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Table 3.10.1: Changes in Near-storm rainfall <strong>and</strong> wind intensity associated with Tropical storms in under global<br />
warming scenarios<br />
Reference GHG<br />
scenario<br />
Knutson et al.<br />
(2008)<br />
Knutson <strong>and</strong> Tuleya<br />
(2004)<br />
Type of Model Domain Change in nearstorm<br />
intensity<br />
rainfall<br />
A1B Regional Climate Model Atlantic (+37, 23, 10)%<br />
when averaged<br />
within 50, 100<br />
<strong>and</strong> 400 km of<br />
the storm centre<br />
1% per<br />
year CO 2<br />
increase<br />
9 GCMs + nested regional<br />
model with 4 different<br />
moist convection<br />
schemes.<br />
Oouchi et al. (2006) A1B High Resolution GCM Global<br />
3.11. Sea Level Rise<br />
30<br />
Change in peak<br />
wind intensity<br />
+2.9%<br />
Global +12-33% +5-7%<br />
N/A +14%<br />
North Atlantic +20%<br />
Observed records of sea level from tidal gauges <strong>and</strong> satellite altimeter readings indicate a global mean SLR<br />
of 1.8 (+/- 0.5) mm yr -1 over the period 1961-2003 (Bindoff et al., 2007). Acceleration in this rate of<br />
increase over the course of the 20 th Century has been detected in most regions (Woodworth et al., 2009;<br />
Church <strong>and</strong> White, 2006).<br />
There are large regional variations superimposed on the mean global SLR rate. Observations from tidal<br />
gauges surrounding the Caribbean basin (Table 3.11.1) indicate that SLR in the Caribbean is broadly<br />
consistent with the global trend (Table 3.11.2).<br />
Table 3.11.1: Sea level rise rates at observation stations surrounding the Caribbean Basin<br />
Tidal Gauge Station Observed trend (mm yr -1 ) Observation period<br />
Bermuda 2.04 (+/- 0.47) 1932-2006<br />
San Juan, Puerto Rico 1.65 (+/- 0.52) 1962-2006<br />
Guantanamo Bay, Cuba 1.64 (+/- 0.80) 1973-1971<br />
Miami Beach, Florida 2.39 (+/1 0.43) 1931-1981<br />
Vaca Key, Florida 2.78 (+/- 0.60) 1971-2006<br />
(Source: NOAA, 2009)<br />
Projections of future SLR associated with climate change have recently become a topic of heated debate in<br />
scientific research. The IPCC’s AR4 report summarised a range of SLR projections under each of its st<strong>and</strong>ard<br />
scenarios, for which the combined range spans 0.18-0.59 m by 2100 relative to 1980-1999 levels (see<br />
ranges for each scenario in Table 3.11.2). These estimates have since been challenged for being too<br />
conservative <strong>and</strong> a number of studies (e.g. Rahmstorf, 2007; Rignot <strong>and</strong> Kanargaratnam, 2006; Horton et<br />
al., 2008) have provided evidence to suggest that their uncertainty range should include a much larger<br />
upper limit.<br />
Total sea level rises associated with atmospheric warming appear largely through the combined effects of<br />
two main mechanisms: (a) thermal expansion (the physical response of the water mass of the oceans to<br />
atmospheric warming) <strong>and</strong> (b) ice-sheet, ice-cap <strong>and</strong> glacier melt. Whilst the rate of thermal expansion of<br />
the oceans in response to a given rate of temperature increase is projected relatively consistently between<br />
GCMs, the rate of ice melt is much more difficult to predict due to our incomplete underst<strong>and</strong>ing of icesheet<br />
dynamics. The IPCC total SLR projections comprise of 70-75% (Meehl et al., 2007a) contribution from