Professor Richard Gragg teaches graduate and undergraduate courses in environmental toxicology and human health, environmental toxicology, environmental justice, and environmental ethics. Dr. Gragg is also the Director of the Center for Environmental Equity and Justice for the State of Florida. His research interests include: [a] ecosystem and human health impacts of light absorption by environmental contaminants; [b] environmental justice and policy; and [c] environmental health disparities. Dr. Gragg currently serves as a member of the Florida Environmental Regulatory Commission, the Board of Directors for Audubon of Florida and is Co-Chair of the Communications and Outreach Subcommittee, and the Florida Brownfields Association and is Co-Chair of the Environmental Justice and Public Health Subcommittee. Dr. Gragg is a former member of the Environmental Protection Agency’s National Environmental Justice Advisory Council and its Health and Research Subcommittee.
Gragg has a B.S. in Biochemistry from SUNY Binghamton University, a M.S. in Pharmacology from Florida A&M University, and a Ph.D. in Pharmaceutical Sciences/Toxicology from Florida A&M University.
E-mail: Richard Gragg
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Originally Published As:
Title: On the Existence of an Equivalent Relation between Heat and the ordinary Forms of Mechanical Power
Author: James Prescott Joule
Source: Philosophical Magazine, series 3, vol. xxvii, p. 205
Year published: 1845
EDITOR'S NOTE: In a classic experiment in 1843, James Joule showed the energy equivalence of heating and doing work by using the change in potential energy of falling masses to stir an insulated container of water with paddles. Joule reported this and other related work in a letter to th editors of the Philosophical Magazine. Although German physicist Julius Robert von Mayer had made the same discovery independently of Joule a few years earlier, it was Joule who received the credit. Joule made a series of measurements and found that, on average, a weight of 772 pounds falling through a distance of one foot would raise the temperature of one pound of water by 1° F. This corresponds to 772 ft lbs × 1.356 J/ft lb = 59,453.6 Calories or 1 cal = 4.15 Joules; this is in close agreement with the current accepted value of 1 cal = 4.184 J. These findings contradicted the "caloric theory,” which embodied the day's widespread belief that heat was a fluid that could be neither created nor destroyed. Joule, on the other hand, claimed that heat was only one of many forms of energy and only the sum of all forms was conserved. This formed the basis for the theory of conservation of energy (the First Law of Thermodynamics).
Gentlemen,
The principal part of this letter was brought under the notice of the British association at its last meeting at Cambridge. I have hitherto hesitated to give it further publication, not because I was in any degree doubtful of the conclusions at which I had arrived, but because I intended to make a slight alteration in the apparatus calculated to give still greater precision to the experiments. Being unable, however, just at present to spare time necessary to fulfil this design, and being at the same time most anxious to convince the scientific world of the truth of the positions I have maintained, I hope you will do me the favour of publishing this letter in your excellent Magazine.
The apparatus exhibited before the Association consisted of a brass paddle-wheel working horizontally in a can of water. Motion could be communicated to this paddle by means of weights, pulleys, &c., exactly in the matter described in a previous paper.*
The paddle moved with great resistance in the can of water, so that the weights (each of four pounds) descended at the slow rate of about one foot per second. The height of the pulleys from the ground was twelve yards, and consequently, when the weights had descended through that distance, they had to be wound up again in order to renew the motion of the paddle. After this operation had been repeated sixteen times, the increase of the temperature of the water was ascertained by means of a very sensible and accurate thermometer.
A series of nine experiments was performed in the above manner, and nine experiments were made in order to eliminate the cooling or heating effects of the atmosphere. After reducing the result to the capacity for heat of a pound of water, it appeared that for each degree of heat evolved by the friction of water a mechanical power equal to that which can raise a weight of 890 lb. to the height of one foot had been expended.
The equivalents I have already obtained are; -- 1st, 823 lb., derived from magneto-electrical experiments (Phil. Mag. ser. 3 vol. xxiii. pp. 263, 347); 2nd, 795 lb., deduced from the cold produced by the rarefaction of air (Ibid. May 1845, p. 369); and 3rd, 774 lb. from experiments (hitherto unpublished) on the motion of water through narrow tubes. This last class of experiments being similar to that with the paddle wheel, we may take the mean of 774 and 890, or 832 lb., as the equivalent derived from the friction of water. In such delicate experiments, where one hardly ever collects more than one another than that above exhibited could hardly have been expected. I may therefore conclude that the existence of an equivalent relation between heat and the ordinary forms of mechanical power is proved; and assume 817 lb., the mean of the results of three distinct classes of experiments, as the equivalent, until more accurate experiments shall have been made.
Any of your readers who are so fortunate as to reside amid the romantic scenery of Wales or Scotland could, I doubt not, confirm my experiments by trying the temperature of the water at the top and at the bottom of a cascade. If my views be correct, a fall of 817 feet will course generate one degree of heat, and the temperature of the river Niagra will be raised about one fifth of a degree by its fall of 160 feet.
Admitting the correctness of the equivalent I have named, it is obvious that the vis viva of the particles of a pound water at (say) 51° is equal to the vis viva possessed by a pound of water at 50° plus the vis viva which would be acquired by a weight of 817 lb. after falling through the perpendicular height of one foot.
Assuming that the expansion of elastic fluids on the removal of pressure is owing to the centrifugal force of revolving atmospheres of electricity, we can easily estimate the absolute quantity of heat in matter. For in an elastic fluid the pressure will be proportional to the square of the velocity of the revolving atmosphere, and the vis viva of the atmospheres will also be proportional to the square of their velocity; consequently the pressure of elastic fluids at the temperatures 32° and 33° is 480 : 481; consequently the zero of temperature must be 480° below the freezing-point of water.
We see then what an enormous quantity of vis viva exists in matter. A single pound of water at 60° must possess 480° + 28° = 508° of heat; in other words, it must possess a vis viva equal to that acquired bt a weight of 415036 lb. after falling through the perpendicular height of one foot. The velocity with which the atmosphere of electricity must revolve in order to present this enormous amount of vis viva must of course be prodigious, and equal probably to the velocity of light in the planetary space, or to that of an electric discharge as determined by the experiments of Wheatstone.
* Phil. Mag. ser. 3, vol. xxiii, p. 436. The paddle-wheel used by Rennie in his experiments on the friction of water (Phil. Trans. 1831, plate xi, fig, 1) was somewhat similar to mine. I have employed, however, a greater number of "floats," and also a corresponding number of stationary floats, in order to prevent the rotatory motion of the can.
I remain, Gentlemen,
Yours Respectfully,
James P Joule.
Permafrost is soil, rock, sediment, or other earth material with a temperature that has remained below 0°C for two or more consecutive years. Permafrost underlies most of the surfaces in the terrestrial Arctic. Permafrost extends as far south as Mongolia[11], and is present in alpine areas at even lower latitudes. Figure 6.21 shows the distribution of permafrost in the Northern Hemisphere, classified into continuous, discontinuous, and sporadic zones. In the continuous zones, permafrost occupies the entire area (except below large rivers and lakes). In the discontinuous and sporadic zones, the percentage of the surface underlain by permafrost ranges from 10 to 90%. Discontinuous permafrost underlies a larger percentage of the landscape than does sporadic permafrost, although there is not a standard definition of the boundary between the two zones (Fig. 6.21 uses 30% coverage as the boundary). In the Northern Hemisphere, permafrost zones occupy approximately 26 million square-kilomters (km2) or about 23% of the exposed land area, but permafrost actually underlies 13 to 18% of the exposed land area[12]. Distinctions are made between permafrost that is very cold (temperatures of -10°C and lower) and thick (500–1400 meters [m]), and permafrost that is warm (within 1 or 2°C of the melting point) and thin (several meters or less). Ground ice (0–20 m depth) in permafrost exhibits large spatial variability, with generally much more ice in lowland permafrost than in mountain permafrost[13].
The role of permafrost in the climate system is threefold[14]. First, because it provides a temperature archive, permafrost is a "geoindicator" of environmental change. At depths below 15 to 20 m, there is generally little or no annual cycle of temperature, so seasonality does not influence warming or cooling. Second, permafrost serves as a vehicle for transferring atmospheric temperature changes to the hydrological and biological components of the earth system. For example, the presence of permafrost significantly alters surface and subsurface water fluxes, as well as vegetative functions. Third, changes in permafrost can feed back to climate change through the release of trace gases such as CO2 and methane (CH4), linking climate change in the Arctic to global climate change[15].
The active layer is the seasonally thawed layer overlying permafrost. Most biogeochemical and hydrological processes in permafrost are confined to the active layer, which varies from several tens of centimeters to one to two meters in depth. The rate and depth of active-layer thaw are dependent on heat transfer through layers of snow, vegetation, and organic soil. Snow and vegetation (with the underlying organic layer) have low thermal conductivity and attenuate annual variations in air temperature.
During summer, the thermal conductivity of the organic layer and vegetation is typically much smaller than in winter. This leads to lower heat fluxes in summer and ultimately keeps permafrost temperatures lower than they would be in the absence of vegetation and the organic layer. The latent heat associated with evapotranspiration and with melting and freezing of water further complicates the thermodynamics of the active layer. Over longer timescales, the thawing of deep permafrost layers can lag considerably (decades or centuries) behind a warming of the surface because of the large latent heat of fusion of ice[16]. Moreover, thermal conductivity is typically 20 to 35% lower in thawed mineral soils than in frozen mineral soils. Consequently, the mean annual temperature below the level of seasonal thawing can be 0.5 to 1.5°C lower than on the ground surface.
Thawing of permafrost can lead to subsidence of the ground surface as masses of ground ice melt, and to the formation of uneven topography known as hermokarst. The development of thermokarst in some areas of warm and discontinuous permafrost in Alaska has transformed some upland forests into wetlands[17]. Recent thaw subsidence has also been reported in areas of Siberia[18] and Canada[19]. Climate-induced thermokarst and thaw subsidence may have detrimental impacts on infrastructure built upon permafrost[20], as section 16.3 discusses in more detail. Permafrost degradation can also pose a serious threat to arctic biota through either oversaturation or drying[21]. The abundance of ground ice is a key factor in subsidence, such that areas with little ice (e.g., the Canadian Shield or Greenland bedrock masses) will suffer fewer subsidence effects when permafrost degrades.
Seasonal soil freezing and thawing are the driving forces for many surficial processes that occur in areas with permafrost or seasonally frozen soils. Cryoturbation, a collective term for local vertical and lateral movements of the soil due to frost action, is one of these potentially important cryogenic processes (see Washburn[22] for a review). Cryoturbation typically occurs in the permafrost zone, but also occurs in soils that freeze only seasonally. Cryoturbation can cause the downward displacement of organic material from the near-surface organic horizons to the top of the permafrost table, resulting in sequestration of organic carbon in the upper permafrost layer[23]. During the past several thousand years, a significant amount of organic carbon has accumulated in permafrost due to this process.
Because surface temperatures are increasing over most permafrost areas (section 2.6.2), permafrost is receiving increased attention within the context of past and present climate variability. Measurements of ground temperature in Canada, Alaska, and Russia have produced a generally consistent picture of permafrost warming over the past several decades. Lachenbruch and Marshall[24] were among the first to document systematic warming by using measurements from permafrost boreholes in northern Alaska to show that the surface temperature increased by 2 to 4°C between the beginning of the 20th century and the mid-1980s. Measurements conducted by Clow and Urban[25] in the same Alaska borehole network indicated further warming of about 3°C since the late 1980s. Figure 6.22 confirms this warming with results from a site-specific permafrost model driven by observed air temperatures and snow depths for the period 1930 to 2003, calibrated using measurements of permafrost temperatures between 1995 and 2000. While warming has predominated since 1950, considerable interannual variability is also apparent.
Data from northwestern Canada, indicating that temperatures in the upper 30 m of permafrost have increased by up to 2°C over the past 20 years[26], provide further evidence of warming. Although cooling of permafrost in the Ungava Peninsula of eastern Canada in recent decades has been widely cited as an exception to the dominant warming trend, Brown J. et al.[27] and Allard et al.[28] indicated that shallow permafrost temperatures in the region have increased by up to nearly 2°C since the mid-1990s. Smith et al.[29] reported warming in the upper 30 m of permafrost in the Canadian High Arctic since the mid-1990s. Smaller temperature increases, averaging 1°C or less, have been reported in northwestern Siberia[30]. Measurements from a network of recently drilled boreholes in mountainous areas of Europe indicate warming of a degree or less[31], while Isaksen et al.[32] have reported warming of Scandinavian permafrost. Table 6.8 summarizes recent trends in permafrost temperatures in terms of region, time period, and the approximate temperature change over the period of record. In general, the changes in permafrost temperature are consistent with other environmental changes in the circumpolar Arctic[33].
Most of the boreholes mentioned in this section are included in an emerging system for comprehensive monitoring of permafrost temperatures (Fig. 6.21), the Global Terrestrial Network for Permafrost (GTN-P), established with the assistance of the International Permafrost Association. Burgess et al.[34] provide an overview of the GTN-P.
This section describes regional projections that were generated by soil models run at high resolution for an area in which relatively detailed information on soil properties was available. The soil information included soil temperatures used for model calibration. While this section presents results for northern Alaska, model-based evaluations of the sensitivities of permafrost to warming in other areas, including Canada, are also available[59].
Detailed projections of future changes in permafrost in northern Alaska were obtained from a soil model[60] calibrated using observational data from three sites on the North Slope of Alaska. The two major types of vegetation in northern Alaska are tundra and taiga (boreal forest). Permafrost is continuous north of the Brooks Range and discontinuous in much of Interior Alaska to the south. Permafrost is >600 m thick in northern areas but is only one to several meters thick near its southern limits. In the lowlands of the southern discontinuous zone, where the mean annual air temperature ranges from -7 to 0°C, the temperature of the permafrost below the layer of seasonal temperature variation ranges from -5 to -1°C. In the continuous permafrost zone north of the Brooks Range, permafrost temperatures typically range from -11 to -4°C.
Surface air temperature and snow-cover projections from the five ACIA-designated climate models and the older HadCM2 model[61], forced with the B2 emissions scenario (section 4.4.1), were used as input to the soil model to project the active-layer and mean annual ground-temperature dynamics in northern Alaska between 2000 and 2100. The across-model average projected increase in mean annual air temperature between 2000 and 2100 ranges from 8 to 10°C in the north to 4 to 6°C in the southern part of the region.
In the central and northern areas of Alaska, projected increases in mean annual ground temperatures between 2000–2010 and 2100 range from 1 to 2°C using the CGCM2 climate scenario to 5°C using the HadCM3 and ECHAM4/OPYC3 scenarios (Fig. 6.25). The HadCM3, HadCM2, and ECHAM4/OPYC3 scenarios generate significant projected increases in mean annual ground temperatures over the entire area.
An analysis of the maximum active-layer thickness was also performed. All the scenarios project that, by 2100, the active-layer thickness is likely to increase by up to 1 m in areas occupied by coarse-grained material and rocks with high thermal conductivity, and by up to 0.5 m throughout the rest of the region (Fig. 6.26). The HadCM2, HadCM3, and ECHAM4/OPYC3 scenarios generate the greatest projected increases in active-layer thickness.
By 2100, all the scenarios except for the CSM_1.4 project that a zone with permafrost degradation (failure of some portion of the former active layer to refreeze during winter) will exist in northern Alaska (Fig. 6.26). The HadCM2 and GFDL-R30_c scenarios project that this zone will occupy the southeastern part of the modeled area. The HadCM2 scenario projects a relatively constant increase in this zone throughout the years, with almost one-third of the modeled area degraded by 2100. The ECHAM4/OPYC3 scenario projects the second largest zone of degradation by 2100, but the development of this zone throughout the century is not uniform. The CGCM2 scenario projects that this zone will be located in the southeastern and central parts of the modeled area and in the Brooks Range. The HadCM3 and ECHAM4/OPYC3 scenarios project that the zone will occupy the southeastern and southwestern parts of the modeled area and some parts of the Brooks Range (the eastern part in HadCM3, the western part in ECHAM4/OPYC3). The GFDL-R30_c scenario projects that the zone of permafrost degradation will occupy less than 5 to 7% of the modeled area. The CSM_1.4 scenario is an outlier in that it projects no permafrost degradation between 2000 and 2100.
Similar dependencies on climate model forcing scenarios have been found by Malevsky-Malevich et al.[62], who used output from the same climate models to drive a different type of soil model. The results of these simulations showed that the projected active-layer response in Siberia would be greater in southern and western regions than in eastern and northern regions, indicating the potential importance of snow cover to projections of permafrost change[63]. The decrease in snow-cover duration is projected to be greater in southern and western Siberia than in northern and eastern Siberia, and greater in the spring season (section 6.4) when insolation is relatively high.
The scenarios of permafrost change clearly vary with the choice of climate model, and they contain many examples of decadal-scale variations that can complicate the detection of change. Nevertheless, the projected changes are substantial in nearly all cases, and terrestrial permafrost is likely to remain one of the more useful indicators of global change because large regions of the arctic terrestrial system now have mean annual temperatures close to 0°C.
Projected climate change is very likely to increase the active-layer thickness and the thawing of permafrost at greater soil depths. The impacts of permafrost degradation include changes in drainage patterns and surface wetness resulting from subsidence and thermokarst formation, especially where soils are ice-rich. Thawing of ice-rich permafrost can trigger mass movements on slopes, and possibly increase sediment delivery to water-courses. Thawing of permafrost in peatlands and frozen organic matter sequestered by cryoturbation is likely to accelerate biochemical decomposition and increase the GHGs released into the atmosphere.
Changes in surface drainage and wetness are likely to result in vegetative changes (e.g., shallow-rooted versus deeper-rooted vegetation, changes in plant density); the development of thermokarst has transformed some upland forests into extensive wetlands. Microbial, insect, and wildlife populations are likely to evolve over time as soil drainage and wetness change (section 7.4.1). Changes in drainage resulting from changes in the distribution of permafrost are also likely to affect terrestrial ecosystems, and will determine the response of peatlands and whether they become carbon sources or sinks (section 7.5.3).
Permafrost degradation is likely to cause instabilities in the landscape, leading to surface settlement and slope collapse, which may pose severe risks to infrastructure (e.g., buildings, roads, pipelines). The possibilities for land use change with soil wetness. Offshore engineering (e.g., for resource extraction) is highly affected by coastal permafrost and its degradation (section 16.3.10). Containment structures (e.g., tailing ponds, sewage lagoons) often rely on the impermeable nature of frozen ground; thawing permafrost would reduce the integrity of these structures. Over the very long term, the disappearance of permafrost coupled with infrastructure replacement will eliminate many of the above concerns.
In order to improve the credibility of model projections of future permafrost change throughout the Arctic, the soil/vegetation models must be validated in a more spatially comprehensive manner. In particular, there is a need for intercomparison of permafrost models using the same input parameters and standardized measures for quantifying changes in permafrost boundaries. Global models do not yet use such regionally calibrated permafrost models, nor do they treat the upper soil layers in sufficient detail to resolve the active layer. The need for additional detail is particularly great for areas with thin permafrost (e.g., Scandinavia). Enhanced model resolution, and validation and calibration at the circumpolar scale, will be necessary before fully coupled simulations by global models will provide the information required for assessment activities such as the ACIA.
There is likely to be a significant linkage between changes in terrestrial permafrost and the hydrology of arctic drainage basins. Long-term field data are required to increase understanding of permafrost–climate interactions and the interaction between permafrost and hydrological processes, and for model improvement and validation. The active-layer measurements from the Circumpolar Active Layer Monitoring Program and the borehole measurements from the GTN-P will be especially valuable in this regard, if the numbers of sites are increased.
The terms subsea (or offshore) and coastal permafrost refer to geological materials that have remained below 0°C for two or more years and that occur at or below sea level. At present, the thermal regime of subsea permafrost is controlled partially or completely by seawater temperature. Subsea permafrost has formed either in response to negative mean annual sea-bottom temperatures or as the result of inundation of terrestrial permafrost. Coastal permafrost includes the areas of permafrost that are near a coastline (offshore or onshore) and that are affected, directly or indirectly, by marine processes. Direct marine influences include seawater temperature, sea-ice action, storm surges, wave action, and tides. Indirect marine influences include the erosion of cliffs and bluffs. This review focuses on those parts of the permafrost environment found below the storm tide line, since the thermal and chemical environments that affect them are substantially different from those affecting terrestrial permafrost.
The development and properties of subsea permafrost are largely dependent on the detailed history of postglacial relative sea level. Coastal permafrost conditions are influenced by a range of oceanographic and meteorological processes, ranging from sea-ice thickness to storm-surge frequency. During the transition from terrestrial to submarine, permafrost is subjected to a set of intermediary environments that affect its distribution and state.
Based on the strict definition above, not all permafrost is frozen, since the freezing point of sediments may be depressed below 0°C by the presence of salt or by capillary effects in fine-grained material. In the marine environment, non-frozen materials do not present serious problems for engineering activities, so modifiers are used to further define frozen permafrost as either ice-bonded, ice-bearing, or both[64]. Ice-bearing material refers to permafrost or seasonally frozen sediments that contain some ice. Ice-bonded sediments are mechanically cemented by ice. While the ice component of permafrost usually consists of pore or interstitial ice that fills the small spaces between individual grains of sand, silt, or gravel, it sometimes occurs in much larger forms referred to as "massive ice". Unfrozen fluids may be present in the pore spaces in both ice-bearing and ice-bonded materials. As with terrestrial permafrost, some subsea permafrost has an active (seasonally thawed) layer. Hubberten and Romanovskii[65] discussed the characteristics of permafrost in one particular offshore environment, the Laptev Sea.
While the stability of terrestrial permafrost depends directly on atmospheric forcing (temperature and precipitation), the effect of atmospheric forcing on the stability of subsea permafrost is a second- or third-order impact mediated through oceanographic and sea-ice regimes. Most subsea permafrost formed during past glacial cycles, when continental shelves were exposed to low mean annual temperatures during sea-level lowstands, thus it is restricted to those parts of the Arctic that were not subjected to extensive glaciation during the Late Quaternary Period[66]. Permafrost that developed on exposed continental shelves during glacial epochs subsequently eroded when sea-level rise submerged the shelves during interglacial warm intervals and regraded the land surface to a quasi-equilibrium seabed profile. Positive mean annual sea-bottom temperatures degrade upland permafrost as it passes through the coastal zone, but with continued sea-level rise, the sea-bottom water temperature falls to negative values and permafrost degradation slows. Thus, in any locality, the distribution of relict subsea permafrost is a function of its original distribution on land, and the depth to ice-bonded or ice-bearing permafrost is a function of the time spent in the zone of positive sea-bottom temperatures along with other variables (e.g., volumetric ice content, salt content, etc.)[67].
Subsea relict permafrost is thought to contain or overlie large volumes of CH4 in the form of gas hydrates at depths of up to several hundred meters. Degradation of gas hydrates resulting from climate change (section 6.6.2.3) could increase the flux of CH4 to the atmosphere[68].
A combination of observations and models has been used to estimate the distribution of subsea permafrost (Fig. 6.27). The distribution is largely inferred from glacial extent during the last glacial maximum, water temperature, and the location of the 100 m depth contour (approximate minimum sea level during the past 100,000 years). Narrow zones of coastal permafrost are probably present along most arctic coasts.
Coastal and subsea permafrost can be subdivided into four zones (Fig. 6.28), based primarily on water depth and on the dominant processes that operate in those depth zones[69]. Zone 1 covers the inter- and supra-tidal environments of the beaches and flats. Seaward of the intertidal zone, in Zone 2, the seasonal ice cover freezes to the seabed each year, allowing cold winter temperatures to penetrate the water column and reach the sediments. This occurs in water depths of 1.5 to 2 m. Zone 3 covers areas where water depths are too great for the sea ice to freeze to the seabed; however, under-ice circulation may be restricted, with attendant higher salinities and lower seabed temperatures. In Zone 4, "normal" seawater salinity and temperatures prevail, providing a more or less constant regime. Sea-bottom temperatures on the arctic shelves range from -1.5 to -1.8°C; salinities range from 30 to 34[70].
There are no ongoing programs to monitor the state of coastal and subsea permafrost, although some effort is being devoted to monitoring the forcing variables and coastal erosion[71] (Table 16.8). Therefore, most publications addressing changes in the state of subsea permafrost are model-based and speculative. Zones 1 and 2 are the most dynamic, especially in locations where erosion is rapid (e.g., the Laptev and Beaufort Sea coasts). In these areas, erosion rates of several meters per year cause a rapid transition from terrestrial to nearshore marine conditions. High rates of erosion caused by exposure to waves and storm surges during the open water season lead to deep thermal notch development in cliffs, block failure in the backshore (area reached only by the highest tides), melting of sea-level-straddling massive ice, and possible offshore thermokarst development[72]. The rate at which destabilization of permafrost in these zones occurs is dependent on the erosion rate, which in turn varies according to storm frequency and severity[73] and the presence or absence of sea ice. The degree to which permafrost destabilization affects erosion remains conjectural. Thaw subsidence in Zones 2 and 3 that accompanies melting of excess ice (ice that is not in thermal equilibrium with the existing soil–ice–air configuration) in the nearshore provides accommodation space for sediments produced by erosion. Thus, there is a potential feedback between high erosion rates and thaw subsidence, but there are few observations to support this hypothesis. An analysis of time series of erosion measurements and environmental forcing (e.g., weather, storms, freeze-thaw cycles) in the Beaufort Sea area did not reveal any trends, but showed pronounced interannual and decadal-scale variability[74].
Sea-ice thickness plays a major role in the development of subsea permafrost within Zone 2. However, none of the recent analyses of historic data on sea-ice thickness in the Arctic[75] (section 6.3.2) addresses the state of the sea ice that forms very close to the coast[76], since the coastal waters are too shallow for submarines. Time series of ice thickness measurements from several coastal locations extending back to the late 1940s are available from the Canadian Ice Service[77]. Polyakov et al.[78] describe a similar dataset from Russia. Neither dataset shows any trend over the period of record, which is dominated by large interannual fluctuations. Figure 6.29 illustrates the variability in the annual maximum thickness of landfast ice measured at four coastal locations in the Canadian Arctic. Smoothing the data with a five-year moving average reveals some similarities between the stations.
Air-temperature changes in the Arctic are well documented, and many studies have examined the impact of these changes on the active-layer thickness and temperature of terrestrial permafrost, however, there are no equivalent multi-year studies for coastal permafrost.
Seabed temperature is a critical upper boundary condition for subsea permafrost. Decadally averaged temperatures (1950s–1980s) for various water depths in the Arctic Ocean are available from the National Snow and Ice Data Center in Boulder, Colorado[79]. These data indicate that there have been decadal-scale changes of a degree or more in the temperatures of shallow water, and smaller changes in deeper water (Fig. 6.30). Interdecadal variability is apparent along the Beaufort Shelf (warmer in the 1960s and 1980s) and the Laptev Sea Shelf (cooler in the 1980s).
The stability of coastal and subsea permafrost in a changing climate depends directly on the magnitude of changes in water temperature and salinity, air temperature, sea-ice thickness, and coastal and seabed stability. It is difficult to extract the relevant projections of environmental forcing (subsurface and seabed water temperatures in particular) from any of the scenarios generated by climate models. In general terms:
Decreases in the stability of coastal permafrost are likely to result in greater nearshore thaw subsidence and increased rates of coastal erosion. This will introduce greater sediment loads to the coastal system; higher levels of suspended sediment and changes in depositional patterns may ensue. Increased erosion rates will also result in greater emissions of CO2 from coastal and nearshore sources, and increased emission rates of CH4 from terrestrial permafrost. Over the long-term, destabilization of intra-permafrost gas hydrates is likely to enhance climate change.
Changing deposition patterns and suspended sediment loads along the coast are likely to have impacts on marine ecosystems, including anadromous fish migration, phytoplankton blooms, and benthic communities. Negative or positive impacts are possible. Increased suspended material may increase nutrients, resulting in higher productivity in nutrient-limited systems. Conversely, increased suspended material lowers light levels, resulting in lower productivity. The potential impacts of changes in subsea and coastal permafrost on marine ecosystems are discussed further in Chapter 9.
Decreases in the stability of coastal permafrost will have an impact on coastal infrastructure. Increased erosion rates, caused in part by nearshore thaw subsidence, are likely to affect communities and industrial facilities situated close to the coast. Permafrost thawing and subsidence could affect pipelines in nearshore and coastal environments in excess of their design specifications. Warming and/or thawing permafrost is likely to reduce the foundation strength of wharves and associated pilings.
In deeper water (Zones 3 and 4), permafrost warming could affect design considerations for hydrocarbon production facilities, including casing strings and platforms anchored to the seabed. Chapter 16 addresses specific infrastructure issues associated with changes in coastal permafrost.
A circumpolar program to monitor changes in the coastal and offshore cryosphere is required, as is a better understanding of the processes that drive those changes. The Arctic Coastal Dynamics (ACD) project, sponsored by the International Arctic Science Committee and the International Permafrost Association, is promoting the need for such studies. At present, there is no monitoring of coastal and subsea permafrost, and this lack represents a critical gap in the understanding of coastal stability in the Arctic. The absence of monitoring is a result of the difficulty in working in arctic coastal environments, particularly in Zones 1 and 2. Equipment for measuring temperatures throughout the year must be placed in such a way that cables are not jeopardized by storms and sea ice. The technology exists, but it is more expensive than that used for similar measurements on land.
A comprehensive understanding of coastal permafrost processes, including the interaction between storms and permafrost, is needed. Heat convection is thought to play a major role in coastal permafrost thawing during storms after the thawed overlying material is removed[82]. However, given the difficulty of making measurements at the shoreline under storm conditions, there are no observations supporting this hypothesis. Laboratory studies could play a role in this regard. Thaw subsidence rates can exceed the rate of eustatic sea-level rise (rise due to changes in the mass of ocean water, see section 6.9.1), and are therefore thought to contribute to coastal erosion, at least at a local scale. However, there are few documented observations of the magnitude of thaw subsidence and/or its role in coastal erosion.
The role of brine exclusion and convection in enhancing coastal and subsea permafrost degradation requires further investigation.
Finally, the gas hydrates in coastal and subsea permafrost require further study in order to evaluate their stability over the range of future climate change scenarios produced by climate models.
[[category:|Permafrost in the Arctic]]
The Queen Charlotte Islands represent a major offshore archipelago of islands separated from the British Columbia and Alaskan mainland by Hectate Strait at a distance of approximately 75-100 kilometers (km).
The climate in this ecoregion is considered oceanic and maritime South Pacific Cordilleran. The mean annual temperature is 7.5°C, mean summer temperature is 11.5°C, and mean winter temperature is 3.5°C. Annual precipitation in the islands is between 800 (in eastern areas) and 4,000 millimeters (mm) (on western slopes) per year.
Physiographically, the Queen Charlotte Islands are characterized by irregular, steep slopes in the west and gently sloping lowlands in the east.
This ecoregion has significant areas of old-growth, west coast rainforests. Watersheds on the islands are important for anadromous fish while elevational gradients result in high terrestrial species richness and community variation.
Along the west coast of the islands, vegetation is comprised of stunted, open-growing western red cedar (Thuja plicata), yellow cedar (Chamaecyparis nootkatensis), shore pine (Pinus contorta var. contorta), and western hemlock (Tsuga heterophylla). Better drained sites also support Sitka spruce (Picea sitchensis). Wetlands are common in the islands and are comprised of open western hemlock and shore pine.
Several species of introduced mammals are present on the island, including black-tailed deer (Odocoileus hemionus), elk (Cervus elaphus), raccoon (Procyon lotor), rats (Rattus spp.), eastern gray squirrel (Sciurus carolinensis) and beaver (Castor canadensis). Native, common wildlife includes black bear (Ursus americanus), river otter (Lontra canadensis), seabirds, shorebirds, and marine mammals.
This ecoregion is a critical stopover for migratory waterbirds flying north to Alaska and south to Mexico. As one of the most isolated island archipelagos in western North America, the ecoregion harbors several endemic subspecies of plants, birds, and small mammals as well as an endemic sub-species of black bear. Critical nesting sites for colonial nesting birds and raptors are also found here.
Approximately 50% of the habitat has been altered on the Queen Charlotte Islands, primarily as a result of clearcut logging. The remaining habitat is relatively intact. High rainfall levels in this ecoregion have created serious erosion and landslide problems where logging has been extensive. The logging has provided habitat suitable for the introduced black-tailed deer, which in turn are causing other serious habitat impacts through selective over-browsing of some conifer and forest understory species.
Logging has been the principal land-use responsible for the fragmentation of habitat. Since logging is directed principally at the valley bottom and lower slope forests, fragmentation occurs for upper slope communities and impacts species movements.
Logging and road building remain significant threats to mature forest habitat and to some species such as marbled murrelets (Brachyramphus marmoratus), cavity nesters and raptors. Introduced species to this island system are also a major threat to native biodiversity. Black tailed deer are having a major impact on the regeneration of western red cedar, a dominant species in many of the islands’ forested habitats. Damming by introduced beaver of small streams used by coho salmon (Oncorhynchus kisutch) for spawning threaten some stocks. The introduction of rats (Rattus spp.), squirrels (Sciurus spp.) and raccoons have had a profound impact on seabird colonies.
The Queen Charlotte Islands are characterized by the Queen Charlotte Lowland and Ranges (TEC 188 and 189). The Ranges form the backbone of the Islands, and the Lowland in the north and east is primarily forested plain and wetlands. The Islands fall within the Coast forest region (4), and have a rainforest type of vegetation.
The Sultanate of Oman occupies the south-eastern corner of the Arabian Peninsula and has a total area of 312,500 km2. It is bordered in the north-west by the United Arab Emirates, in the west by Saudi Arabia and in the south-west by Yemen. A detached area of Oman, separated from the rest of the country by the United Arab Emirates, lies at the tip of the Musandam Peninsula, on the southern shore of the Strait of Hormuz. The country has a coastline of almost 1,700 km, from the Strait of Hormuz in the north to the borders of the Republic of Yemen in the south-west, overlooking three seas: the Persian Gulf, the Gulf of Oman and the Arabian Sea.
Oman can be divided into the following physiographic regions:
The cultivable area has been estimated at 2.2 million hectares (ha), which is 7% of the total area of the country. The cultivated area was 61,550 ha in 1993, of which 18,550 ha consisted of annual crops and 43,000 ha consisted of permanent crops. Over half the agricultural area is located in the Batinah Plain in the north which has a total area representing about 3% of the area of the country.
The total population is about 2.16 million (1995), of which 87% is rural according to United Nations (UN) estimates.
According to the national population census of 1993, 28% of the total population was rural. The difference between the two figures is explained by the fact that the UN standards for Oman consider as rural all the inhabitants of the country, except those of the two cities: Muscat and Matrah. The annual demographic growth rate is estimated at 3.7%. While agriculture and fisheries employed about 37% of the total labor force in 1993, they accounted for only 3.3% of gross domestic product (GDP).
The climate differs from one region to another. It is hot and humid during summer in the coastal areas and hot and dry in the interior regions with the exception of some higher lands and the southern Dhofar region, where the climate remains moderate throughout the year. In the north and center of Oman, rainfall occurs during the winter (November-April), while in the south and some internal parts of the country it is a result of seasonal summer storms (June-September). Average annual rainfall has been estimated at 55 mm, varying from less than 20 mm in the internal desert regions to over 300 mm in the mountain areas.
A great deal of uncertainty lies in the assessment of Oman's water resources. Internal renewable water resources have been evaluated at 985 million m3/year. Surface water resources are scarce. In nearly all wadis, surface runoff occurs only for some hours or up to a few days after a storm, in the form of rapidly rising and falling flood flows. Since 1985, 15 major recharge dams have been constructed together with many smaller structures, in order to retain a portion of the peak flows, thus allowing more opportunity for groundwater recharge. In addition, several flood-control dams produce significant recharge benefits. In 1996, the total dam capacity is 58 million m3. Groundwater recharge is estimated at 955 million m3/year.
In 1995, the total produced wastewater was estimated at 58 million m3. Only 28 million m3 was treated, of which 26 million m3 was reused. Also in 1995, the quantity of desalinated water was 34 million m3.
In 1995, total water withdrawal was 1,223 million m3, of which 93.9% for agricultural purposes (4.6% is withdrawn for domestic use and 1.5% for industrial use). The treated wastewater was reused mainly for the irrigation of trees along the roads, while the desalinated water was used for domestic purposes. At present, groundwater depletion is thus estimated at around 240 million m3/year.
All agriculture in Oman is irrigated and since the 1970s the equipped area increased from about 28,000 ha to 61,550 ha in 1993, of which 34,930 ha, or almost 57%, is located in the Al Batinah province in the north. Although 2.2 million ha are considered to be suitable for agriculture, there are no figures on the irrigation potential, as no reliable data are available on groundwater availability in the deep aquifers. At present, groundwater depletion already takes place, especially in coastal areas, leading to seawater intrusion and a deterioration in water quality.
The falaj system ('aflaj' in the plural) is the traditional method developed centuries ago for supplying water for irrigation and domestic purposes. Many of the systems currently in use are estimated to be over a thousand years old. The falaj comprises the entire system: the source, which might be a qanat, a spring or the upper reaches of flowing wadis from which water is diverted; the conveyance system, which is usually an open-earth or cement-lined ditch; and the delivery system. The falaj has assumed social significance, and well established rules of usage, maintenance and administration have evolved.
Originally, the falaj developed where higher-elevation water sources such as springs, qanats or surface water could be intercepted by diversion or small catchment dams and then conveyed by gravity to the point of use. More recently, however, dug wells have been used to supplement the falaj water. This is especially the case in the coastal areas where many hand-dug wells and tubewells have been constructed. For 47% of the total number of 62,411 households involved in irrigation, wells are now the main source of water, 39% rely on falaj water, while the remaining 14% have access to both sources.
Of the total area of 61,550 ha equipped for irrigation, all of which is power-irrigated using groundwater (wells, falaj), only 1,640 ha, or 2.7%, benefit from sprinkler irrigation and 2,090 ha, or 3.4%, from micro-irrigation techniques. Although the Ministry of Agriculture and Fisheries (MAF) is making efforts to introduce modern irrigation techniques, the traditional flood system remains the most common irrigation technique. In order to encourage farmers to take up the new techniques, MAF has approved a financial subsidy varying between 75% for small-scale schemes (less than 10 feddans or 4.2 ha), 50% for medium-scale schemes and 25% for large-scale schemes (more than 50 feddans or 21 ha). Most of the area consists of small schemes.
In 1996, the cost of irrigation development was estimated at US$3,250/ha for medium and large schemes and US$4,415/ha for small schemes. These costs represent the average cost of installing sprinkler irrigation and micro-irrigation systems. The average annual operation and maintenance costs are US$845, 1,170 and 1,820/ha for large, medium and small schemes respectively.
Date palm is the main crop grown in Oman, occupying about half the total cropped area. Other crops are fodder crops (mainly alfalfa), other fruit trees (citrus, bananas, mangoes, coconuts) vegetables and cereals (mainly barley, wheat and sorghum).
No reliable information on the area salinized by irrigation is available. A study done in 1994 on the salinity of soils in general in Oman, states that an area of 11.7 million ha, which is 35% of the total area of Oman, is affected by salinity. No drainage is practiced.
Until May 2001, the Ministry of Water Resources (MOWR) was in charge of water resources assessment, whereas the Ministry of Agriculture and Fisheries (MAF) was in charge of irrigation. However, in May 2001, the Ministry of Water Resources was cancelled and its activities were transferred to the Ministry of Regional Municipality and Environment and Water Resource.
In 1988, Royal Decree No. 83/88 declared the water resources of Oman a national resource. This is the most far-reaching and important piece of legislation on water resources. Oman has several laws on water resources and the main measures taken for water management and conservation are:
Three broadly-based programs have been set up by the government for:
In addition to the above measures taken for water management and conservation, the government has recently initiated programs to relocate some of the large-scale farms in the Batinah and Salalah Plains, where the water resources are over-utilized, to areas with underutilized water resources. Several water conservation initiatives have been developed, like leakage control in municipal water supply schemes and the improvement of irrigation methods through subsidy programs. Public awareness of water resources issues has created a general and focused understanding of the overall situation and of the specific contribution each citizen can make.
The main issues and strategies that the government will address in the coming years are: