We present a new method for estimating ice mass loss from glaciers and ice sheets using Interferometric Synthetic Aperture Radar (InSAR) time-series data. We use a linear inversion method based on observations of nearby bedrock uplift and a solution for surface loading of an elastic half-space. The method assumes that mass loss is focused on lower elevation terminal regions of the glacier or ice sheet, and that there is an exponential decrease in thinning rate toward the higher elevation interior. We apply the method to uplift rates between 1995 and 2009 near Vatnajökull, Iceland. The data reveal up to 13 mm/yr relative line-of-sight (LOS) velocity around the south-western edge of Vatnajökull. We find an ice mass loss rate of Gt/yr, in approximate agreement with other estimates. Ice loss since 1995 is twice as fast as the loss rate estimated for the rest of the 20th century.
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 The mass balance of ice sheets, ice caps, and glaciers is one expression of global climate change. Many recent studies suggest rapid acceleration of cryosphere melting since the late 1990s [Khan et al., 2007, 2010; Howat et al., 2008; Wouters et al., 2008; Chen et al., 2009; Jiang et al., 2010; Sørensen et al., 2011; Ewert et al., 2011; Shepherd et al., 2012; Lenaerts et al., 2013; Yang et al., 2013]. Ice loss currently contributes 0.7–1.8 mm/yr to present-day global sea level rise [Meier et al., 2007; Gardner et al., 2013] and this is likely to increase in the future.
 Space geodetic techniques commonly used to estimate ice mass balance include the Gravity Recovery and Climate Experiment (GRACE) [Velicogna and Wahr, 2006; Chen et al., 2006; Ramillien et al., 2006; Wouters et al., 2008; Slobbe et al., 2009] and laser and radar altimetry [Howat et al., 2008; Pritchard et al., 2009; Sørensen et al., 2011]. These techniques typically have limited spatial resolution. InSAR and speckle tracking can be used to measure ice flow velocities and their temporal changes [Joughin, 2002; Rignot et al., 2011b, 2013] from which, combined with ice thickness data and regional models, changes in mass balance can be inferred [Rignot et al., 2008; Osmanoğlu et al., 2013]. The main challenge of InSAR-based ice flow measurements is poor temporal resolution (sampling intervals of several weeks), although this recently was improved with the launch of TerraSAR-X [Joughin et al., 2011]. InSAR and GPS have also been used to directly measure uplift at the edge of glaciers [Jiang et al., 2010; Bevis et al., 2012; Liu et al., 2012; Auriac et al., 2013; Yang et al., 2013], from which mass balance can be inferred, as described below.
 The mass loss of a glacier results in uplift of nearby crust, due to isostasy and local deformation, a process known as glacial isostatic adjustment (GIA). Hence, uplift measurements can constrain mass balance [e.g., Jiang et al., 2010]. However, these methods have two limitations. First, they require independent information (or assumptions) on load distribution in areas where no geodetic observations are available, for example assuming a homogenous unloading slab [Jiang et al., 2010]. Second, the observed ground deformation consists of both an instantaneous elastic and a delayed viscous component (Figure 1) [e.g., Peltier, 1974; Wu, 1992; Mitrovica et al., 2001]. The elastic deformation can be assumed to represent contemporaneous uplift in response to current melting. The viscous deformation may have two components, a long delayed component due to melting of ice sheets from Earth's last glacial maximum, approximately 20,000 years ago, and a more recent component in response to the early phases of the current melting period. For example, in Iceland, the current melting period started at the end of the Little Ice Age at ∼1890 AD [Sigmundsson, 1991]. This is long enough before present that viscous response of the lower crust and upper mantle might contribute to the contemporary surface deformation field. The viscous component has a long-wavelength signal (spatial extent larger than 40 km) because it occurs in response to flow in the mantle (mainly below 40 km). The interpretation of ground deformation in terms of mass balance requires separation of these various spatial and temporal components [Jiang et al., 2010; Bevis et al., 2012].
 This paper presents a new approach for mass balance estimation from geodetic observations (Figure 1). We use InSAR, which measures relative displacements across a SAR scene and is sensitive to local deformation differences. Since ice melting occurs primarily at lower elevations near the ice edge, the short wavelength contemporaneous deformation (spatial extent a few tens of kilometers or less), is resolvable with InSAR and is dominated by the contemporary elastic component of deformation.
 The Icelandic ice caps were the 7th largest contributor to global sea level rise between 2003 and 2010 [Jacob et al., 2012]. Vatnajökull is the largest ice cap in Iceland, with a mean elevation of 1215 m and a maximum ice thickness of 950 m [Björnsson and Pálsson, 2008]. The other three big Icelandic ice caps, Hofsjökull, Mýrdalsjökull, and Langjökull, are located further west (Figure 2). The western part of Vatnajökull is underlain by the mid-Atlantic-ridge, which spreads at a half rate of about 1 cm/yr [LaFemina et al., 2005; Jónsson, 2008], and by the Icelandic hot spot, coincident with the ridge. GIA following the last deglaciation ended at ∼9000 BP [Sigmundsson, 1991], reflecting the thermal influence of the spreading ridge and hot spot, and the corresponding low viscosity of the Icelandic upper mantle. Vatnajökull started its most recent retreat at the end of the little ice age, ∼1890 [Sigmundsson, 1991], when its surface area was ∼8600 km2 [Björnsson and Pálsson, 2008]. From 1890 to 2003, Vatnajökull lost 435 km3 ice. Its surface area in 2007 was ∼8100 km2 [Pagli et al., 2007a, Árnadóttir et al., 2009]. The corresponding average thinning rate since 1890 is 0.5 m/yr (Table 1). Vatnajökull's ice loss and accumulation has varied in time, e.g., there was net growth from 1991 to 1994 [Björnsson and Pálsson, 2008]. The ice loss from 1994 to 2005 was 84 km3, corresponding to an average thinning rate of 0.84 m/yr [Björnsson and Pálsson, 2008], almost half of the maximum rate following the last glacial maximum [2 m/yr; Pagli and Sigmundsson, 2008].
Table 1. Ice Mass Loss Rates of the Vatnajökull Ice Cap and Whole Iceland
Ice Loss Rate(Gt/yr)
Volume Loss (km3)
Average Thinning Rate (m/yr)
Parameter given in reference.
Calculated from total thinning of 9.2 m water equivalent thickness.
Calculated from the mass loss rate. Other parameters are calculated using an ice density of 917 kg/m3 and a surface area of Vatnajökull of 8100 km2 (post-1990).
 In this section, we have reported average ice thinning rates. In the following sections, we consider spatially varying thinning rates following an exponential model, except for special cases of uniform thinning, when we quote the results of Grapenthin et al. , and in Table 1, where we have converted the estimated mass loss rate into an average thinning rate. Throughout this paper ice thinning stands for ice elevation change.
3. Ice Mass Loss Rate Estimation From InSAR Observations
 Crustal uplift due to ice melting is a surface unloading problem, similar to loading the crust by water level changes in artificial or natural lakes [Kaufmann and Amelung, 2000; Cavalie et al., 2007; Nof et al., 2012]. We use the solution for the surface displacement of an elastic half space due to a point source with a unit mass in cylindrical coordinates assuming axial symmetry [Sneddon, 1951; Pinel et al., 2007]:
where V and U are the vertical and radial displacements, g is the gravitational acceleration, υ is the Poisson's ratio, E is the Young's modulus, and r is the distance from the point source. We assume that the load change (mass loss rate) is constant with time and use velocities instead of displacements. In the following, we formulate a linear inverse problem to estimate the load change from surface velocities.
 Glaciers and ice sheets generally melt from the edge toward the interior [Sigmundsson and Einarsson, 1992; Marshall et al., 2005]. We assume that the mass loss rate decreases exponentially with distance from the ice edge and describe it using the thinning rate h(x),
where k is the decay distance (the distance where the thinning rate reduces to 1/e of the rate at the edge), x is the distance from the ice edge, c is the thinning rate at the inland portion of a glacier (x >> k), and a is the thinning rate at the ice edge (x = 0). The units of h, a, and c are m/yr (positive for thinning), and k is in meters. Ice accumulation far from the ice edge is represented by negative c. We can expand this one-dimensional model to a two-dimensional model by dividing the load change into a series of square blocks, calculating the displacement rate due to point loads with the corresponding masses for each block, and superposing the solutions for all blocks. The ground velocities for such a model are calculated as
where superscripts v, e, n represent vertical, east, and north directions, xi is the distance of an ice block to the ice edge, i = 1,…, N with N the number of blocks, δ is the block spacing, ρ is the density of ice, and rli the distance between the point load representing block i and observation point l = 1,…, L with L the number of observations.
 The ground velocity is linear with respect to parameters a and c and nonlinear with respect to k. InSAR measures velocities in the radar line-of-sight direction (LOS). For a given k, we have a linear system,
where is the L × 1 vector of observations (LOS velocities) and the 2 × 1 vector of model parameters. We use the least-squares solution
with A−g the generalized inverse. The model variance is given by [Snieder and Trampert, 1999]
where is the model standard error of the ith ice block, is the standard error of lth velocity field. The design matrix A can be written as
where A is a L × 2 matrix, and each line represents the mapping relationship between independent variables and observation at location l. The lth line of A represents the mapping from mass loss rate to the lth absolute velocity field. By subtracting the line representing the reference point from each line, A is then a relative mapping matrix. The dot operator represents matrix elementary multiplication, and the cross operator represents matrix multiplication.
 where B and C are 2 L × 3N matrices, in which the first N columns correspond to vertical component, the second N columns correspond to east component, and the third N columns correspond to north component. B contains the mapping parameters from three-dimensional velocities to LOS direction. C is generated from equations (4) and (5). θ is the look angle of the radar beam and α is the azimuth angle representing the flight direction. D is a 3N × 2 matrix for parameters describing the exponential unloading model.
 We establish a series of linear inversions by searching each possible value of k with reasonable stepping (5000 m). For a given k, we thus solve for a and c. Although the inversion problem is overdetermined, the sensitivity of the data for predicting the model varies spatially. In the far field (far from the ice edge), the data resolutions [Menke, 1989] are very poor. Low data resolution can bias the model predictions [Lohman and Simons, 2005; Xia et al., 2008]. We thus use a weighting approach according to the diagonal values of the data resolution matrix w = (diag(N))p, where w is the weighting vector, N is the data resolution matrix, diag() represents the process of retrieving the diagonal vector of N, and p is a amplification factor. We use p = 2 for this study.
 The estimated mass loss rate thus should depend on k. In practice, we find that although a and c are sensitive to k, the estimated mass loss rate is not (see section 'Ice Mass Loss Rate Estimation'). We conclude that the proposed approach allows a reliable estimation for glaciers and ice sheets with exponential thinning from edge to interior.
4. InSAR Data
 We use 1995–2009 C-band ERS imagery and the Small Baseline InSAR time-series method [Berardino et al., 2002; Fattahi and Amelung, 2013] for measuring the contemporaneous deformation around Vatnajökull. In Iceland, only summer acquisitions (late June to early October) are suitable for InSAR because of snow cover during other seasons; the typical temporal density is three images per year for each track. We combine the SAR acquisitions to form interferogram networks using thresholds in perpendicular spatial baseline of 300 m and temporal baseline of 3 years, supplemented by a few longer temporal or spatial baseline interferograms to ensure full network connection (110 and 43 interferograms on descending and ascending tracks, see supporting information1 Figure 1). We estimate ground velocity assuming linear deformation (neglecting seasonal effects although they are known to be significant) [Grapenthin et al., 2006]. We eliminate long-wavelength phase contributions (the signal across the two SAR frames) by removing quadratic surfaces in range and azimuth directions, estimated at each epoch of the InSAR time-series after masking out the deforming areas near the ice edge. The long-wavelength phase contributions are due to plate motion [LaFemina et al., 2006; Geirsson et al., 2012], viscous deformation, and possibly orbital uncertainties [Gourmelen et al., 2010]. The effect of stratified atmospheric delays is small because of limited topographic relief in the study area. InSAR measurements, in particular at high latitudes, can be affected by ionospheric disturbances but this effect is generally small for C-band data [Meyer, 2011].
 Figures 2a and 2b show the 1995–2009 relative LOS velocities for the descending and ascending tracks. The InSAR measurements are relative to a reference point, which is a point near GPS station 7485 of Árnadóttir et al. . Although the relative velocities could be transferred into absolute velocities using the motion of this station, it is not needed, because our modeling approach uses relative velocities only.
 Figure 2 shows a 5–10 km wide yellow-red band around the southwestern edge of Vatnajökull, corresponding to relative LOS velocities up to 13 mm/yr and a large area of uplift west of the ice cap. The standard error of the LOS velocity fields are ∼0.4 mm/yr and ∼0.7 mm/yr for the descending and ascending tracks, respectively, estimated following Gourmelen et al.  in an 18 × 18 km2 nondeforming area (marked by the rectangle in Figures 2a and 2b). The displacement histories shown for two points near the ice edge suggest almost constant LOS annual velocity during the observation period (Figures 2c and 2d). Deviations up to 3 cm are most likely due to atmospheric effects and seasonal loading variations. The spatial extent of uplift is clearly represented in a map of vertical velocity (Figure 3), obtained by combining the descending and ascending LOS velocities vertical and horizontal velocities. The vertical ground velocity from InSAR is consistent with the relative changes in GPS velocities of Arnadottir et al.  (the root-mean-square deviation is 2.1 mm/yr, see supporting information Figure 2).
5. Ice Mass Loss Rate Estimation
 We estimate the ice mass loss rate using equation (7) for thinning rate models with different decay distances k. To build matrices B and C, we represent the load change (the change of ice mass) by a series of 1.4 km2 square blocks, each of which is approximated by a point load. We do not consider changes in surface area because the associated mass change is small. We select an area not influenced by recent volcanic activity southwest of Vatnajökull (the rectangle in Figure 4, surface area ∼2500 km2) and sample the velocity fields using a uniform grid to obtain a data vector consisting of 478 descending and 454 ascending LOS velocities. The fit of a model to the data is described by the Root Mean Square Error, , with dl is the observations, pl is the model predictions, and L is the number of observations. We assume unit variance for all data points.
 We first test an unrealistic spatially uniform thinning rate model (k→∞ in equation (3)). The solution suggests an ice mass loss rate of 20.8 Gt/yr (corresponding to an average thinning rate of 2.8 m/yr), significantly higher than previous mass loss rate estimates (Table 1). This model is characterized by an RMSE of 4.3 mm/yr, suggesting a relatively poor fit to the observations, and suggesting that a spatially uniform thinning rate model is not appropriate.
 We next consider exponential thinning rate models. We conduct a grid search over the decay distance k, and estimate for each k the parameters a and c using equation (6), varying k from 1 to 30 km with a step size of 0.5 km. The estimated mass loss rate depending on k is 6.8–7.3 Gt/yr (Figure 5). This narrow range of 0.5 Gt/yr suggests that variations in k are largely compensated by variations of a and c. We also found that RMSE does not vary significantly with k, i.e., the data are not sufficient to resolve k. Björnsson and Pálsson  present a thinning rate model that can approximated by an exponential model with k = 7.5 km, a = 5.5 m/yr, and c = −1.6 m/yr (Figure 6). We thus use k = 7.5 km and invert for a and c. We find a = 3.75 m/yr and c = −0.75 m/yr, similar to values calculated by Björnsson and Pálsson .
 Including the observation error, the estimated range of mass loss rate is Gt/yr. Adding the uncertainties associated with bounds in Young's modulus (40 ± 15 GPa) [Grapenthin et al., 2006], the estimated mass loss rate is Gt/yr.
 Figure 4 shows the comparison between the model with k = 7.5 km and the observations. In the area southwest of Vatnajökull, the model predictions closely resemble the observations (Figures 4c and 4f). Some areas with high residuals are addressed below (section 6.1).
 For the Hofsjökull (surface area 925 km2) and Mýrdalsjökull (600 km2) ice caps we also use exponential thinning rate models, invert for the mass loss rate and obtain rates of 0.9 and 1.7 Gt/yr, respectively. The estimate for Hofsjökull is close to that of Grapenthin et al.  (their average thinning rate of 1 m/yr for 1996–2001 corresponds to a mass loss rate of 0.85 Gt/yr), but not the estimate for Mýrdalsjökull. Grapenthin et al.  report an average thinning rate of 0.5 m/yr which corresponds to a mass loss rate of 0.3 Gt/yr. The estimates of the smaller ice caps are not well constrained because of the depth variation of Young's modulus (see section 'Young's Modulus'). For Langjökull (950 km2), we use the average thinning rate of 1.3 m/yr of Grapenthin et al. , which corresponds to a mass loss rate of 0.9 Gt/yr, 1996–2004.
6.1. Model Fit
 Here we investigate discrepancies between our model predictions and observations. First, there is a lack of observed uplift at the northwestern edge of Vatnajökull. This is an area of highest topographic elevation where melting is slow because of low air temperature [Björnsson and Pálsson, 2008]. This is not represented by our simple thinning rate model. This area was also subjected to subsidence following the 1996 eruption of Gjalp subglacial volcano [Pagli et al., 2007b]. Discrepancies near the Hofsjökull and Myrdalsjökull ice caps are also likely due to simplification of the assumed thinning rate model. For these small ice caps, the exponential model may not fit very well because of the large contribution of outlet glaciers. Third, there is an excess uplift (Figure 4) west of Vatnajökull, also noted by Árnadóttir et al. . This area is located above and west of the spreading center. A possible explanation for excess uplift here is viscoelastic deformation related to a locally low effective elastic layer thickness. The data from these areas are not included in the modeling and do not affect the estimated ice mass loss rate.
6.2. Effect of Viscoelastic Behavior
 Our approach to mass loss estimation is based on the assumption that the observed relative uplift can be explained by rebound of a homogeneous elastic half-space. However, GIA has both elastic and viscous components due to viscous flow in the upper mantle and possibly in the lower crust. Modeling of GPS observations suggest that Icelandic lithosphere has a high viscosity lower crust and a low viscosity upper mantle, with average viscosities of >1021 Pa·s and 1019 Pa·s, respectively, and a crustal thickness of 40 km [e.g., Árnadóttir et al., 2009]. Auriac et al.  show that this rheological structure holds for the larger Vatnajökull area. However, spatial variations in rheology are likely. Iceland is located on a mid-ocean ridge and a hot spot. The lower crust and upper mantle can be thermally weakened depending on location [e.g., Barnhoorn et al., 2011]. For the ridge area in southwestern Iceland, Jónsson  finds lower crustal and upper mantle viscosities of 1019 Pa s and 3–4 × 1018 Pa·s, respectively. LaFemina et al.  find near Vatnajökull a stronger lower lithosphere (1019 to 1020 Pa s), which may reflect an increased crustal thickness. For most of Iceland, the seismic crustal thickness is 30–40 km; it is thickest under Vatnajökull and thins to 20 km in the southwest [Foulger and Natland, 2003].
 To assess the potential impact of these effects, we compute the effect of viscoelastic relaxation on the deglaciation-induced uplift using the 3D version of the finite element code GTecton [Govers and Wortel, 2005]. We try the effects of two different models—one with a 40 km elastic plate and half-space viscosity of 1018 Pa·s (model A) and a second one with a thinner elastic layer over a viscoelastic half space with a higher viscosity (5 km elastic plate and half-space viscosity of 1019 Pa·s, model B). Model A is similar to the model of Auriac et al.  but has a lower viscosity, simulating the effect of elevated temperature due to the mid-ocean ridge. Model B has a low lower crustal (5–40 km) viscosity, which could be the result of high water content or nonlinear rheology. We use a time-variable, constant disk load to simulate a realistic deglaciation history (see caption of Figure 7 for details of the load).
 For model A, the elastic and viscoelastic responses are similar. The viscous component produces a constant offset of 2 mm/yr (red dashed line in Figure 7a) without affecting the uplift gradient. For model B, the viscous component decreases from 10 mm/yr at the load center to 1 mm/yr at 150 km distance (Figure 7b). It contributes ∼2.5 mm/yr to the uplift gradient at 50–80 km distance. Our approach of eliminating long-wavelength deformation further lessens the impact of possible viscous deformation because it is largely removed from the observations. Weighting based on data resolution further reduces the magnitude of these viscous effects because areas with higher viscous than elastic deformation (far from the ice edge) receive less weight.
 We conclude that for modeling relative uplift near the ice edge the viscous component can safely be neglected, except in the case of a very weak lithosphere and a thin elastic layer. In this case, the elastic half-space assumption (i.e., neglecting viscous deformation) would lead to an overestimation of the mass loss rate, with the actual rates being smaller than the estimates. In other words, except for this very special situation, relative InSAR observations at the ice edge are mainly sensitive to the elastic component but not to the viscous component of surface deformation associated with melting ice. Of course, InSAR can only resolve mass loss at the edge of glaciers and ice sheets.
 The low viscosities of Model B are unlikely to occur under Iceland for two reasons. First, the upper mantle is relatively dry [Barnhoorn et al., 2011] and there is no water that could act to reduce the viscosity. Second, for typical grain sizes of mid-ocean ridge mantle rock and for relatively low deglaciation-induced strain rates, linear diffusion creep is likely the dominant deformation mechanism [Barnhoorn et al., 2011].
6.3. Young's Modulus
 Our model assumes a Young's modulus of 40 GPa. It is important to justify this assumption because surface displacement is proportional to the load and inversely proportional to Young's modulus (equations (1) and (2)). An inversion with twice the value of the Young's modulus would yield twice the mass loss rate.
 This modulus was estimated from GPS observations of the vertical deformation associated with seasonal loading in Iceland (winter snowfall and summer melting) [Grapenthin et al., 2006]. It can be considered an effective Young's modulus for the elastic crust sampled by the load. For smaller loads, the effective Young's modulus could be smaller because the shallow crust is likely to be more fractured, hence weaker. For example, Pinel et al.  found an effective Young's modulus of 29 GPa for the smaller Myrdalsjökull ice cap, suggesting that also the load change due to melting is of smaller spatial extent than for Vatnajökull. For larger seasonal loads significantly larger effective Young's moduli are found [Bevis et al., 2005; Steckler et al., 2010].
 For the Icelandic crust, the mean P-wave velocities of 6.0 and 6.6 km/s at depths of 5 and 10 km [from Yang and Yang, 2005] correspond to dynamic modulii of 87 and 105 GPa, respectively (using a density of 2900 kg/m3 and Poisson's ratio of 0.25). Our choice of Young's modulus is significantly lower than these values and is more likely representative of conditions associated with relatively slow load changes induced by glacial melting compared to higher values estimated from the passage of seismic waves.
 Our values is consistent with the effective Young's modulus of 44 GPa of Nof et al.  from modeling uplift induced by rapid decline of the Dead Sea water level. The Dead Sea load change (∼15 km across) is similar in size to the Vatnajökull load change (k = 7.5 km).
6.4. Mass Loss Rate
 For the 1995–2009 period, the mass loss rate of the Vatnajökull ice cap estimated from the InSAR data is (depending on k) Gt/yr. Mass loss rates from this and previous studies are summarized in Table 1. Our estimate agrees with the 1994–2005 rate of 6.4 Gt/yr from Björnsson and Pálsson . A limitation of our study is that we only use observations from the southeast edge of the ice cap. That our mass loss rate estimate agrees with the in situ observations suggests that this section is melting at the average rate of the ice cap. The estimated mass loss is about twice the average mass loss rate of 3.5 Gt/yr from 1890 to 2003 [Pagli et al., 2007a]. The rather constant uplift velocity during 1995–2009 (Figures 2c and 2d) suggests ice loss at a constant rate, in contrast to Greenland where ice loss is accelerating [Jiang et al., 2010; Rignot et al., 2011a].
 We estimate mass loss rates for the Hofsjökull and Myrdalsjökull ice caps of 0.9 and 1.7 Gt/yr. Together with Langjökull's mass loss rate of 0.9 Gt/yr, the total loss rate for the four major Icelandic ice caps (Vatnajökull, Hofsjökull, Myrdalsjökull, and Langjökull) is 10.3 ± 1 Gt/yr. This is equivalent to the 11 ± 2 Gt/yr estimated from 2003 to 2010 GRACE data [Jacob et al., 2012].
 We have presented an approach to estimate ice loss from uplift measurements of the Earth's crust near glaciers and ice sheets that is optimized for the high spatial resolution of InSAR. The linear relationship between surface load change and ground uplift for elastic rheology allows us to estimate the ice mass loss rate from the measured uplift as long as prior information on Young's modulus and the spatial thinning pattern of ice is available. An exponential decrease in thinning rate with distance from the ice edge is applicable for many glaciers and ice sheets. Our InSAR-based approach resolves small-wavelength, relative changes in uplift across a SAR frame, and is especially sensitive to contemporaneous load changes along the ice edge. It is presumably also applicable to systems dominated by ice loss near the terminus, e.g., systems undergoing the initial stages of rapid retreat (later stages may be dominated by dynamic effects and mass loss farther from the terminus). Spatial variations in ice loss due to variations in air temperature or precipitation and variable outlet glacier geometry can in principle be resolved by separately analyzing different sections of ice.
 For Vatnajökull, we find for the 1995–2009 period an average ice mass loss rate of Gt/yr consistent with ground-based estimates and broadly consistent with GRACE estimates for the entire island. We used only observations from the southwestern ice edge, suggesting that mass loss in this area is representative of the entire ice cap.
 The National Aeronautics and Space Administration Earth Science division supported this study with grants to F.A., T.D., and S. W. We thank two anonymous reviewers for their constructive comments.