V.U.B. Master in Human Ecology, Academic year 2003-2004 The Effects of Global Warming on the Hydrologic Cycle Thomas Deflo | Yuhua Bai | Ang Li | Katarina Tuharska 2 1. The water molecule In order to understand how the state of the hydrologic cycle will change as water molecules are affected by a rise in temperature, it is advised to fully fathom the unique behavior of the water molecule H2O. Water molecules are polar molecules: they have two oppositely charged atoms. Within each water molecule, hydrogen binds with oxygen atoms through regular electron sharing. As a result, two hydrogen atoms have their positively charged proton core partly exposed. The negatively charged electrons from the oxygen atoms bind to these free protons. This combination is a so-called hydrogen bond, allowing water to remain in the liquid, solid state at higher temperatures than any oth er liquid – up to 100°C. Hydrogen bonds (in brown) give water its unique liquidness. This doesn’t mean that water can not reach the gaseous state below its high boiling point. When solar radiation hits water on the Earth surface, some water attains the gaseous phase, because molecules near the surface have enough energy and freedom to overcome the relatively weak hydrogen bonds of their neighbors. As surface temperatures rise, the number of energetic molecules to jostle and escape the water’s surface tension will be greater, and evaporation will be more rapid. Evaporation is also greater with more surface area and air circulation, such as in oceans, because more space is available for the vapor to turn away from the liquid phase. The hydrogen bonds between water molecules give water a particularly large heat capacity, as they allow a relatively great vibration between molecules. As a result, much more latent heat is absorbed and released when water changes phase than with other liquids. Latent heat first occurs inside water vapor from the ocean to the atmosphere. When water vapor rises and cools, water molecules condensate into clouds. The amount of energy that is ultimately released far from the source of evaporation, when clouds rain, is exactly equal to the amount that was absorbed when the water vaporized. This latent heat capacity of water, thanks to hydrogen bonds, is very important in Earth's climate: liquid and gaseous water serves as a transporter of energy over the globe, influencing local temperatures. We can say that the hydrogen bonds inside water indirectly shape the Earth’s climate. Over one third of the Earth’s net radiation goes into the phase change of liquid into gaseous water. 3 2. The hydrologic cycle Water molecules can take on three molecular phases of ice, liquid water, and water vapor. The hydrologic cycle is the perpetual movement of water in all these phases on Earth. This dynamic water transport is driven by radiation, thermodynamic circulation, and gravity. All water now present on Earth has been recycled for billions of years, with virtually no new water created or lost since. Schematic representation of the hydrologic cycle. 2.1. Quantities of the hydrologic cycle Earth's total water volume is 1 360 000 000 km³ (one km³ contains 106 liters). Of this volume, the following storage can be distinguished (in km³): oceans glaciers, icecaps groundwater lakes and rivers water vapor 1320 x 106 25 x 106 13 x 106 250 x 103 13 x 103 Annually, the hydrologic cycle moves 496 x 103 km³ of water around the Earth. Evidently, the amount of water is in balance between the different components of the cycle: input and output are equal. This is essential for the cycle to remain harmoniously circular. For instance: if evaporation would not fully replenish the atmosphere, the latter would dry up in ten days. Or if precipitation from the atmosphere into the oceans would grind to a halt, the Earth’s sea level would lower by 1 meter per year. The mean residence time of water molecules is about 10 days in the form of atmospheric vapor, but about 3 000 years in liquid water. The atmosphere has a very short memory compared with the longer memory of the oceans. 4 The hydrologic cycle involves evaporation, transpiration, condensation, precipitation, and runoff of water. Let us follow through the quantitative fluxes of these components. We can say that the cycle starts with evaporation of water into the atmosphere from the main storage sinks on the planet’s surface: 85% of water vapor comes from the oceans (425 x 103 km³/y), 25% rises up from water bodies and transpiration by vegetation, a combination called evapotranspiration (71 x 103 km³/y). A very small portion of water evaporates through sublimation, when water changes from ice or snow into a gas. Most of the evaporated water rains back down into the seas (385 x 103 km³/y), while (40 x 103 km³/y) starts its travel through the atmosphere by horizontal air advection and joins the (71 x 103 km³/y) of evaporated water from inland water bodies. This water vapor (111 x 103 km³/y) then cools off as it rises in the atmosphere up to 50km, and because of this cooling, a phase change in the water molecule appears from gas into liquid – the reverse phase change from evaporation: water condensates into clouds. The condensed water droplets inside the clouds become more heavy, and then fall down to the surface by the effect of gravity. This precipitation can have different densities, dependent on the temperature inside the clouds: rain, partially frozen raindrops, snow, or hail. Of this precipitation, the majority (71 x 103 km³/y) infiltrates and percolates deep into the ground, to later return to the oceans via groundwater flow – slowly but eventually. The remaining (40 x 103 km³/y) of precipitation becomes land runoff, to be absorbed as land moisture and evapotranspirate again, or to be returned back to the inland and oceanic water bodies through rivers and streams. 2.2. Components of the hydrologic cycle As water covers 70% of the Earth, the hydrologic cycle constitutes the planet’s major biogeochemical system. Produced by the Sun, and together with features offered by lithosphere and atmosphere, water transport shapes and sustains the Earth’s biosphere. The transport of water irrigates surface vegetation, renews freshwater resources, sustains vital food chains, provides sanitation, heating and cooking, produces energy, cleans up bacteria, and transforms the land. Its influence on the global climate is both complex and sensible to change. Water determines life on our planet, and the water cycle provides it. 2.2.1. Oceans The hydrologic cycle is the main mechanism for the distribution of solar heat around the globe, fundamentally shaping the global climate. Solar radiation is first and foremost absorbed by the oceans, as oceanic heat capacity is much greater than that of land (because of the water molecules’ hydrogen bonds). This oceanic heat capacity is then to be transported, along ocean currents, to other latitudes around the globe. Ocean currents thus moderate the surface of the Earth's overall temperature. Heat budgets in seawater create fundamental variability in temperature conditions: due to the heat absorbing capacity, land closer to the sea will have seasonally fewer differences of +/-10°C, while temperatures far inland can fluctuate up to 60°C (e.g. in Siberia). Solar radiation and ocean currents are thus in a constant combine to shape surface temperatures. 5 Map of major ocean currents around the globe. These currents result from a transport of energy towards the poles in atmosphere and water. Warmer currents originating from the tropics are apparent. 2.2.2. Water vapor The next component in the hydrologic cycle occurs in the atmosphere. Evaporation requires absorption of heat from the surrounding air and stores it as latent heat. By doing so, the water cycle helps to cool off the surface of the Earth. This is of central importance to our study topic – how the permanently residing of water vapor in the air, before the condensation phase, is chiefly responsible for the natural greenhouse effect, rising earth surface temperatures to a habitable level. Water vapor is the main greenhouse gas, as it is highly absorptive to reflected infrared radiation. Distribution and absorption of heat in the atmosphere by water vapor is, in other words, another crucial biogeochemical aspect of the planet. 2.2.3. Precipitation Next after evaporation, condensation into liquid water occurs by cooling convection. The latent heat is released again by this condensation into the atmosphere, as the reverse physical process of evaporation. The heat then becomes sensible with precipitation: at an atmospheric saturation point in moisture levels (relative humidity 100%), rain falls out of the denser clouds with gravity. Rain is more likely to fall above mountainous regions. Consistent rainfall above maritime, or seasonally concentrated rainfall above continental coordinates exist, dependent on the distance the condensed water can travel before it rains down. The importance of this final phase change in the hydrologic cycle, in which the desalinated water becomes liquid again, can not be overstated. Life depends on it. It is also essential in keeping the hydrologic cycle intact, as the 40 x 103 km³/y of oceanic 6 water vapor that moved land-inward is returned through streams and rivers to its source, thus keeping ocean levels equalized. This does not mean that the amount of precipitation around the globe is equally distributed. Average annual precipitation for the world is estimated to be 2,9 mm per day, but large variations exist around the mean, mostly due to latitudinal differences in insolation levels. Tropical latitudes next to the equator receive most of the solar radiation. This has a direct effect on the amount of water movement upward into the atmosphere. Indeed, precipitation levels are the highest above these latitudes. The remaining dried up air then moves by advection and falls down above higher latitudes (30° N & S). These arid zones receive the least of precipitation. Other precipitation-poor regions are the polar areas, where cold air (because of low insolation levels) prevents longer stays of water vapor. Integration of mean observed precipitation levels from 25 years up to 1997 in mm per day [CMI 2003]. Tropical latitudes have the highest precipitation levels. Subtropical and polar regions have the lowest. Indeed, most of the world’s deserts occur at 30°N and 30°S. 2.2.4. Groundwater and surface runoff As indicated, most of the evaporation rains back into the oceans. Water that rains on the land as freshwater provides its vital drinking water to the biosphere. It has a series of destinations. River and lake beds can be replenished by rain. Rain can infiltrate into the soil and reside in different materials as soil moisture, to be taken up by vegetation and fauna, or to freeze (for at least two years) as permafrost. If it is drained deeper into the ground, while being filtered through the soil layers, some water can return as throughflow to the oceans or percolate deeper and become groundwater, to be contained in deep rocky aquifers, well up to the biosphere in natural springs, or be retrieved by artificial pumping. The horizontal movement of groundwater flow will find its way back to the oceans. Surface runoff occurs when infiltration can not keep up with precipitation, and water forms streams or rivers. This runoff flows back into bigger water bodies on land or towards the sea. This runoff balances the hydrologic cycle by replenishing the oceans with the exact amount of water that left land inwards as vapor. Excess of water over the river beds leads to flooding. This is a normal phenomenon, and fertilizing to the surrounding grounds, but exacerbated by anthropogenic land-use change such as 7 deforestation, river straightening, wetland transformation, and global warming. We now turn to the latter and then assess its influence on the described hydrologic cycle. 3. Global warming The relationship between temperature and the hydrologic cycle is the central subject of this study. As we have seen, the hydrologic cycle dominantly affects the temperature distribution of the globe, over ocean, atmosphere, and land. Simultaneously, temperature levels fundamentally influence the hydrologic cycle. Changes in the former are bound to engender changes in the latter – and vice versa. By investigating the condition of the current evolution in global temperature, we can deduce how the hydrologic cycle will respond to it, and in turn influence it. Of all insolation reaching the Earth, 51% is reflected or retained in the Earth’s atmosphere, before 49% is absorbed by the surface. Light hitting the surface gets partly retransmitted in the form of longer waves, or infrared radiation. Gases in the atmosphere with dense molecular structures capture this radiation and scatter it through the air and back to the surface. Infrared radiation that is trapped by these gases in the surfacetroposphere region (0-16km) warms up the Earth. This is the so-called ‘greenhouse’ effect, thanks to which the mean temperature is +14°C at the Earth’s surface instead of 19°C. Atmospheres of neighboring planets contain much more (Venus), or much less (Mars) greenhouse gases. Consequently, their surface temperatures are higher or lower. Greenhouse gases are water vapor (H2O), carbon dioxide (CO2), methane (CH4), and nitrous oxide (N2O). These gases are added to the natural state as byproducts of human activity. CO2 is responsible for 60% of the contribution to the anthropogenic greenhouse effect. The natural carbon cycle releases CO2 into the atmosphere by biosphere and oceanic sinks who then reabsorb it. This is a balanced cycle. Human activities add to this cycle by fossil fuel combustion and by reducing the cycle’s sink potential through land-use (mainly deforestation). The human burning of fossil fuels by industry, households and transport releases up to 6,3 gigatonsi of CO2 per year, while human land-use change prevents +/- 1,7 gigatons of CO2 uptake per year. This results in a net addition of up to 3,2 gigatons of CO2 in the atmosphere per year. As a result, atmospheric concentrations i Gigaton : billion metric tons. 8 of CO2 since the last two centuries have not likely been exceeded for 20 million years, and if present trends continue, their levels could quadruple by 2100. Changes in solar radiation, volcanic dust emission, terrestrial magnetism, climatic feedback mechanisms and rotational or orbital shifts, have been natural sources for temperature variability for the past millions of years [Goudie 1992 pp. 255 – 276], resulting in glacial and interglacial periods. But current warming trends are unusually rapid and self-reinforcing. Anthropogenic greenhouse gases will exacerbate the natural greenhouse effect by their radiative forcing, without any counteracting mechanism in place. The opposite is true: the greenhouse effect is expected to reinforce itself by positive feedback processes. The ‘radiative forcing’ of a gas is its influence on the balance of energy in the atmosphere, expressed in Watts per square meter (Wm-2), and a positive radiative forcing means that more energy remains in the atmosphere than is emitted. The radiative forcing by the anthropogenic greenhouse gases make the average temperature over the surface of the Earth climb. Global meteorological data are concordant with this: parallel with the increase in CO2, Earth’s mean surface temperature has increased by 0.6(±0.2)°C, likely to be the greatest temperature rise in 1000 years [IPCC 2001]. From their current level of 14°C, temperatures will very probably rise with 1.4°C to 5.8°C by 2100, due to increased positive radiative forcing. Variations of the Earth’s surface temperature since measurements begun (a), and over the last millennium from proxy data (b) [IPCC 2001]. The temperature increase in the 20th century is likely to be unprecedented for at least 1000 years. 9 4. Effects on the hydrologic cycle 4.1. Oceans 4.1.1. Sea level 120 000 years ago, just before last ice age, the mean global temperature was higher than today, and average sea level altitude was 5-6 meters higher. This was caused by the natural melting of Greenland and Antarctic ice sheets, over a long period of time. Current global warming trends are exceedingly faster. In one century, global average sea level rose between 0,1 and 0,2 m, and could increase up to 0,94 m by 2100. After that, many scenarios predict a continuing increase in sea levels. 4.1.1.1. Thermal expansion First of all, global warming induces the thermal expansion of surface waters. When surface water is heated, its molecules absorb thermal energy and express it as kinetic energy. As does any other material, it will expand because of this. There is widespread agreement that sea levels will rise as a result, but scientists are uncertain how the thermal expansion will be distributed over the oceans. As thermal expansion has a lower effect in cooler than in warmer water, sea level rise is expected to vary with geographical position, e.g. northern Europe is less prone to thermal expansion than southern Europe [Houghton 1998]. Because of the large heat capacity of water, sea level rise is projected to continue for hundreds of years, even after stabilisation of present greenhouse gas concentrations. 4.1.1.2. Melting a) Glaciers: The amount of water evaporating and precipitating over land is surmounted by runoff quantities from melting freshwater bodies. The hydrologic cycle is thus quantitatively disturbed, with more water put into the oceans. Sea levels rise because of this. Northerly continents have more to fear from melting of glaciers and ice sheets than from thermal expansion. Globally, glaciers are projected to lose about 25% of their mass by 2050. In the European Alps, about half of the original ice volume has already been lost since 1850, while almost all existing European glaciers could disappear over the next 100 years, with many of the smaller ones already disappearing within decades [Haeberli & Hoezle 1995]. Glacial ice in the Austrian Alps is more reduced today than any time during the past 5 000 years. Similar melting is visible in Spain, Russia and many other regions with glaciers: in Mt. Kenya's largest glacier has almost disappeared. Since 1912, 82% of Kilimanjaro’s ice has melted, with about one-third melting in just the last dozen years. At this rate, all of its ice will be gone in about 15 years. b) Ice sheets: Melting ice sheets will contribute even more to sea level rise. In the Arctic Ocean, satellite measurements indicate that ice cover has decreased by about 7% per decade since 1978. The potential for sea level rise from melting ice sheets is dramatic. 10 There are predictions that if Antarctic and Greenland ice sheets would melt in the next hundred years or more, it would change global sea levels up to 5 meters [Houghton 1998]. Indeed, the Larsen ice sheet of Antarctica is only one of the ice sheets that started to melt. West Antarctic ice sheets has been steadily melting since the end of the last ice age. Global warming will speed the process, and will continue to steer it for thousands of years after greenhouse gas concentrations will have been stabilised. 4.1.2. Thermohaline circulation The danger with global warming is that surpassing physical threshold levels could lead to the climate entering a new state. Global warming will also lead to nonlinear responses in the oceanic system. The oceanic body seems vulnerable to temperature triggers overarching a certain capacity. By 2100, a quadrupling of CO2 concentrations, with subsequent temperature climbing of 1,4°C to 5,8°C, could lead to the collapse of the thermohaline circulation. The Great Ocean Conveyor Belt is a large oceanic current, driven by differences in ocean density. It originates in the central Pacific, travels above the north coast of Australia, rounds the southern tip of Africa, to move into the North Atlantic. The current becomes the Gulf Stream by the time it passes the Gulf of new Mexico. The conveyor belt cools down as it releases heat above the European continent by evaporation and precipitation. As it loses water to evaporation from its surface layer, it becomes increasingly salty. Around the latitude of Iceland, the stream becomes so dense that it sinks and flows back, along the ocean floor, rounding South-Africa and Australia, into the Pacific, where it is warmed and pushed back up to the surface to restart. Global circulation pattern of the Great Ocean Conveyor Belt, with warmer waters on the surface, and cold waters deeper down. Due to global warming, Arctic sea ice is bound to melt, and precipitation above the northern oceans is bound to increase. This adding of freshwater into the oceans will interfere with the conveyor belt, as it slows down in the North-Atlantic. The system depends on high salt concentrations near the water surface. Melting the ice dilutes the salt 11 and weakens the pumping effect of the stream. By further diminishing the density of the North Atlantic water, the Gulf Stream could be halted. Most global climate models show how this could lead to the cooling of the European climate, with temperatures dropping by 5°-10°C, leading to a Little Ice Age, as in the 15th century. General Circulation Model reflecting changes in surface air temperature, caused by a modelled halt in deep, saline water formation in the North Atlantic [Rahmstorf 2002]. Furthermore, the Great Conveyor Belt could be altered more widely. As more tropical water vapor moves towards the north pole and precipitates above the northern hemisphere, the input of fresh water into the North Atlantic ocean could increase up to a point where the thermohaline ocean belt would be lacking so much saline, heavy water, that it would be cut through, prevented to return southwards, and collapse altogether [Marotzke 2000]. This would definitely further change the regional patterns of temperature, evaporation and precipitation. These changes could lead to a completely different climate in many parts of the world. 4.1.3. Ocean-atmosphere interactions Meteorological oscillations between ocean and atmosphere are bound to be influenced by global warming. One such interaction between water and air is the inter-annual occurrence of El Niño. This climate phenomenon is a shift in air pressure above the Pacific ocean: high pressure develops above the southern Pacific and low pressure above the central Pacific. This alters trade wind patterns and dependent ocean currents. Heat that is normally blown westward is concentrated at Eastern and central Pacific parts of the ocean. Of the 29 El Niños that have occurred since 1700, the 1982-83 El Niño was the strongest. It caused droughts in Africa, Australia, India, Indonesia, and the Philippines, flooding in Peru and Ecuador, and devastating storms in California. 12 Normal situation (above) and El Niño phenomenon (below) over the Pacific Ocean [SOEST 2004]. Trade winds heading west collapse or even reverse. The warm water of the western Pacific flows back eastward, and sea surface temperatures increase significantly off the western coast of South America. The steep rise in temperature the past century has probably lead to an exacerbation of the El Niño phenomenon, whose behavior is stronger and more frequent from 1976 than since the last 100 years. The year 1997 gave another record El Niño event, when global temperature records were broken for sixteen consecutive months. Unusual floods, strong cyclones and droughts are the result. The circulation of heat away from the tropics is a natural phenomenon, regularly concentrated in the El Niño event. But as global warming pushes more and faster evaporation upwards from the tropics, with its accompanying latent heat, more ‘fuel’ would be delivered for El Niño to develop. Even if global warming would have little influence on the El Niño amplitude, it is likely to worsen the meteorological phenomena that occur when El Niño appears (more heavy rainfall, and risk of severe droughts and floods). 4.2. Water vapor Although measurement problems hinder the analysis of long-term water vapor changes, recent studies confirm that evaporation increases. Knowledge about changes in water vapor at upper tropospheric and lower stratospheric levels is of great importance because positive radiative forcing can result from them. As sunlight evaporates water, heat is released from the water in the form of infrared radiation. A small part of this radiation escapes into space, but most of it remains trapped inside the water vapor and radiates back to the surface of the Earth. This effect is chiefly 13 responsible for the natural greenhouse effect. Indeed, water vapor is the most important greenhouse gas. Absorptivity of infrared electromagnetic radiation by H2O. Water molecules absorb much of the radiation between wavelengths of 0,7 to 20> µm. As surface temperatures increase with global warming, more evaporation of water will occur over the oceans. More evaporation is related to increasing temperatures. Hence, the amount of water vapor in the atmosphere will increase. By its greenhouse potential, additional water vapor will further exacerbate global warming effects. Evaporation will lead to more evaporation; the process intensifies itself. Water evapora tion Radia tive forcing Surface warming Clockwise scheme of the positive feedback effect on water vapor by global warming. Warmer air can also hold more vapor: the amount of water needed to saturate air humidity increases exponentially with temperature. Global warming will thus allow higher humidity levels in the atmosphere. This has been shown to stimulate evapotranspiration. 4.3. Clouds Between evaporation and precipitation, water molecules first condensate into clouds. Cloud formation has an important influence on the radiative balance of the Earth, 14 particularly in the atmosphere: by keeping solar radiation from reaching the surface, clouds keep the Earth at a cooler temperature. Simultaneously though, clouds prevent reflected solar radiation from escaping into space and have a warming effect. Overall, the cooling effect is estimated to be dominant: clouds reflect about 50 Watt/m2 of incoming solar radiation back to space (half the planet’s albedo), while their absorption of heat keeps 20 Watt/m2 in the atmosphere. This is another crucial climatologic feature of the hydrologic cycle, and varies with cloud typology. The formation of clouds is part of a negative feedback system. It is likely that there has been a 2% increase in cloud cover over mid- to high latitude land areas during the 20th century. This translates well into an observed decrease in daily temperatures. The extra formation of clouds by global warming can be assumed to have a net cooling effect on the Earth’s climate. The process of global warming thus reduces its own origin. But as we said, cloud typology determines their radiative effect. Global warming can also drag cloud formation into a positive feedback system. As temperatures rise, an increase in high clouds will result, which are efficient at reflecting long-wave radiation back to the Earth’s surface, while letting short-wave radiation through. This will lead to further warming of the atmosphere. 4.4. Precipitation [IPCC]states that ‘the influence of warmer temperatures and increased water vapor in the atmosphere are not independent events, and are likely to be jointly related to increases in heavy and extreme precipitation events’. Overall, global warming will lead to an increase in global precipitation levels – about +2% since the beginning of the 20th century – as more water vapor will be available to condensate and deliver water in liquid form, back to the surface, as rain and snow. However, this increase is unevenly distributed across the climatologic areas of the planet, and over time, as well as varying with altitude. Topographical factors such as mountains and soil types locally shape hydrologic cycles. Some areas will receive more, others less rainfall. What is certain, is that global warming will reshape the distribution of precipitation patterns, likely to become much more variable, with more deviations from the mean levels. As a result, a less steady input of water into the ground is apparent over many areas, leading to reduced flow regimes. For the northern hemisphere, [IPCC 2001] considers it very likely that global warming has increased precipitation with 10% since the turn of the century, with a growing 2 to 4% of extreme rainfall. In 1998, the northern hemisphere (55°N and higher) had their wettest year on record. Over the tropics, more extreme precipitation patterns are observed in the past century. The Asian southwest monsoon, for instance – one of the most important climate systems in the world – is more extreme. This is because it is generated by the heat capacity contrast between land and sea, and global warming extrapolates this contrast, as the heat capacity of water is greater than that of land. 15 But rainfall has decreased over the sub-tropics (10°N to 30°N) by about 0.3% per decade, leading to more droughts and desertification, especially in summer. This is explained by an exacerbation of the Hadley cell; the main atmospheric current of warm, humid air rising above the tropics and drying up before reaching subtropic latitudes. This will worsen by the overshadowing of precipitation levels by evapotranspiration levels in arid areas. Global annual precipitation trends during the previous century [IPCC 2001]. It is noteworthy that at the stage of desertification, a positive feedback system sneaks in: desertification means a decrease in vegetation, which provides the atmosphere with less evapotranspiration, hence less precipitation, which further worsens local droughts. Deforestation in the Amazon, for instance, shows this evolution towards lower precipitation levels because of dryer land cover [Pagano & Soroosh 2002] and less available moisture. Once an area has been made into a desert, it is not likely to change without external aid, on the contrary: it is more likely to dry up further. 4.5. Groundwater Groundwater in arid lands is considered to be a stable water source, if its drainage or evaporation rate doesn’t exceed its natural recharge rate. The combined effect of higher evaporation and less precipitation from global warming on the land surface, means that more water leaves the basins than is replenished by rain and runoff. At the same time, social drainage continues, which can make the systematic input of water into the water body crash. Recharge of aquifers, which occurs primarily through seepage of water from streams, is exceeded by evaporation, because of recurrent heat waves. Similarly, soil moisture and streamflow are more rapidly depleted. Water bodies in centrally located, continental areas are very vulnerable to this imbalance: with a 1° to 2°C increase in annual surface temperature, with increased evaporation, and with a 10% precipitation reduction, a 1,5 to 2-fold decrease in water resources is 16 envisaged. Indeed, many great lakes across the world manifest a decrease in net basin levels, and continents such as North-America have suffered from the most severe droughts in a 100 years. 4.6. Surface runoff As a consequence of global warming, extreme weather events like floods and droughts are projected to increase, in all parts of the world. Regions that did not suffer from these events will likely be affected. Regions already suffering from these events will not be spared from more extremities. Floods and droughts are the result of the hydrologic cycle becoming less regular and quantitatively more unevenly distributed. Continents were recently affected with both unusual droughts as well as unusual floods. 4.6.1. Floods Global streamflow trends are directly proportional to global precipitation trends. Global warming has led to increased precipitation at higher latitudes, especially in winter periods. In these regions, river beds are liable to overflow. Small increases of water to already saturated soils can cause large increases in runoff, resulting in floods. Many low latitude rivers reach their maximum during raining periods over equatorial rain forests. This makes them vulnerable to floods. Even with existing dams and reservoirs, the increasing frequency in heavy rains could not be handled by them. Per year, 20 billion tons of soil and rock are eroded to be exported to the oceans [Deléage 2001]. As floods worsen, more land would be eroded, which would in turn reduce the river beds, allowing more flooding – one of the many positive feedback mechanisms induced by global warming. River deltas and their surrounding land are under menace of permanent overflow. As an example, 20% of the Nile river delta is under threat of being flooded [Titus 1989]. A projected increase in extreme rainfall events during winter and spring, when soils are saturated, could increase the frequency and severity in floods. An increase in large-scale precipitation might also lead to increased flood risks of large river basins. 4.6.2. Droughts The developing global warming scenario shows a radical decrease in rainfall in several other parts of the world, especially in the summer periods. Warmer global temperatures will cause an intensification of evaporation and melting over land, leading to greater drying of soils and vegetation. Although the projections for rainfall vary considerably by region, droughts are expected to be longer-lasting and more severe because of higher temperatures and increased evaporation. 17 In arid, continental regions, river runoff will be profoundly reduced by global warming. With a 1° to 2° C increase in annual air temperature and a 10% precipitation reduction, a 40 to 70% reduction of annual river runoff can be expected in these regions. Snow and ice contribute fundamentally to major rivers. We have seen that changes in the cryosphere, with warmer temperatures and melting of glaciers, is happening fast. Over a short time, major rivers like the Rhine could decline in flow by 10% during the summer, as less snow is replenished. The Nile, which is very dependent on mountain snow from Ethiopia, could also be altered drastically in its flow regime. Seasonal rivers are unlikely to see their input of water maintained, with lowering patterns of precipitation and even more extensive usage of their waters, as droughts occur elsewhere. 5. Conclusion Understanding of hydrologic processes and their incorporation in temperature models have improved over the years. However, because of the nonlinear nature of the global warming effects, precise biogeochemical dynamics are difficult to predict. What is undisputed, is that the hydrologic cycle will be both quantitatively as well as qualitatively affected, undiscriminating over all continents. In time, global warming could give the planet a new hydrologic distribution. Presently, the clearest changes will result in more extreme events. While considerable caution exists to give an exhaustive picture of all components of the hydrologic cycle under global warming conditions, certain trends are already visible. Overall, the intensity of the cycle is strengthening, but its regularity is weakening. A patchwork of hydrologic anomalies at several stages exist, dependent on latitude and local climate conditions. General conclusions are hard to shape, but we can safely conclude that sea level, evaporation, precipitation and runoff have increased in most parts of the world, but that this has not happened in a regular fashion, effectively leading to more drinking water shortages and reduced flow regimes. Anthropogenic radiative forcing is most worrying by its positive feedback processes. By concentrating on temperature effects on the hydrologic cycle, we have discovered clear examples of this. Temperature and water systems are engaged in a positively correlated relationship, of which the long-term result is uncertain but potentially very destabilizing for the Earth’s climatic baseline conditions. Think of the possible shutdown of the thermohaline circulation of the world’s oceans. As for hydrology, most water management planning is made more fragile due to the introduction of more extremities from global warming in the hydrologic cycle. Unusually wet or dry events will affect reliability of models to estimate water fluxes. Predicted magnitudes cannot take future extreme events into account when assessing risk scenarios. The instability of the hydrologic cycle will make hydrographic practice more difficult. 18 References CMI (Climate Modeling Initiative). 10/2003. http://web.mit.edu/cgcs/www/cmi.html (04/2004). Deléage, Jean-Paul. 2001. La Biosphère, Notre Terre Vivante. Luçon: Gallimard. Goudie, Andrew. 1992. Environmental Change. New York: Oxford University Press. Haeberli, W. & M. Hoezle, 1995. Application of inventory data for estimating characteristics of regional climate change effects on mountain glaciers: a pilot study with the European Alps. Annals of Glaciology 21. Houghton, J. 1998. Global warming. Praha: Academia. IPCC (Intergovernmental Panel on Climate Change). 2001. Climate Change 2001: Synthesis Report. http://www.grida.no/climate/ipcc_tar/vol4/english/ (03/2004). LSBU (London South Bank University), The Phase Diagram of Water, http://www.lsbu.ac.uk/water/phase.html (04/2004). Mannion, A.M. 1997. Global Environmental Change. New York: Longman. Marotzke, Jochem. 2000. Abrupt climate change and thermohaline circulation: Mechanisms and predictability. PNAS (Proceedings of the National Academy of Sciences) 97: 1347–1350. Myles, R. Allen & William J. Ingram. 2002. Constraints on future changes in climate and the hydrologic cycle. Nature 419: 224-233. NASA (National Aeronautics & Space Administration). A Chilling Possibility. 3/2004. http://science.nasa.gov/headlines/y2004/05mar_arctic.htm Pagano, Thomas & Soroosh Sorooshian. 2002. Hydrologic Cycle. In Encyclopedia of Global Environmental Change, edited by Dr. Michael C. Mac Cracken & Dr. John S. Perry. Chichester: John Wiley & Sons, Ltd. PO.DAAC (Physical Oceanography Distributed Active Archive Center). 11/2003. http://podaac.jpl.nasa.gov/cgi-bin/dcatalog/fam_summary.pl?sst+mcsst (04/2004). Rahmstorf Stefan. 2002. Ocean circulation and climate during the past 120,000 years. Nature 419: 207-214. Titus, James G. 1989. The Cause and Effects of Sea Level Rise, The Challenge of Global Warming. Washington: Inland Press.