> Cheers,
>>>>>>>
>>>>>>> John
>>>>>>>
>>>>>>> --
>>>>>>>
>>>>>>> Agenda for Arctic methane workshop
>>>>>>>
>>>>>>> Considerations:
>>>>>>>
>>>>>>>  * Arctic warming is much faster than global warming, and the
>>>>>>>    warming is accelerating
>>>>>>>  * Warming is driven by currents from the Atlantic and the albedo
>>>>>>>    effect
>>>>>>>  * The extra heat flux, which is warming the Arctic with respect to
>>>>>>>    its pre-industrial temperature, is currently of the order of one
>>>>>>>    petawatt
>>>>>>>  * September sea ice volume trend is to zero in 2015, by which time
>>>>>>>    the heat flux could be of the order of two petawatts, ignoring
>>>>>>>    increased methane emissions
>>>>>>>  * Around 1600 Gt carbon is held in terrestrial permafrost
>>>>>>>  * Around 30% of this permafrost could thaw by 2050, producing
>>>>>>>    mainly methane
>>>>>>>  * Methane being a potent greenhouse gas, the corresponding global
>>>>>>>    forcing could rise to over 20 Watts/m², compared to current net
>>>>>>>    forcing of 1.6 Watts/m²
>>>>>>>  * Under shallow seas there is around 500 Gt carbon in sub-sea
>>>>>>>    permafrost, 1000 Gt methane as methane hydrate and 700 Gt
>>>>>>>    methane as free gas
>>>>>>>  * Up to 50 Gt of this methane could be released “at any time”
>>>>>>>    (e.g. by an earthquake), increasing atmospheric concentration by
>>>>>>>    up to 11 times
>>>>>>>  * The global forcing from such a pulse could rise to around 20
>>>>>>>    Watts/m² over the course of a single year and then fall only
>>>>>>> slowly
>>>>>>>  * Such forcing could send global warming over 2 degrees C in a
>>>>>>> decade
>>>>>>>  * Such forcing would also lead to further Arctic methane release
>>>>>>>    in a positive feedback loop, with the prospect of runaway global
>>>>>>>    warming, disintegration of Greenland and Antarctic ice sheets
>>>>>>>    and many metres of sea level rise
>>>>>>>
>>>>>>>
>>>>>>> The objectives of the workshop are to:
>>>>>>>
>>>>>>>  * ascertain the scale of the methane excursion threat and
>>>>>>>    probability over time;
>>>>>>>  * ascertain the scale of the local engineering and regional
>>>>>>>    (geo)engineering required to prevent a significant methane
>>>>>>>    excursion;
>>>>>>>  * propose a set of techniques which could meet these requirements;
>>>>>>>  * propose techniques to capture methane in the event of an
>>>>>>> excursion;
>>>>>>>  * decide on priorities for trials and deployment of key
>>>>>>> technologies;
>>>>>>>  * agree a plan for preparations and pilot trials according to
>>>>>>>    these priorities;
>>>>>>>  * agree an outline report to AGU in December.
>>>>>>>
>>>>>>>
>>>>>>> Agenda:
>>>>>>>
>>>>>>>  * Introductions of participants
>>>>>>>  * Terrestrial and marine methane threats
>>>>>>>  * Local methane management/engineering ideas
>>>>>>>  * Regional (geo)engineering – cooling technologies and capabilities
>>>>>>>  * Mixed technology strategy to optimise cooling distribution
>>>>>>>  * Methane air capture
>>>>>>>  * Preparation of project plans for preparation, trial and timely
>>>>>>>    deployment
>>>>>>>  * Agree outline report for presentation at AGU
>>>>>>>
>>>>>>>
>>>
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>


-- 
Alexander V. Chernokulsky
A.M.Obukhov Institute of Atmospheric Physics, Russian Academy of Sciences
3 Pyzhevsky, 119017 Moscow, Russia
Tel.: 7 (495) 951 64 53
Fax: 7 (495) 953 16 52
E-mail: [email protected], [email protected]

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