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Royal Society - David Keith

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These model experiments (also discussed above) are<br />

designed such that the reduction in absorbed solar<br />

radiation exactly balances the radiative forcing due to<br />

the increased concentration of greenhouse gases. The<br />

resulting climate is compared with that of a world of preindustrial<br />

CO 2 concentrations and no reduction in sunlight.<br />

It is found that the temperature of the air near the surface<br />

is substantially less affected in the geoengineered world<br />

than in the non-geoengineered case but, nevertheless, is<br />

slightly cooler in tropical regions, where the solar effect<br />

dominates, and warmer at high latitudes, where the<br />

greenhouse trapping is greater. The weaker latitudinal<br />

temperature gradient affects other climate parameters.<br />

For example the amplitude of the seasonal cycle is<br />

reduced, giving warmer winters and cooler summers.<br />

The cooler tropics result in less evaporation and a generally<br />

drier atmosphere with less precipitation. One model study<br />

(Lunt et al. 2008), which included fully coupled ocean<br />

circulations, also shows a decreased intensity of El Niño<br />

events, with concomitant impacts on tropical climate, in<br />

particular tending to enhance overall precipitation over<br />

south-east Asia and India.<br />

Even though the global radiation balance is the same for<br />

both, the pre-industrial and geoengineered simulations<br />

show significant regional and temporal differences.<br />

Nevertheless, these differences are small compared to<br />

those associated with a non-geoengineered future.<br />

There are numerous and considerable uncertainties<br />

involved in most aspects of the proposed space-based<br />

SRM methods and all these would need to be addressed<br />

by detailed research before any method might be deemed<br />

potentially fit for purpose. Apart from the development<br />

of necessary technology, and the solution of problems<br />

concerning its implementation and maintenance in space,<br />

the research would need to investigate carefully the<br />

potential impacts on the climate system. All the spacebased<br />

SRM methods propose to reduce the total amount<br />

of solar energy entering the atmosphere but each affects<br />

the incoming solar beam differently. Reflectors at the L1<br />

point would essentially have the effect of reducing the<br />

solar constant and initial studies of the impact of this,<br />

within in a high CO 2 atmosphere, have already been carried<br />

out, as outlined above. More detailed assessments would<br />

investigate the impact on regional meteorology,<br />

temperature and precipitation patterns, including any<br />

changes in seasonality and variability, and also impacts<br />

on polar ice cover and ocean circulations. Reflectors in low<br />

Earth orbit would redistribute solar radiation in far more<br />

complex ways which would each need to be carefully<br />

determined, even before any model assessment could be<br />

made of their climate impact. While such studies would be<br />

able to give some indication of the potential impacts of the<br />

space-based SRM methods all would be subject to the<br />

caveats expressed in Box 1.2 concerning the limitations<br />

of climate models.<br />

All of the space-based techniques summarised in this<br />

section (see Table 3.5) contain such great uncertainties<br />

in costs, effectiveness (including risks) and timescales<br />

of implementation that they are not realistic potential<br />

contributors to short-term, temporary measures for<br />

avoiding dangerous climate change. This is not to dismiss<br />

them from future consideration, however. If, in the future<br />

it became probable that some form of geoengineering<br />

would be needed for a period approaching a century or<br />

longer, on such a timescale (and with the continual<br />

advance of technical capabilities) it is quite possible that<br />

the best examples of this type may offer a cheaper and<br />

less risky approach to SRM than any of the stratospheric<br />

or near-Earth techniques. With launch costs to near-Earth<br />

orbit approaching a few $ M per tonne (http://www.<br />

thespacereview.com/article/233/1), it may eventually be<br />

possible to place a one Megatonne system into high orbit<br />

at a price of a few $ trillion, of the same order as that for<br />

some of the other proposals considered, and potentially<br />

with a much longer lifetime. Some designs proposed for<br />

the L1-based systems have masses considerably lower<br />

than a Megaton, so even at current launch costs; the cost<br />

of launch could conceivably be smaller than the cost of<br />

other SRM techniques (<strong>Keith</strong> 2000). However at these<br />

rates, the costs of placing billions of tonnes of material<br />

(eg dust) into orbit would be prohibitive. Desk-based<br />

engineering design studies could advance understanding<br />

of the likely feasibility and costs of such proposals<br />

Table 3.5. Summary evaluation table for space-based methods<br />

Space-based methods<br />

Effectiveness<br />

Affordability<br />

Timeliness<br />

Safety<br />

No inherent limit to effect on global temperatures<br />

SRM method so does nothing to counter ocean acidification<br />

High cost of initial deployment (depends on mass required): plus additional<br />

operational costs (eg maintaining positions): but long lifetime once deployed<br />

Would take several decades (at least) to put reflectors into space<br />

Once in place, reflectors would reduce global temperatures within a few years<br />

Residual regional climate effects, particularly on hydrological cycle<br />

No known direct biochemical effects on environment beyond possible effects of<br />

reduced insolation<br />

High<br />

Very low<br />

to Low<br />

Very low<br />

Medium<br />

The <strong>Royal</strong> <strong>Society</strong><br />

Geoengineering the Climate I September 2009 I 33

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