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  • 1
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    PANGAEA
    In:  NASA Earth Observatory | Supplement to: Gardner, Alex S; Moholdt, Geir; Wouters, Bert; Wolken, G J; Burgess, D O; Sharp, M J; Cogley, J G; Braun, C; Labine, C (2011): Sharply increased mass loss from glaciers and ice caps in the Canadian Arctic Archipelago. Nature, 473(7347), 357-360, https://doi.org/10.1038/nature10089
    Publication Date: 2023-02-18
    Description: Though much attention has been focused in recent years on the melting of ice from Greenland and Antarctica, nearly half of the ice volume currently being lost to the ocean is actually coming from other mountain glaciers and ice caps. Ice loss from a group of islands in northern Canada accounts for much of that volume. In a study published in April 2011 in the journal Nature, a team of researchers led by Alex Gardner of the University of Michigan found that land ice in both the northern and southern Canadian Arctic Archipelago has declined sharply. The maps above show ice loss from surface melting for the northern portion of the archipelago from 2004-2006 (left) and 2007-2009 (right). Blue indicates ice gain, and red indicates ice loss. In the six years studied, the Canadian Arctic Archipelago lost an average of approximately 61 gigatons of ice per year. (A gigaton is a billion tons of ice.) The research team also found the rate of ice loss was accelerating. From 2004 to 2006, the average mass loss was roughly 31 gigatons per year; from 2007 to 2009, the loss increased to 92 gigatons per year. Gardner and colleagues used three independent methods to assess ice mass, all of which showed the same trends. The team used a model to estimate the surface mass balance of ice and the amount of ice discharged. They also compiled and analyzed measurements from NASA's Ice, Cloud and Land Elevation Satellite (ICESat) to assess changes in the surface height of ice. Finally, they gathered observations from NASA's Gravity Recovery and Climate Experiment (GRACE) to determine changes in the gravity field in the region, an indicator of the amount of ice gained or lost. The Canadian Arctic Archipelago generally receives little precipitation, and the amount of snowfall changes little from year to year. But the rate of snow and ice melting varies considerably, so changes in ice mass come largely from changes in summertime melt. During the 2004 to 2009 study period, the Canadian Arctic Archipelago experienced four of its five warmest years since 1960, likely fueling the melting. Gardner notes that from 2001 to 2004, the sum of melting from all mountain glaciers and ice caps around the world (but not the Greenland and Antarctic ice sheets) contributed an estimated 1 millimeter per year to global sea level rise. Recent estimates suggest the Greenland and Antarctic ice sheets add another 1.3 millimeters per year to sea level. "This means 1 percent of the land ice volume--mountain glaciers and ice caps--account for about half of all ice loss to the world's oceans," Gardner said. "Most of the ice loss is coming from the Canadian Arctic Archipelago, Alaska, Patagonia, the Himalayas, and the smaller ice masses surrounding the main Greenland and Antarctic ice sheets."
    Keywords: Date/time end; Date/time start; Ellesmere_Island; Ellesmere Island, Canadian Arctic Archipelago; File format; File size; Uniform resource locator/link to image
    Type: Dataset
    Format: text/tab-separated-values, 25 data points
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Langmuir 11 (1995), S. 764-766 
    ISSN: 1520-5827
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Manuscripta mathematica 96 (1998), S. 23-35 
    ISSN: 1432-1785
    Keywords: Mathematics Subject Classification (1991):43A20
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract: Let V be an exponential ?-module, ? being an exponential Lie algebra. Put ? = exp ?. Then every orbit of V under the action of ? admits a closed orbit in its closure. If G= exp ? is a nilpotent Lie group and ? an exponential algebra of derivations of ?, then ? = exp ? acts on G, L 1(G), (?) and the maximal ?-invariant ideals of L 1(G), resp. of (?) coincide with the kernels Ker Ω, resp. Ker Ω∩ (?), where Ω is a closed orbit of ?*.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    The journal of membrane biology 142 (1994), S. 229-240 
    ISSN: 1432-1424
    Keywords: Calcium ; Exocytosis ; Membrane fusion ; Paramecium tetraurelia ; Veratridine
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology , Chemistry and Pharmacology
    Notes: Abstract Paramecium tetraurelia wild-type (7S) cells respond to 2.5 mm veratridine by immediate trichocyst exocytosis, provided [Ca2+] o (extracellular Ca2+ concentration) is between about 10−4 to 10−3 m as in the culture medium. Exocytosis was analyzed by light scattering, light and electron microscopy following quenched-flow/ freeze-fracture analysis. Defined time-dependent stages occurred, i.e., from focal (10 nm) membrane fusion to resealing, all within 1 sec. Veratridine triggers exocytosis also with deciliated 7S cells and with pawn mutants (without functional ciliary Ca channels). Both chelation of Ca2+ o or increasing [Ca2+] o to 10−2 m inhibit exocytotic membrane fusion. Veratridine does not release Ca2+ from isolated storage compartments and it is inefficient when microinjected. Substitution of Na+ o for N-methylglucamine does not inhibit the trigger effect of veratridine which also cannot be mimicked by aconitine or batrachotoxin. We conclude that, in Paramecium cells, veratridine activates Ca channels (sensitive to high [Ca2+] o ) in the somatic, i.e., nonciliary cell membrane and that a Ca2+ influx triggers exocytotic membrane fusion. The type of Ca channels involved remains to be established.
    Type of Medium: Electronic Resource
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  • 5
    ISSN: 1432-1424
    Keywords: Key words: Calcium — Endocytosis — Exocytosis — Membrane fusion — Secretion —Paramecium
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology , Chemistry and Pharmacology
    Notes: Abstract. We had previously shown that an influx of extracellular Ca2+ (Ca2+ e ), though it occurs, is not strictly required for aminoethyldextran (AED)-triggered exocytotic membrane fusion in Paramecium. We now analyze, by quenched-flow/freeze-fracture, to what extent Ca2+ e contributes to exocytotic and exocytosis-coupled endocytotic membrane fusion, as well as to detachment of ``ghosts'' — a process difficult to analyze by any other method or in any other system. Maximal exocytotic membrane fusion (analyzed within 80 msec) occurs readily in the presence of [Ca2+] e ≥ 5 × 10−6 m, while normally a [Ca2+] e = 0.5 mm is in the medium. A new finding is that exocytosis and endocytosis is significantly stimulated by increasing [Ca2+] e even beyond levels usually available to cells. Quenching of [Ca2+] e by EGTA application to levels of resting [Ca2+] i or slightly below does reduce (by ∼50%) but not block AED-triggered exocytosis (again tested with 80 msec AED application). This effect can be overridden either by increasing stimulation time or by readdition of an excess of Ca2+ e . Our data are compatible with the assumption that normally exocytotic membrane fusion will include a step of rapid Ca2+-mobilization from subplasmalemmal pools (``alveolar sacs'') and, as a superimposed step, a Ca2+-influx, since exocytotic membrane fusion can occur at [Ca2+] e even slightly below resting [Ca2+] i . The other important conclusion is that increasing [Ca2+] e facilitates exocytotic and endocytotic membrane fusion, i.e., membrane resealing. In addition, we show for the first time that increasing [Ca2+] e also drives detachment of ``ghosts'' — a novel aspect not analyzed so far in any other system. According to our pilot calculations, a flush of Ca2+, orders of magnitude larger than stationary values assumed to drive membrane dynamics, from internal and external sources, drives the different steps of the exo-endocytosis cycle.
    Type of Medium: Electronic Resource
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  • 6
    ISSN: 0003-2697
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Biology , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 7
    ISSN: 0008-6215
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 87 (1983), S. 4776-4778 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 91 (1987), S. 4436-4438 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 30 (1987), S. 499-509 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A three-level atomic model is used for determining the steady-state collisional-radiative coefficients in nonequilibrium partially ionized argon plasmas. Rate equations for populations of the atomic levels are coupled to an electron Boltzmann equation that includes inelastic processes. The solution of these coupled equations yields an analytical form for the non-Maxwellian electron distribution function. The reabsorption of radiation in the plasma is included through the use of Holstein radiation escape factors [Phys. Rev. 83, 1159 (1951)]. The cross sections in this model are included in the form of simple analytical expressions obtained from a numerical fitting of available experimental data. The results and limitations of the approach are discussed in a broad range of plasma conditions (electron temperature below 25 000 °K and atomic density of 1014–1018 cm−3).
    Type of Medium: Electronic Resource
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