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

[2] 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

---

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

[2] http://en.wikipedia.org/wiki/Stefan%E2%80%93Boltzmann_law

[3] http://instaar.colorado.edu/~marchitt/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
This has excellent maps showing currents.

[5] 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/%7Ehbrix/papers/brix03jgr.pdf>

[7] From 1975:
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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