<?xml version="1.0" encoding="utf-8"?><rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns="http://purl.org/rss/1.0/" xmlns:dc="http://purl.org/dc/elements/1.1/"><channel rdf:about="http://www.the-cryosphere-discuss.net/xml/rss1_0.xml"><title>TCD - Latest Articles</title><link>http://www.the-cryosphere-discuss.net/</link><description>The Cryosphere Discussions Latest Articles</description><items><rdf:Seq><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2943/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2891/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2845/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2801/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2761/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2725/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2703/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2679/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2635/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2595/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2567/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2533/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2489/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2455/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2413/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2373/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2333/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2293/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2247/2013/" /><rdf:li resource="http://www.the-cryosphere-discuss.net/7/2191/2013/" /></rdf:Seq></items></channel><item rdf:about="http://www.the-cryosphere-discuss.net/7/2943/2013/"><title>What drives basin scale spatial variability of snow water equivalent during two extreme years?</title><link>http://www.the-cryosphere-discuss.net/7/2943/2013/</link><description>&lt;b&gt;What drives basin scale spatial variability of snow water equivalent during two extreme years?&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2943-2977, 2013&lt;br /&gt;&lt;br /&gt;Author(s): G. A. Sexstone and S. R. Fassnacht&lt;br /&gt;&lt;br /&gt;This study uses a combination of field measurements and Natural
  Resource Conservation Service (NRCS) operational snow data to
  understand the drivers of snow water equivalent (SWE) spatial
  variability at the basin scale. Historic snow course snowpack
  density observations were analyzed within a multiple linear
  regression snow density model to estimate SWE directly from snow
  depth measurements. Snow surveys were completed on or about 1 April
  2011 and 2012 and combined with NRCS operational measurements to
  investigate the spatial variability of SWE. Bivariate relations and
  multiple linear regression models were developed to understand the
  relation of SWE with terrain and canopy variables (derived using
  a geographic information system (GIS)). Calculation of SWE directly
  from snow depth measurement using the snow density model has strong
  statistical performance and model validation suggests the model is
  transferable to independent data within the bounds of the original
  dataset. This pathway of estimating SWE directly from snow depth
  measurement is useful when evaluating snowpack properties at the
  basin scale, where many time consuming measurements of SWE are often
  not feasible. During both water year (WY) 2011 and 2012, elevation
  and location (UTM Easting and UTM Northing) were the most important
  model variables, suggesting that orographic precipitation and storm
  track patterns are likely consistent drivers of basin scale SWE
  variability.  Terrain characteristics, such as slope, aspect, and
  curvature, were also shown to be important variables, but to
  a lesser extent at the scale of interest.</description><dc:date>2013-06-18T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2891/2013/"><title>2001&amp;ndash;2010 glacier changes in the Central Karakoram National Park: a contribution to evaluate the magnitude and rate of the &quot;Karakoram anomaly&quot;</title><link>http://www.the-cryosphere-discuss.net/7/2891/2013/</link><description>&lt;b&gt;2001&amp;ndash;2010 glacier changes in the Central Karakoram National Park: a contribution to evaluate the magnitude and rate of the &quot;Karakoram anomaly&quot;&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2891-2941, 2013&lt;br /&gt;&lt;br /&gt;Author(s): U. Minora, D. Bocchiola, C. D'Agata, D. Maragno, C. Mayer, A. Lambrecht, B. Mosconi, E. Vuillermoz, A. Senese, C. Compostella, C. Smiraglia, and G. Diolaiuti&lt;br /&gt;&lt;br /&gt;Karakoram is one of the most glacierized region worldwide, and
      glaciers therein are the main water resource of Pakistan. The
      attention paid to this area is increasing, because the evolution of
      its glaciers recently depicted a situation of general stability, known
      as &quot;Karakoram Anomaly&quot;, in contrast to glacier retreat
      worldwide. Here we focused our attention upon the glacier evolution
      within the Central Karakoram National Park (CKNP, a newborn park of
      this region, ca. 12 162 km&lt;sup&gt;2&lt;/sup&gt; in area) to assess the magnitude
      and rate of such anomaly. By means of Remote Sensing data (i.e.:
      Landsat images), we analyzed a sample of more than 700 glaciers, and
      we found out their area change between 2001 and 2010 is not
      significant (+27 km&lt;sup&gt;2&lt;/sup&gt; ± 42 km&lt;sup&gt;2&lt;/sup&gt;), thus
      confirming their stationarity. We analyzed climate data, snow coverage
      from MODIS, and supraglacial debris presence, as well as potential
      (con-) causes. We found a slight decrease of summer temperatures (down
      to −1.5 &amp;deg;C during 1980–2009) and an increase of wet days
      during winter (up +3.3 days yr&lt;sup&gt;&amp;minus;1&lt;/sup&gt; during 1980–2009),
      possibly increasing snow cover duration, consistently with MODIS
      data. We further detected considerable supra-glacial debris coverage
      (ca. 20% of the glacier area which rose up to 31%
      considering only the ablation area), which could have reduced buried
      ice melting during the last decade. These results provide further
      ground to uphold the existence of the Karakoram Anomaly, and present
      an useful template for assessment of water availability within the
      glaciers of the CKNP.</description><dc:date>2013-06-18T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2845/2013/"><title>Parameter and state estimation with a time-dependent adjoint marine ice sheet model</title><link>http://www.the-cryosphere-discuss.net/7/2845/2013/</link><description>&lt;b&gt;Parameter and state estimation with a time-dependent adjoint marine ice sheet model&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2845-2890, 2013&lt;br /&gt;&lt;br /&gt;Author(s): D. N. Goldberg and P. Heimbach&lt;br /&gt;&lt;br /&gt;To date, assimilation of observations into large-scale ice models has
consisted predominantly of time-independent inversions of surface
velocities for basal traction, bed elevation, or ice stiffness, and
has relied primarily on analytically-derived adjoints of diagnostic
ice velocity models. To overcome limitations of such &quot;snapshot&quot;
inversions, i.e. their inability to assimilate time-dependent data, or
to produce initial states with minimum artificial drift and suitable
for time-dependent simulations, we have developed an adjoint of
a time-dependent parallel glaciological flow model. The model
implements a hybrid shallow shelf-shallow ice stress balance, involves
a prognostic equation for ice thickness evolution, and can represent
the floating, fast-sliding, and frozen bed regimes of a marine ice
sheet. The adjoint is generated by a combination of analytic methods
and the use of algorithmic differentiation (AD) software. Several
experiments are carried out with idealized geometries and synthetic
observations, including inversion of time-dependent surface elevations
for past
thicknesses, and simultaneous retrieval of basal traction and
topography from surface data. Flexible generation of the adjoint for
a range of independent uncertain variables is exemplified through
sensitivity calculations of grounded ice volume to changes in basal
melting of floating and basal sliding of grounded ice. The results are
encouraging and suggest the feasibility, using real observations, of
improved ice sheet state estimation and comprehensive transient sensitivity assessments.</description><dc:date>2013-06-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2801/2013/"><title>Grain shape influence on light extinction in snow</title><link>http://www.the-cryosphere-discuss.net/7/2801/2013/</link><description>&lt;b&gt;Grain shape influence on light extinction in snow&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2801-2843, 2013&lt;br /&gt;&lt;br /&gt;Author(s): Q. Libois, G. Picard, J. L. France, L. Arnaud, M. Dumont, C. M. Carmagnola, and M. D. King&lt;br /&gt;&lt;br /&gt;The energy budget and the photochemistry of a snowpack greatly depend
      on the penetration of solar radiation into the snowpack. While
      representing snow by a collection of spherical particles has been
      a successful option in the numerical computation of the albedo, such
      models poorly reproduce light extinction measurements. Here, we
      explore the limits of the spherical representation by using numerical
      tools and experimental data. For this, we investigate the influence of
      grain shape on light extinction in the visible and near-infrared (NIR)
      ranges. To compute light extinction, we developed a multi-layer
      radiative transfer model based on the δ-Eddington approximation
      and analytical expressions of the albedo, α, and the asymptotic
      flux extinction coefficient (AFEC), &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;e&lt;/sub&gt;. The snowpack is
      characterized by the profiles of density, specific surface area (SSA)
      and two parameters (&lt;i&gt;B&lt;/i&gt; and &lt;i&gt;g&lt;/i&gt;&lt;sup&gt;G&lt;/sup&gt;) depending only on the
      grain shape. The aim of the paper is to estimate the values of &lt;i&gt;B&lt;/i&gt; and
      &lt;i&gt;g&lt;/i&gt;&lt;sup&gt;G&lt;/sup&gt; and to understand how they impact macroscopic optical
      properties of snow. First, the values of &lt;i&gt;B&lt;/i&gt; and &lt;i&gt;g&lt;/i&gt;&lt;sup&gt;G&lt;/sup&gt; are
      deduced from simulations with ray tracing models for a variety of
      simple geometric shapes. The results show that spherical grains
      propagate light deeper into snow than the other shapes we have
      investigated, in agreement with theoretical and experimental studies
      from the literature. Then we present an experimental method to
      retrieve &lt;i&gt;B&lt;/i&gt; for natural snow using optical measurements. Analytical
      expressions of albedo and AFEC demonstrate that &lt;i&gt;B&lt;/i&gt; can be retrieved
      from simultaneous measurements of albedo and AFEC of a snow layer, or
      similarly from vertical profiles of reflectance and light intensity in
      a snowpack. Such measurements were performed in Antarctica and in the
      Alps and led to values of &lt;i&gt;B&lt;/i&gt; between 0.8 and 2.0, which
      significantly differs from the theoretical value for spherical grains:
      &lt;i&gt;B&lt;/i&gt; = 1.25. In addition, values of &lt;i&gt;B&lt;/i&gt; were estimated from data in the
      literature. This led to a wider range of values (1.0–9.9) which may
      be partially explained by the accuracy of the data. We demonstrate
      that grain shape has a significant influence on AFEC in natural
      snow. It highlights the large variety of natural snow microstructure
      and the importance of considering grain shape for snow optics
      questions. It experimentally demonstrates that spherical grains are
      inappropriate to model light extinction in snow, an important result
      that should be considered in further studies dedicated to subsurface
      absorption of shortwave radiation and snow photochemistry.</description><dc:date>2013-06-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2761/2013/"><title>Feedbacks and mechanisms affecting the global sensitivity of glaciers to climate change</title><link>http://www.the-cryosphere-discuss.net/7/2761/2013/</link><description>&lt;b&gt;Feedbacks and mechanisms affecting the global sensitivity of glaciers to climate change&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2761-2800, 2013&lt;br /&gt;&lt;br /&gt;Author(s): B. Marzeion, A. H. Jarosch, and J. M. Gregory&lt;br /&gt;&lt;br /&gt;Mass loss by glaciers has been an important contributor to sea level
  rise in the past and is projected to contribute a substantial
  fraction of total sea level rise during the 21st century. Here, we
  use a model of the world's glaciers in order to quantify equilibrium
  sensitivities of global glacier mass to climate change, and to
  investigate the role of changes in glacier hypsometry for long term
  mass changes. We find that 21st century glacier mass loss to a~large
  degree is governed by the glaciers responding to 20th century
  climate change. This limits the influence of 21st century climate
  change on glacier mass loss, and explains why there are relatively
  small differences in glacier mass loss under greatly different
  scenarios of climate change. Because of the geographic distribution
  of glaciers, both temperature and precipitation anomalies
  experienced by glaciers are vastly stronger than on global
  average. The projected increase in precipitation partly compensates
  for the mass loss caused by warming, but this compensation is
  negligible at higher temperature anomalies since an increasing
  fraction of precipitation at the glacier sites it liquid. Loss of
  low-lying glacier area, and more importantly, eventual complete
  disappearance of glaciers, strongly limit the projected sea level
  contribution from glaciers in coming centuries. The adjustment of
  glacier hypsometry to changes in the forcing reduces the sensitivity
  of global glacier mass to changes in global mean temperature by
  a factor of two to three. This result is a second reason for the
  relatively weak dependence of glacier mass loss on future climate
  scenario, and helps explain why glacier mass loss in the first half
  of the 20th century was of the same order of magnitude as in the
  second half of the 20th century, even though the rate of warming was
  considerably smaller.</description><dc:date>2013-06-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2725/2013/"><title>Seasonal evolution of snow permeability under equi-temperature and temperature-gradient conditions</title><link>http://www.the-cryosphere-discuss.net/7/2725/2013/</link><description>&lt;b&gt;Seasonal evolution of snow permeability under equi-temperature and temperature-gradient conditions&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2725-2759, 2013&lt;br /&gt;&lt;br /&gt;Author(s): F. Domine, S. Morin, E. Brun, and M. Lafaysse&lt;br /&gt;&lt;br /&gt;The permeability &lt;i&gt;K&lt;/i&gt; of snow to air flow affects the transfer of energy, water vapor and chemical species between the snow and
  the atmosphere. Yet today little is known of the temporal evolution of snow permeability as a function of metamorphic
  regime. Furthermore, our ability to simulate snow permeability over the seasonal evolution of a snowpack has not been
  tested. Here we have measured the evolution of snow permeability in a subarctic snowpack subject to high temperature-gradient
  (TG) metamorphism. We have also measured the evolution of the same snowpack deposited over tables so that it evolved in the
  equi-temperature (ET) regime.  Permeability varies in the range 31 &amp;times; 10&lt;sup&gt;&amp;ndash;10&lt;/sup&gt; (ET regime) to 650 &amp;times; 10&lt;sup&gt;&amp;ndash;10&lt;/sup&gt;
  m&lt;sup&gt;2&lt;/sup&gt; (TG regime). Permeability increases over time in TG conditions and decreases under ET conditions. Using measurements of
  density &lt;i&gt;&amp;rho;&lt;/i&gt; and of specific surface area (SSA), from which the equivalent sphere radius &lt;i&gt;r&lt;/i&gt; is determined, we show that the
  equation linking SSA, density &lt;i&gt;&amp;rho;&lt;/i&gt; and permeability, &lt;i&gt;K&lt;/i&gt; = 3.0 &lt;i&gt;r&lt;/i&gt;&lt;sup&gt;2&lt;/sup&gt; &lt;i&gt;e&lt;/i&gt;&lt;sup&gt;(&amp;ndash;0.013 &lt;i&gt;&amp;rho;&lt;/i&gt;)&lt;/sup&gt; (with &lt;i&gt;K&lt;/i&gt; in m&lt;sup&gt;2&lt;/sup&gt;, &lt;i&gt;r&lt;/i&gt; in m and &lt;i&gt;&amp;rho;&lt;/i&gt; in kg m&lt;sup&gt;−3&lt;/sup&gt;) obtained in a previous study adequately predicts permeability values. The detailed snowpack model Crocus is used to simulate the physical properties of the TG and ET snowpacks. For the most part, all variables are well reproduced. Simulated permeabilities
  are up to a factor of two greater than measurements for depth hoar layers, which we attribute to snow microstructure, as the
  aerodynamic properties of hollow depth hoar crystals are different from those of spheres.  Finally, the large difference in
  permeabilities between ET and TG metamorphic regimes will impact atmosphere-snow energy and mass exchanges and these effects
  deserve consideration in predicting the effect of climate change on snow properties and snow-atmosphere interactions.</description><dc:date>2013-06-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2703/2013/"><title>Modeling surface response of the Greenland Ice Sheet to interglacial climate</title><link>http://www.the-cryosphere-discuss.net/7/2703/2013/</link><description>&lt;b&gt;Modeling surface response of the Greenland Ice Sheet to interglacial climate&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2703-2723, 2013&lt;br /&gt;&lt;br /&gt;Author(s): D. Rau and I. Rogozhina&lt;br /&gt;&lt;br /&gt;This study presents a~new approach to parameterizing surface mass balance
(SMB) of the Greenland Ice Sheet (GIS) under interglacial climate validated
against recent satellite observations and the results of
a high-resolution model on a regional
scale. Based on detailed analysis of the modeled
SMB, we conclude that existing parameterizations fail to
capture either spatial pattern or amplitude of the observed surface
responses of the GIS. This is due to multiple
simplifying assumptions adopted by the majority of modeling studies within
the framework of a positive degree-day
method. Modeled surface melting is found to be highly
sensitive to a choice of daily temperature standard deviation
(SD), which is generally assumed to have uniform
distribution across Greenland. The range of commonly
used SD values does not however receive support from climate datasets
available. In this region, SD
distribution is highly inhomogeneous and characterized by low values during
summer months in areas where most surface melting
occurs. Our approach is to make use of spatially
variable SD and here we show that this leads to significant improvements in
the modeled SMB over the instrumental record. Our
findings necessitate evaluating potential consequences of the simplified SMB
treatment for assessment of the history and future of glaciation on
Earth.</description><dc:date>2013-06-14T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2679/2013/"><title>A note on the water budget of temperate glaciers</title><link>http://www.the-cryosphere-discuss.net/7/2679/2013/</link><description>&lt;b&gt;A note on the water budget of temperate glaciers&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2679-2702, 2013&lt;br /&gt;&lt;br /&gt;Author(s): J. Oerlemans&lt;br /&gt;&lt;br /&gt;In this note the total dissipative melting in temperate glaciers is studied. The analysis is based
  on the notion that the dissipation is determined by the loss of potential energy, due to the
  downward motion of mass (ice, snow, meltwater and rain). A mathematical formulation of the
  dissipation is developed and applied to a simple glacier geometry. In a next step, meltwater
  production resulting from enhanced ice motion during a glacier surge is calculated. The amount of
  melt energy available follows directly from the lowering of the centre of gravity of the glacier.
&lt;br&gt;&lt;br&gt;
  To illustrate the concept, schematic calculations are presented for a number of glaciers with
  different geometric characteristics. Typical dissipative melt rates, expressed as water-layer
  depth averaged over the glacier, range from a few cm per year for smaller glaciers to half a meter
  per year for Franz-Josef Glacier, one of the most active glaciers in the world (in terms of mass
  turnover).
&lt;br&gt;&lt;br&gt;
  The total generation of meltwater during a surge is typically half a meter. For Variegated Glacier
  a value of 70 cm is found, for Kongsvegen 20 cm. These values refer to water layer
  depth averaged over the entire glacier. The melt rate depends on the &lt;i&gt;duration&lt;/i&gt; of
  the surge. It is generally an order of magnitude larger than the water production by &quot;normal&quot;
  dissipation. On the other hand, the additional basal melt rate during a surge is comparable in
  magnitude to the water input from meltwater and precipitation. This suggests that enhanced melting
  during a surge does not grossly change the total water budget of a glacier. Basal water generated
  by enhanced sliding is an important ingredient of many theories of glacier surges. It provides
  a positive feedback mechanism that actually makes the surge happen. The results found here suggest
  that this can only work if water generated by enhanced sliding is accumulating in a part of the
  glacier base where surface meltwater and rain has no or very limited access. This finding seems
  compatible with the fact that on many glaciers surges are initiated in the lower accumulation
  zone.</description><dc:date>2013-06-14T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2635/2013/"><title>A wavelet melt detection algorithm applied to enhanced resolution scatterometer data over Antarctica (2000&amp;ndash;2009)</title><link>http://www.the-cryosphere-discuss.net/7/2635/2013/</link><description>&lt;b&gt;A wavelet melt detection algorithm applied to enhanced resolution scatterometer data over Antarctica (2000&amp;ndash;2009)&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2635-2678, 2013&lt;br /&gt;&lt;br /&gt;Author(s): N. Steiner and M. Tedesco&lt;br /&gt;&lt;br /&gt;Melting is mapped over Antarctica at a high spatial resolution using a novel melt-detection algorithm based on wavelets and
  multi-scale analysis. The method is applied to Ku band (13.4 GHz) normalized backscattering measured by SeaWinds on
  QuikSCAT and spatially enhanced on a 5 km grid over the operational life of the sensor (1999–2009).  Wavelet-based
  estimates of melt spatial extent and duration are compared with those obtained by means of threshold-based detection methods,
  where melting is detected when the measured backscattering is 3 dB below the preceding winter mean value. Results from
  both methods are assessed by means of Automatic Weather Station (AWS) air surface temperature records. The yearly melting index,
  the product of melted area and melting duration, found using a fixed threshold and wavelet-based melt algorithm are found to
  have a relative difference within 7% for all years. The majority of the difference between melting records determined from
  QuikSCAT are related to short-duration backscatter changes identified as melting using the threshold methodology but not the
  wavelet-based method. Compared with AWS records both methods show a relative accuracy to within 10% based on estimated melt
  conditions using air temperatures.  Melting maps obtained with the wavelet-based approach are also compared with those obtained
  from spaceborne brightness temperatures recorded by the Special Sensor Microwave/Image (SSMI). With respect to passive microwave
  records, we find a higher degree of agreement (9% relative difference) for the melting index using the wavelet-based
  approach than threshold-based methods (11% relative difference). Additionally, linkages between melting variability and the
  Southern Annular Mode (SAM), an important large-scale climate driver for Antarctica, are suggested by the results using wavelet
  based methods that are not found using threshold-based methods.</description><dc:date>2013-06-14T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2595/2013/"><title>Comparison of automatic segmentation of full polarimetric SAR sea ice images with manually drawn ice charts</title><link>http://www.the-cryosphere-discuss.net/7/2595/2013/</link><description>&lt;b&gt;Comparison of automatic segmentation of full polarimetric SAR sea ice images with manually drawn ice charts&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2595-2634, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M.-A. N. Moen, A. P. Doulgeris, S. N. Anfinsen, A. H. H. Renner, N. Hughes, S. Gerland, and T. Eltoft&lt;br /&gt;&lt;br /&gt;In this paper we investigate the performance of an algorithm for
      automatic segmentation of full polarimetric, synthetic aperture radar
      (SAR) sea ice scenes.  The algorithm uses statistical and polarimetric
      properties of the backscattered radar signals to segment the SAR image
      into a specified number of classes. This number was determined in
      advance from visual inspection of the SAR image and by available
      in-situ measurements.  The segmentation result was then compared to
      ice charts drawn by ice service analysts. The comparison revealed big
      discrepancies between the charts of the analysts, and between the
      manual and the automatic segmentations.  In the succeeding analysis,
      the automatic segmentation chart was labeled into ice types by sea ice
      experts, and the SAR features used in the segmentation were
      interpreted in terms of physical sea ice properties.
&lt;br&gt;&lt;br&gt;
      Studies of automatic and robust estimation of the number of ice
      classes in SAR sea ice scenes will be highly relevant for future work.</description><dc:date>2013-06-13T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2567/2013/"><title>The sensitivity of flowline models of tidewater glaciers to parameter uncertainty</title><link>http://www.the-cryosphere-discuss.net/7/2567/2013/</link><description>&lt;b&gt;The sensitivity of flowline models of tidewater glaciers to parameter uncertainty&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2567-2593, 2013&lt;br /&gt;&lt;br /&gt;Author(s): E. M. Enderlin, I. M. Howat, and A. Vieli&lt;br /&gt;&lt;br /&gt;Depth-integrated (1-D) flowline models have been widely used to
  simulate fast-flowing tidewater glaciers and predict future change
  because their computational efficiency allows for continuous
  grounding line tracking, high horizontal resolution, and
  a physically-based calving criterion, which are all essential to
  realistic modeling of tidewater glaciers. As with all models, the
  values for parameters describing ice rheology and basal friction
  must be assumed and/or tuned based on observations. For prognostic
  studies, these parameters are typically tuned so that the glacier
  matches observed thickness and speeds at an initial state, to which
  a perturbation is applied. While it is well know that ice flow
  models are sensitive to these parameters, the sensitivity of
  tidewater glacier models has not been systematically
  investigated. Here we investigate the sensitivity of such flowline
  models of outlet glacier dynamics to uncertainty in three key
  parameters that influence a glacier's resistive stress
  components. We find that, within typical observational uncertainty,
  similar initial (i.e. steady-state) glacier configurations can be
  produced with substantially different combinations of parameter
  values, leading to differing transient responses after
  a perturbation is applied. In cases where the glacier is initially
  grounded near flotation across a basal overdeepening, as typically
  observed for rapidly changing glaciers, these differences can be
  dramatic owing to the threshold of stability imposed by the
  flotation criterion. The simulated transient response is
  particularly sensitive to the parameterization of ice rheology:
  differences in ice temperature of &amp;sim; 2 &amp;deg;C can determine
  whether the glaciers thin to flotation and retreat unstably or
  remain grounded on a marine shoal. Due the highly non-linear
  dependence of tidewater glaciers on model parameters, we recommend
  that their predictions are accompanied by sensitivity tests that
  take parameter uncertainty into account.</description><dc:date>2013-06-13T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2533/2013/"><title>Impact of physical properties and accumulation rate on pore  close-off in layered firn</title><link>http://www.the-cryosphere-discuss.net/7/2533/2013/</link><description>&lt;b&gt;Impact of physical properties and accumulation rate on pore  close-off in layered firn&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2533-2566, 2013&lt;br /&gt;&lt;br /&gt;Author(s): S. A. Gregory, M. R. Albert, and I. Baker&lt;br /&gt;&lt;br /&gt;Investigations into the physical characteristics of deep firn near the
lock-in zone through pore close-off are needed to improve understanding of
ice core records of past atmospheric concentrations. Specifically, the
permeability and microstructure profiles of the firn through the diffusive
column influence the entrapment of air into bubbles and thus the ice age-gas
age difference. The purpose of this study is to examine the nature of pore
closure processes at two polar sites with very different local temperatures
and accumulation rates. Density, permeability, and microstructure
measurements were made on firn cores from WAIS Divide in West Antarctica and
Megadunes in East Antarctica. We found that the open pore structure plays a
more important role than density in predicting gas transport properties,
through the porous firn matrix. For both WAIS Divide and Megadunes, fine
grained layers experience close-off shallower in the firn column than do
coarse grained layers, regardless of which grain sized layer is the more
dense layer at depth. Pore close-off occurs at an open porosity that is
accumulation rate dependent. Low accumulation sites, with coarse grains,
close-off at lower open porosities (&lt; 10%) than the open porosity
(&gt; 10%) of high accumulation sites with finer grains. The
depth and length of the lock-in zone is primarily dependent upon
accumulation rate and microstructural variability due to differences in
grain size and pore structure, rather than the density variability of the
layers.</description><dc:date>2013-06-13T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2489/2013/"><title>Decadal changes from a multi-temporal glacier inventory of Svalbard</title><link>http://www.the-cryosphere-discuss.net/7/2489/2013/</link><description>&lt;b&gt;Decadal changes from a multi-temporal glacier inventory of Svalbard&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2489-2532, 2013&lt;br /&gt;&lt;br /&gt;Author(s): C. Nuth, J. Kohler, M. König, A. von Deschwanden, J. O. Hagen, A. K&amp;auml;&amp;auml;b, G. Moholdt, and R. Pettersson&lt;br /&gt;&lt;br /&gt;We present a multi-temporal digital inventory of Svalbard glaciers
      with the most recent from the late 2000s containing
      33 775 km&lt;sup&gt;2&lt;/sup&gt; of glaciers, or 57% of the total land
      area of the archipelago. At present, 68% of the glaciated
      area of Svalbard drains through tidewater glaciers that have a summed
      terminus width of ~ 740 km. The glaciated area over the
      entire archipelago has decreased by an average of
      80 km&lt;sup&gt;2&lt;/sup&gt; a&lt;sup&gt;&amp;minus;1&lt;/sup&gt; over the past ~ 30 yr,
      representing a reduction of 7%. For a sample of
      ~ 400 glaciers (10 000 km&lt;sup&gt;2&lt;/sup&gt;) in the south and west of
      Spitsbergen, three digital inventories are available from 1930/60s,
      1990 and 2007 from which we calculate average changes during
      2 epochs. In the more recent epoch, the terminus retreat was larger
      than in the earlier epoch while area shrinkage was smaller. The
      contrasting pattern may be explained by the decreased lateral wastage
      of the glacier tongues. Temporal retreat rates for individual glaciers
      show a mix of accelerating and decelerating trends, reflecting the
      large spatial variability of glacier types and climatic/dynamic
      response times in Svalbard. Last, retreat rates estimated by dividing
      glacier area changes by the tongue width are larger than centerline
      retreat due to a more encompassing frontal change estimate with
      inclusion of lateral area loss.</description><dc:date>2013-06-10T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2455/2013/"><title>The physical basis for gas transport through polar firn: a case study at Summit, Greenland</title><link>http://www.the-cryosphere-discuss.net/7/2455/2013/</link><description>&lt;b&gt;The physical basis for gas transport through polar firn: a case study at Summit, Greenland&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2455-2487, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. C. Adolph and M. R. Albert&lt;br /&gt;&lt;br /&gt;Compared to other natural porous materials, relatively little is known about the physical nature
  of polar firn.  This intricate network of ice and pore space that comprises the top
  60–100 m of the polar ice sheets is the framework that forms the natural archive of past
  climate information.  Despite the many implications for ice core interpretation, direct
  measurements of physical properties throughout the firn column are limited.  Models of gas
  transport through firn are used to interpret in-situ chemical data which is retrieved to analyze
  past atmospheric composition. These traditional models treat the firn as a &quot;black box,&quot; with gas
  transport parameters tuned to match gas concentrations with depth to known atmospheric
  histories. Though this method has been largely successful and provided very useful insights, there
  are still many questions and uncertainties to be addressed.  This work seeks to understand the
  impact of firn structure on gas transport in firn from a first principles standpoint through
  direct measurements of permeability, gas diffusivity and microstructure. The relationships between
  gas transport properties and microstructure will be characterized and compared to existing
  relationships for general porous media. Direct measurements of gas diffusivity are compared to
  diffusivities deduced from models based on firn air chemical sampling. Our comparison illuminates
  the primary importance of including microstructural parameters, beyond just porosity or density,
  in mass transport modeling, and it provides insights about the nature of gas transport throughout
  the firn column. Guidance is provided for development of next-generation firn air transport
  models.</description><dc:date>2013-06-07T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2413/2013/"><title>Spatial debris-cover effect on the maritime glaciers of Mount Gongga, south-eastern Tibetan Plateau</title><link>http://www.the-cryosphere-discuss.net/7/2413/2013/</link><description>&lt;b&gt;Spatial debris-cover effect on the maritime glaciers of Mount Gongga, south-eastern Tibetan Plateau&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2413-2453, 2013&lt;br /&gt;&lt;br /&gt;Author(s): Y. Zhang, Y. Hirabayashi, K. Fujita, S. Liu, and Q. Liu&lt;br /&gt;&lt;br /&gt;The Tibetan Plateau and surroundings contain a large number of
  debris-covered glaciers, on which debris cover affects glacier
  response to climate change by altering ice melting rates and spatial
  patterns of mass loss.  Insufficient spatial distribution of debris
  thickness data makes it difficult to analyze regional debris-cover
  effects. Mount Gongga glaciers, maritime glaciers in the
  south-eastern Tibetan Plateau, are characterized by a substantial
  reduction in glacier length and ice mass in recent decades. Advanced
  Spaceborne Thermal Emission and Reflection Radiometer
  (ASTER)-derived thermal property of the debris layer reveals that
  68% of the glaciers have extensive mantles of supraglacial
  debris in their ablation zones, in which the proportion of debris
  cover to total glacier area varies from 1.74% to
  53.0%. Using a surface energy-mass balance model accounting for
  the debris-cover effect applied at a regional scale, we find that
  although the presence of supraglacial debris has a significant
  insulating effect on heavily debris-covered glaciers, it accelerates
  ice melting on ~ 10.2% of the total ablation area and
  produces rapid wastage of ~ 25% of the debris-covered
  glaciers, resulting in the similar mass losses between
  debris-covered and debris-free glaciers. Widespread debris cover
  also facilitates the development of active terminus
  regions. Regional differences in the debris-cover effect are
  apparent, highlighting the importance of debris cover for
  understanding glacier status and hydrology in both the Tibetan
  Plateau and other mountain ranges around the world.</description><dc:date>2013-06-06T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2373/2013/"><title>Solving Richards Equation for snow improves snowpack meltwater runoff estimations</title><link>http://www.the-cryosphere-discuss.net/7/2373/2013/</link><description>&lt;b&gt;Solving Richards Equation for snow improves snowpack meltwater runoff estimations&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2373-2412, 2013&lt;br /&gt;&lt;br /&gt;Author(s): N. Wever, C. Fierz, C. Mitterer, H. Hirashima, and M. Lehning&lt;br /&gt;&lt;br /&gt;The runoff from the snow cover during spring snow melt or
  rain-on-snow events is an important factor in the hydrological
  cycle. In this study, water transport schemes for a 1-dimensional
  physical based snowpack model are compared to 14 yr of
  lysimeter measurements at a high alpine site. The schemes include
  a simple bucket-type approach, an approximation of Richards Equation
  (RE), and the full RE. The results show that daily sums of runoff
  are strongly related to a positive energy balance of the snow cover
  and therefore, all water transport schemes show very similar
  performance in terms of Nash–Sutcliffe efficiency (NSE) coefficients
  (around 0.59) and &lt;i&gt;r&lt;/i&gt;&lt;sup&gt;2&lt;/sup&gt; values (around 0.77). Timing of the
  arrival of meltwater in spring at the bottom of the snowpack showed
  differences between the schemes, where especially in the bucket-type
  and approximated RE approach, meltwater release is slower than in
  the measurements. Overall, solving RE for the snow cover yields the
  best agreement between modelled and measured runoff. On sub-daily
  time scales, the water transport schemes behave very
  differently. Also here, solving RE provides the highest agreement
  between modelled and measured runoff in terms of NSE coefficient
  (0.48), where other water transport schemes loose any predictive
  power. This appears to be mainly due to bad timing of meltwater
  release during the day. Accordingly, solving RE for the snow cover
  improves several aspects of modelling snow cover runoff. The
  additional computational cost was found to be in the order of
  a factor of 1.5.</description><dc:date>2013-06-05T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2333/2013/"><title>Evaluation of the snow regime in dynamic vegetation land surface models using field measurements</title><link>http://www.the-cryosphere-discuss.net/7/2333/2013/</link><description>&lt;b&gt;Evaluation of the snow regime in dynamic vegetation land surface models using field measurements&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2333-2372, 2013&lt;br /&gt;&lt;br /&gt;Author(s): E. Kantzas, M. Lomas, S. Quegan, and E. Zakharova&lt;br /&gt;&lt;br /&gt;An increasing number of studies have demonstrated the significant
  climatic and ecological changes occurring in the northern latitudes
  over the past decades. As coupled, earth-system models attempt to
  describe and simulate the dynamics and complex feedbacks of the
  Arctic environment, it is important to reduce their uncertainties in
  short-term predictions by improving the description of both the
  systems processes and its initial state. This study focuses on
  snow-related variables and extensively utilizes a historical data
  set (1966–1996) of field snow measurements acquired across the
  extend of the Former Soviet Union (FSU) to evaluate a range of
  simulated snow metrics produced by a variety of land surface models,
  most of them embedded in IPCC-standard climate models. We reveal
  model-specific issues in simulating snow dynamics such as magnitude
  and timings of SWE as well as evolution of snow density. We further
  employ the field snow measurements alongside novel and
  model-independent methodologies to extract for the first time (i)
  a fresh snow density value (57–117 kg m&lt;sup&gt;&amp;ndash;3&lt;/sup&gt;) for the
  region and (ii) mean monthly snowpack sublimation estimates across
  a grassland-dominated western (November–February) [9.2, 6.1, 9.15,
  15.25] mm and forested eastern sub-sector (November–March) [1.53,
  1.52, 3.05, 3.80, 12.20] mm; we subsequently use the retrieved
  values to assess relevant model outputs. The discussion session
  consists of two parts. The first describes a sensitivity study where
  field data of snow depth and snow density are forced directly into
  the surface heat exchange formulation of a land surface model to
  evaluate how inaccuracies in simulating snow metrics affect
  important modeled variables and carbon fluxes such as soil
  temperature, thaw depth and soil carbon decomposition. The second
  part showcases how the field data can be assimilated with
  ready-available optimization techniques to pinpoint model issues and
  improve their performance.</description><dc:date>2013-06-05T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2293/2013/"><title>An upper-bound estimate for the accuracy of volume-area scaling</title><link>http://www.the-cryosphere-discuss.net/7/2293/2013/</link><description>&lt;b&gt;An upper-bound estimate for the accuracy of volume-area scaling&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2293-2331, 2013&lt;br /&gt;&lt;br /&gt;Author(s): D. Farinotti and M. Huss&lt;br /&gt;&lt;br /&gt;Volume-area scaling is the most popular method for estimating the ice
 volume of large glacier samples. Here, a series of resampling
 experiments based on different sets of synthetic data are presented
 in order to derive an upper-bound estimate (i.e. a level
 achieved only with ideal conditions) for the accuracy of its
 application. We also quantify the maximum accuracy expected when
 scaling is used for determining the glacier volume change, and area
 change of a given glacier population. A comprehensive set of measured
 glacier areas, volumes, area and volume changes is evaluated to
 investigate the impact of real-world data quality on the so assessed
 accuracies. For populations larger than a few thousand glaciers, the
 total ice volume can be recovered within 30% if all measurements
 available worldwide are used for estimating the scaling
 coefficients. Assuming no systematic biases in ice volume
 measurements, their uncertainty is of secondary importance. Knowing
 the individual areas of a glacier sample for two points in time
 allows recovering the corresponding ice volume change within 40%
 for populations larger than a few hundred glaciers, both for
 steady-state and transient geometries. If ice volume changes can be
 estimated without bias, glacier area changes derived from volume-area
 scaling show similar uncertainties as for the volume changes. This
 paper does not aim at making a final judgement about the suitability
 of volume-area scaling, but provides the means for assessing the
 accuracy expected from its application.</description><dc:date>2013-06-05T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2247/2013/"><title>Changes in glacier Equilibrium-Line Altitude (ELA) in the western Alps over the 1984–2010 period: evaluation by remote sensing and modeling of the morpho-topographic and climate controls</title><link>http://www.the-cryosphere-discuss.net/7/2247/2013/</link><description>&lt;b&gt;Changes in glacier Equilibrium-Line Altitude (ELA) in the western Alps over the 1984–2010 period: evaluation by remote sensing and modeling of the morpho-topographic and climate controls&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2247-2291, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. Rabatel, A. Letréguilly, J.-P. Dedieu, and N. Eckert&lt;br /&gt;&lt;br /&gt;We present time series of equilibrium-line altitude (ELA) measured
  from the end-of-summer snowline altitude computed using satellite
  images, for 43 glaciers in the western Alps over the 1984–2010
  period. More than 120 satellite images acquired by Landsat, SPOT and
  ASTER were used.  In parallel, changes in climate parameters (summer
  cumulative positive degree days, CPDD, and winter precipitation)
  were analyzed over the same time period using 22 weather stations
  located inside and around the study area. Assuming a continuous
  linear trend over the study period: (1) the average ELA of the 43
  glaciers increased by about 170 m; (2) summer CPDD increased
  by about 150 PDD at 3000 m a.s.l.; and (3) winter
  precipitation remained rather stationary.  Summer CPDD showed
  homogeneous spatial and temporal variability; winter precipitation
  showed homogeneous temporal variability, but some stations showed
  a slightly different spatial pattern. Regarding ELAs, temporal
  variability between the 43 glaciers was also homogeneous, but
  spatially, glaciers in the southern part of the study area differed
  from glaciers in the northern part, mainly due to a different
  precipitation pattern. A sensitivity analysis of the ELAs to climate
  and morpho-topographic parameters (elevation, aspect, latitude)
  highlighted the following: (1) the average ELA over the study period
  of each glacier is strongly controlled by morpho-topographic
  parameters; and (2) the interannual variability of the ELA is
  strongly controlled by climate parameters, with the observed
  increasing trend mainly driven by increasing temperatures, even if
  significant nonlinear low frequency fluctuations appear to be driven
  by winter precipitation anomalies.  Finally, we used an expansion of
  Lliboutry's approach to reconstruct fluctuations in the ELA of any
  glacier of the study area with respect to morpho-topographic and
  climate parameters, by quantifying their respective weight and the
  related uncertainties in a consistent manner within a hierarchical
  Bayesian framework. This method was tested and validated using the
  ELA measured on the satellite images.</description><dc:date>2013-06-03T00:00:00+02:00</dc:date></item><item rdf:about="http://www.the-cryosphere-discuss.net/7/2191/2013/"><title>Simulation of wind-induced snow transport in alpine terrain using a fully coupled snowpack/atmosphere model</title><link>http://www.the-cryosphere-discuss.net/7/2191/2013/</link><description>&lt;b&gt;Simulation of wind-induced snow transport in alpine terrain using a fully coupled snowpack/atmosphere model&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;The Cryosphere Discussions, 7, 2191-2245, 2013&lt;br /&gt;&lt;br /&gt;Author(s): V. Vionnet, E. Martin, V. Masson, G. Guyomarc'h, F. Naaim-Bouvet, A. Prokop, Y. Durand, and C. Lac&lt;br /&gt;&lt;br /&gt;In alpine regions, wind-induced snow transport strongly influences the
      spatio-temporal evolution of the snow cover throughout the winter
      season. To gain understanding on the complex processes that drive the
      redistribution of snow, a new numerical model is developed. It couples
      directly the detailed snowpack model Crocus with the atmospheric model
      Meso-NH. Meso-NH/Crocus simulates snow transport in saltation and in
      turbulent suspension and includes the sublimation of suspended snow
      particles. A detailed representation of the first meters of the
      atmosphere allows a fine reproduction of the erosion and deposition
      process. The coupled model is evaluated against data collected around
      the experimental site of Col du Lac Blanc (2720 m a.s.l.,
      French Alps). For this purpose, a blowing snow event without
      concurrent snowfall has been selected and simulated. Results show that
      the model captures the main structures of atmospheric flow in alpine
      terrain, the vertical profile of wind speed and the snow particles
      fluxes near the surface. However, the horizontal resolution of
      50 m is found to be insufficient to simulate the location of
      areas of snow erosion and deposition observed by terrestrial laser
      scanning.  When activated, the sublimation of suspended snow particles
      causes a reduction in deposition of 5.3%. Total sublimation
      (surface + blowing snow) is three times higher than surface
      sublimation in a simulation neglecting blowing snow sublimation.</description><dc:date>2013-06-03T00:00:00+02:00</dc:date></item></rdf:RDF>