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**The Cryosphere**
An interactive open-access journal of the European Geosciences Union

Journal topic

- About
- Editorial board
- Articles
- Special issues
- Highlight articles
- Manuscript tracking
- Subscribe to alerts
- Peer review
- For authors
- For reviewers
- EGU publications
- Imprint
- Data protection

- About
- Editorial board
- Articles
- Special issues
- Highlight articles
- Manuscript tracking
- Subscribe to alerts
- Peer review
- For authors
- For reviewers
- EGU publications
- Imprint
- Data protection

- Abstract
- Introduction
- Model description
- Ice-shelf buttressing and grounding-line ice flux
- Results
- Discussion
- Conclusions
- Code and data availability
- Appendix A: Vertically integrated stress boundary condition at a free calving front
- Appendix B: Consistent results using different model parameters
- Author contributions
- Competing interests
- Acknowledgements
- References
- Supplement

**Research article**
09 Oct 2018

**Research article** | 09 Oct 2018

Grounding-line flux formula applied as a flux condition in numerical simulations fails for buttressed Antarctic ice streams

^{1}Potsdam Institute for Climate Impact Research (PIK), Member of the Leibniz Association, P.O. Box 60 12 03, 14412 Potsdam, Germany^{2}University of Potsdam, Institute of Physics and Astronomy, Karl-Liebknecht-Str. 24–25, 14476 Potsdam, Germany^{3}Department of Geography and Environmental Sciences, Northumbria University, Newcastle upon Tyne, NE1 8ST, UK

^{1}Potsdam Institute for Climate Impact Research (PIK), Member of the Leibniz Association, P.O. Box 60 12 03, 14412 Potsdam, Germany^{2}University of Potsdam, Institute of Physics and Astronomy, Karl-Liebknecht-Str. 24–25, 14476 Potsdam, Germany^{3}Department of Geography and Environmental Sciences, Northumbria University, Newcastle upon Tyne, NE1 8ST, UK

**Correspondence**: Ricarda Winkelmann (ricarda.winkelmann@pik-potsdam.de)

**Correspondence**: Ricarda Winkelmann (ricarda.winkelmann@pik-potsdam.de)

Abstract

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Currently, several large-scale ice-flow models impose a condition on ice flux across grounding lines using an analytically motivated parameterisation of grounding-line flux. It has been suggested that employing this analytical expression alleviates the need for highly resolved computational domains around grounding lines of marine ice sheets. While the analytical flux formula is expected to be accurate in an unbuttressed flow-line setting, its validity has hitherto not been assessed for complex and realistic geometries such as those of the Antarctic Ice Sheet. Here the accuracy of this analytical flux formula is tested against an optimised ice flow model that uses a highly resolved computational mesh around the Antarctic grounding lines. We find that when applied to the Antarctic Ice Sheet the analytical expression provides inaccurate estimates of ice fluxes for almost all grounding lines. Furthermore, in many instances direct application of the analytical formula gives rise to unphysical complex-valued ice fluxes. We conclude that grounding lines of the Antarctic Ice Sheet are, in general, too highly buttressed for the analytical parameterisation to be of practical value for the calculation of grounding-line fluxes.

How to cite

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How to cite.

Reese, R., Winkelmann, R., and Gudmundsson, G. H.: Grounding-line flux formula applied as a flux condition in numerical simulations fails for buttressed Antarctic ice streams, The Cryosphere, 12, 3229–3242, https://doi.org/10.5194/tc-12-3229-2018, 2018.

1 Introduction

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Estimating the future impact of the Antarctic Ice Sheet (AIS) on global sea levels invariably involves calculating changes in ice fluxes across grounding lines, as well as determining the migration of the grounding lines themselves. Accurately describing grounding-line dynamics can therefore be considered an essential prerequisite for any numerical ice-flow simulation of marine ice sheets such as the AIS. Accordingly, over the last decades, considerable efforts have focused on ensuring that large-scale ice-flow models are capable of correctly capturing the dynamical behaviour of grounding lines (Feldmann et al., 2014; Gagliardini et al., 2016; Gladstone et al., 2010; Goldberg et al., 2009; Pattyn et al., 2017; Seroussi et al., 2014). As part of these efforts, several model intercomparison experiments have been conducted to assess different approaches within the ice-sheet modelling community regarding the numerical modelling of marine-type ice sheets (Asay-Davis et al., 2016; Drouet et al., 2013; Pattyn et al., 2012, 2013). Although it is still a subject of active research, one of the outcomes of these intercomparison experiments has been to stress the need for a sufficiently fine resolution of the computational domain around grounding lines. Within the context of the shallow ice-stream computational models – a commonly used flow approximation for describing the flow of ice streams and ice shelves (MacAyeal, 1989; Morland, 1987) – it has, for example, been suggested that for many applications a horizontal resolution of around 1 km or less is suitable (Cornford et al., 2016; Gladstone et al., 2012; Pattyn et al., 2012). However, for large-scale ice flow models using uniform grids, employing such a high resolution globally for large ice sheets such as the AIS can be computationally prohibitively expensive. As a way of resolving this issue, and to allow for an accurate description of grounding-line dynamics without resorting to high spatial resolution, in a number of numerical modelling studies a “flux condition” is imposed at the grounding line, whereby the grounding-line flux is prescribed using an analytical expression (DeConto and Pollard, 2016; Docquier et al., 2011; Pattyn, 2017; Thoma et al., 2014). In other instances, the grounding-line migration rate is prescribed directly (Ritz et al., 2015).

The analytical flux expression most often used is based on a theoretical
study by Schoof (2007a, b) and was derived under the assumption
that the ice shelf provides no buttressing to the ice at the grounding
line. The absence of buttressing implies that the (vertically integrated)
horizontal stresses at the grounding line are not affected by the presence of
the ice shelf, and were the ice shelf to be removed and replaced by ocean
water, the state of stress (in a vertically integrated sense) would remain
unaffected (MacAyeal and Barcilon, 1988; Schoof, 2007a). However, in general, and
this is certainly the case for the AIS today
(De Rydt et al., 2015; Fürst et al., 2016; Reese et al., 2018), ice
shelves do provide some buttressing. To account for this, numerical models
use a modified analytical expression of ice flux based on Schoof (2007a)
involving an additional buttressing parameter (*θ*) describing the
modification in axial stress due to the mechanical impact of the ice shelf on
the stress state at the grounding line. The buttressing parameter (*θ*)
needs to be calculated by the numerical ice flow model and then inserted
into the analytical flux expression. The resulting flux is then used by the
corresponding numerical model as a flux condition along all grounding lines.

Previous numerical model intercomparison experiments (Pattyn et al., 2012) have shown that in the unbuttressed case there is, in general, good agreement between the analytically and numerically calculated ice fluxes for steady-state conditions. For one particular synthetic model set-up, Gudmundsson (2013) also found, in places, good agreement between analytically and numerically calculated ice fluxes for buttressed ice. The question now arises as to how accurately the analytical expression predicts grounding-line ice fluxes for realistic geometries such as that of the present-day AIS. More specifically, if one were to apply sufficiently high resolution around all Antarctic grounding lines, would fluxes calculated directly by such a high-resolution numerical model agree with the predictions of the analytical flux formula? Answering this question is the subject of this study. Here we assess the accuracy and the general applicability of the analytical flux formula for calculating ice fluxes across grounding lines of present-day Antarctica. We do this by comparing predicted analytical fluxes with independently numerically calculated ice fluxes using the community ice-flow model Úa (Gudmundsson, 2013). The ice flow model is applied to the whole continent, using high spatial resolution around all grounding lines of a few hundreds of metres.

The paper is structured as follows: first, we describe our numerical ice flow model Úa, and the model initialization procedure in Sect. 2. We then give a brief overview over the flux formula derived by Schoof (2007a) and discuss several different approaches to quantifying ice-shelf buttressing. The following Sect. 4 on the comparison between numerically calculated grounding-line ice fluxes and those by the flux formula forms the main part of the paper. This is followed by a discussion of the results and final conclusions in Sects. 5 and 6.

2 Model description

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We diagnose the fluxes at the grounding line with the finite-element ice-flow model Úa (Gudmundsson, 2013). The flow model Úa has been used to calculate the ice-flow for various geometries involving ice-shelf buttressing (De Rydt and Gudmundsson, 2016; Gudmundsson et al., 2017; Royston and Gudmundsson, 2016), and results obtained by the model submitted to a number of model intercomparison experiments (Pattyn et al., 2012) and (Pattyn et al., 2013). The model employs an unstructured grid and hence allows for resolving the grounding-line zone locally with high resolution. Simultaneous inversion for the ice rate factor (A) and the basal slipperiness (C) can be done either over nodal or over element values, and using either Bayesian- or Tikhonov-type regularisation. The gradient of the resulting objective function is calculated using the adjoint method.

Here we use Úa to solve the shallow ice-stream equations (MacAyeal, 1989; Morland, 1987) in a diagnostic mode using a Weertman-type sliding law (see Eq. 7) and Glen's flow law (see Eq. 8). In the glaciological literature the shallow ice-stream equations are also referred to as the shallow shelf approximation or shelfy stream approximation and often abbreviated as SSA. In the two horizontal dimensional situation (2HD) the SSA momentum equations are

$$\begin{array}{}\text{(1)}& {\displaystyle}{\displaystyle}{\mathrm{\nabla}}_{xy}\cdot \left(h\mathbf{R}\right)-{\mathit{\tau}}_{\mathrm{bh}}={\mathit{\rho}}_{\mathrm{i}}gh{\mathrm{\nabla}}_{xy}s+{\displaystyle \frac{\mathrm{1}}{\mathrm{2}}}g{h}^{\mathrm{2}}{\mathrm{\nabla}}_{xy}{\mathit{\rho}}_{\mathrm{i}},\end{array}$$

where

$$\begin{array}{}\text{(2)}& {\displaystyle}{\displaystyle}{\mathrm{\nabla}}_{xy}=\left({\partial}_{x},{\partial}_{y}\right),\end{array}$$

and **R**
is the tensor of resistive stresses given by
Eq. (15), *h* is the ice thickness, *s* is the ice surface elevation,
*ρ*_{i} is the vertically averaged ice density, and *τ*_{bh} is
the horizontal part of the bed-tangential basal traction *τ*_{b}.
Where the ice is floating *τ*_{bh}=0.
In the SSA the flotation criterion has the form *h*<*h*_{f} with

$$\begin{array}{}\text{(3)}& {\displaystyle}{\displaystyle}{h}_{\mathrm{f}}=(S-B){\mathit{\rho}}_{\mathrm{w}}/{\mathit{\rho}}_{\mathrm{i}},\end{array}$$

where *S* is the ocean surface, *B* the bedrock, and *ρ*_{w} is the ocean
density. The flotation criterion in Úa is evaluated at each integration
point of the elements of the finite element mesh and the basal drag term is
evaluated accordingly through a standard finite-element procedure involving
element-wise integration.

Using the ice flow model Úa, we calculate ice velocities for the entire Antarctic Ice Sheet, including all ice shelves. The SSA equations are solved throughout the computational domain. Stress boundary conditions (i.e. Neumann boundary conditions) are applied at the margins of the computational domain. Since the modelling domain covers the whole of the AIS, no inflow or outflow boundary conditions (i.e. Dirichlet boundary conditions) need to be applied at any sections of the boundary.

Two different computational meshes were generated and the sensitivity of the results was evaluated using linear (3-node), quadratic (6-node) and cubic (10-node) triangular elements. All results presented here were obtained using a very high-resolution mesh generated with the finite-element mesh generator Gmsh (Geuzaine and Remacle, 2009) with 1 360 894 triangular linear elements and 689 042 nodes. Within 5 km distance to the grounding line, the mesh was refined such that element sizes decrease towards the grounding line to a maximum size of 250 m directly at the grounding line. Overall, the elements have a maximal size of 179 307 m in the interior of the continent and a minimal size of 56 m along the grounding line. The mean element size is 1596 m and the median is 480 m. A regional example of the mesh is given in Fig. S1 in the Supplement. The robustness of the results was also tested based on the mesh used in Reese et al. (2018), as discussed in Appendix B.

Ice thickness and bed geometry input is based on the Bedmap2 estimates
(Fretwell et al., 2013). Vertically averaged ice densities were
calculated using firn thickness fields from RACMO2
(Lenaerts et al., 2012) and assuming a constant ice density of
910 kg m^{−3} and a firn density of 500 kg m^{−3}.
Resulting densities range from 770 to 910 kg m^{−3} and the horizontal gradients in vertically averaged
densities are hence small; see Fig. S2. In a few places the
bathymetry around the grounding lines was vertically modified to improve its
alignment with Bindschadler et al. (2011), with vertical adjustments of
maximally 50 m being allowed.

For the entire Antarctic set-up we inverted for basal slipperiness *C* (see
Eq. 7) and ice softness fields *A* (see Eq. 8) to
match observed 2015–2016 velocities derived from Landsat 8 imagery
(Gardner et al., 2018). The stress exponent of Glen's flow law was set to
*n*=3 and we repeated the inversion for a whole sequence of sliding law
exponents *m*=1, 2, 3, 4, 5, 7, 9, 11. We inverted for *A* and *C* over the
computational nodes using Tikhonov-type regularisation. The inversion
procedure minimizes the function

$$}{\displaystyle}J(u,p)=I\left(u\right)+R\left(p\right),$$

with respect to *p*, where *p* stands for model parameters to be determined
(i.e. *A* and *C*), *u* are modelled surface velocities, *I* is the data misfit
function, and *R* is the regularisation term. The misfit function *I* has the form

$$\begin{array}{}\text{(4)}& {\displaystyle}{\displaystyle}I={\displaystyle \frac{\mathrm{1}}{\mathrm{2}\mathcal{A}}}\int {\left({\mathit{v}}_{\mathrm{modelled}}-{\mathit{v}}_{\mathrm{observed}}\right)}^{\mathrm{2}}/{e}^{\mathrm{2}}\mathrm{d}A,\end{array}$$

where $\mathcal{A}=\int \mathrm{d}A$ is the total area, *v*_{modelled} and
*v*_{observed} are modelled and observed velocities, respectively,
and *e* are the data errors. The regularisation function *R* has the form

$$\begin{array}{ll}{\displaystyle}R& {\displaystyle}={\displaystyle \frac{\mathrm{1}}{\mathrm{2}\mathcal{A}}}\int \left({\mathit{\gamma}}_{\mathrm{s}}^{\mathrm{2}}{\left(\mathrm{\nabla}\left({\mathrm{log}}_{\mathrm{10}}\left(p\right)-{\mathrm{log}}_{\mathrm{10}}\left(\widehat{p}\right)\right)\right)}^{\mathrm{2}}\right.\\ {\displaystyle}& {\displaystyle}\left.+{\mathit{\gamma}}_{\mathrm{a}}^{\mathrm{2}}{\left({\mathrm{log}}_{\mathrm{10}}\left(p\right)-{\mathrm{log}}_{\mathrm{10}}\left(\widehat{p}\right)\right)}^{\mathrm{2}}\right)\mathrm{d}A\\ \text{(5)}& {\displaystyle}& {\displaystyle}={\displaystyle \frac{\mathrm{1}}{\mathrm{2}\mathcal{A}}}\int \left({\mathit{\gamma}}_{\mathrm{s}}^{\mathrm{2}}{\left(\mathrm{\nabla}{\mathrm{log}}_{\mathrm{10}}(p/\widehat{p})\right)}^{\mathrm{2}}+{\mathit{\gamma}}_{\mathrm{a}}^{\mathrm{2}}{\left({\mathrm{log}}_{\mathrm{10}}(p/\widehat{p})\right)}^{\mathrm{2}}\right)\mathrm{d}A,\end{array}$$

where *γ*_{a} and *γ*_{s} are regularisation parameters, and
$\widehat{p}$ are the a priori values for model parameters. Inversions were done for
a wide range of *γ*_{s} and *γ*_{a} and optimal values were determined from
an L-curve analysis. In the results shown here, we use *γ*_{a}=1 and
*γ*_{s}=10 000 m. However, our results are insensitive to the
particular values chosen.

For *γ*_{s}=10 000 m, *γ*_{a}=1 and the sliding exponent
*m*=3, the corresponding basal slipperiness *C* and the ice rate factor *A*
distributions are shown in Figs. S3 and S4. The
average difference between modelled and observed ice speed is 29 m per
year with a median of 13 m per year and a root mean square error of
103 m per year. The measured and modelled velocity fields for the
region of Institute Ice Stream are displayed in the upper panels of
Fig. 1. They agree
well in this area, as the residual histogram for this region shows in the
lower-left panel, but also for the entire continent; see Fig. S5. As a consequence of our
inverse methodology, modelled ice velocities are in close agreement with measurements.

From the modelled stresses obtained with our ice-flow model we calculate the
buttressing parameter *θ* as defined in Sect. 3. We do
this for each of the three different definitions for *θ* (see
Eqs. 11, 12, and 13). We then
calculate the analytical fluxes predicted by the flux formula,
i.e. Eq. (6). Note that we refer to these
fluxes as analytical fluxes, although their calculation involves the use of
our numerical ice-flow model for estimating the buttressing number *θ*.

We also calculate modelled grounding-line fluxes from modelled ice velocities. Since our modelled velocities are in good agreement with observed velocities, these modelled grounding-flux estimates will be in an equally good agreement with fluxes estimated directly from observed velocities. The analytical and the modelled flux estimates are then compared and analysed.

When calculating grounding-line fluxes we interpolate nodal quantities of the computational mesh onto the (calculated) grounding line. The grounding line does not, as such, enter the numerical calculations made by our numerical ice flow model. As described in Sect. 2, it is the flotation mask – evaluated at the integration points – that determines the impact of the basal drag term. However, in a post-processing step we determine the positions of the grounding lines from the flotation mask. Our approximation of the grounding line is a piecewise linear curve, with each linear segment representing the grounding line within a given computational element (see Figs. S1 and B1). We then interpolate nodal values onto the central point of each linear segment. The same procedure is employed when calculating both analytical and modelled fluxes.

3 Ice-shelf buttressing and grounding-line ice flux

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In Schoof (2007a, b), an expression for the grounding-line flux (*q*)
of marine ice sheets is derived. While the analysis is primarily
focused on a flow-line configuration where ice-shelf buttressing plays no
role, Schoof (2007a) also estimates how the flux might be affected by a
reduction *θ* in axial stress at the grounding line due to ice-shelf
buttressing. The resulting analytical flux expression is

$$\begin{array}{}\text{(6)}& {\displaystyle}{\displaystyle}q\left(x\right)={\mathit{\theta}}^{\frac{nm}{m+\mathrm{1}}}{\mathit{\rho}}_{\mathrm{i}}{h}^{\frac{\mathrm{1}+m(n+\mathrm{3})}{m+\mathrm{1}}}{\left({\displaystyle \frac{\mathrm{1}}{{\mathrm{4}}^{n}}}A{\left({\mathit{\rho}}_{\mathrm{i}}g\right)}^{n+\mathrm{1}}{\left(\mathrm{1}-{\mathit{\rho}}_{\mathrm{i}}/{\mathit{\rho}}_{\mathrm{w}}\right)}^{n}{C}^{\mathrm{1}/m}\right)}^{\frac{m}{m+\mathrm{1}}},\end{array}$$

where *q* is the ice flux across the grounding line, *h* is the ice thickness,
*ρ*_{i} the ice density, *ρ*_{w} the density of ocean water and *g* the
gravitational acceleration (please note that in the related Eq. 17 of
Gudmundsson, 2013 for the flux *q* there is a typo in the exponent of
the basal slipperiness *C*). For grounded ice, the tangential component of
the basal traction (*τ*_{b}) is related to the basal velocity (*v*_{b})
through the Weertman-type sliding law

$$\begin{array}{}\text{(7)}& {\displaystyle}{\displaystyle}{\mathit{\tau}}_{\mathrm{b}}={C}^{-\mathrm{1}/m}|{\mathit{v}}_{\mathrm{b}}{|}^{\mathrm{1}/m-\mathrm{1}}{\mathit{v}}_{\mathrm{b}},\end{array}$$

where *C* is the basal slipperiness, and *m* is the stress exponent, while
deviatoric stresses *τ*_{ij} and strain rates ${\dot{\mathit{\u03f5}}}_{ij}$ in ice
flow are linked via Glen's flow law

$$\begin{array}{}\text{(8)}& {\displaystyle}{\displaystyle}{\dot{\mathit{\u03f5}}}_{ij}=A{\mathit{\tau}}^{n-\mathrm{1}}{\mathit{\tau}}_{ij},\end{array}$$

with $\mathit{\tau}=\sqrt{{\mathit{\tau}}_{ij}{\mathit{\tau}}_{ij}/\mathrm{2}}$ the second invariant of the
deviatoric stress tensor, exponent *n* (often set to 3) and rate factor *A*.
Here *τ*_{ij} denote the components of the deviatoric stress tensor
and ${\dot{\mathit{\u03f5}}}_{ij}$ the components of the strain rate tensor.

As mentioned above, *θ* is a scalar quantity that describes the deviation
in deviatoric axial stress at the grounding line from the unbuttressed
situation. For an unbuttressed grounding line in one horizontal dimension
(i.e. no variations in any quantities transverse to the flow direction) and
assuming that the *x* axis of the coordinate system is aligned with the flow,
we have *τ*_{xx}=*τ*_{f} where

$$\begin{array}{}\text{(9)}& {\displaystyle}{\displaystyle}{\mathit{\tau}}_{\mathrm{f}}={\displaystyle \frac{{\mathit{\rho}}_{\mathrm{i}}g}{\mathrm{4}}}\left(\mathrm{1}-{\displaystyle \frac{{\mathit{\rho}}_{\mathrm{i}}}{{\mathit{\rho}}_{\mathrm{w}}}}\right)h,\end{array}$$

which can be derived from the stress boundary condition at the calving front
(see Appendix A). In the buttressed case, *τ*_{xx} is, however,
no longer necessarily equal to *τ*_{f}, and *θ* is defined as

$$\begin{array}{}\text{(10)}& {\displaystyle}{\displaystyle}{\mathit{\theta}}^{\mathrm{1}\mathrm{HD}}={\displaystyle \frac{{\mathit{\tau}}_{xx}^{\mathrm{1}\mathrm{HD}}}{{\mathit{\tau}}_{\mathrm{f}}}}.\end{array}$$

Here we have used the superscript 1HD to indicate that this definition of *θ*
is only unambiguous in the one horizontal dimensional situation (1HD).
In the more general two horizontal dimensional situation (2HD), where
the flow direction is not necessarily aligned with the (horizontal) normal to
the grounding line, several different definitions of *θ* are possible,
and in the literature at least three different definitions of *θ* have
been suggested. In the following we denote these by *θ*_{1}, *θ*_{2},
and *θ*_{3}, with

$$\begin{array}{}\text{(11)}& {\displaystyle}{\displaystyle}{\mathit{\theta}}_{\mathrm{1}}={\displaystyle \frac{{\mathit{n}}_{\mathrm{1}}\cdot \mathbf{R}{\mathit{n}}_{\mathrm{1}}}{\mathrm{2}{\mathit{\tau}}_{\mathrm{f}}}},\end{array}$$

where *n*_{1} is the normal to the grounding line, pointing
horizontally outwards from the grounded ice into the ice shelf, and

$$\begin{array}{}\text{(12)}& {\displaystyle}{\displaystyle}{\mathit{\theta}}_{\mathrm{2}}={\displaystyle \frac{{\mathit{n}}_{\mathrm{1}}\cdot \mathit{\tau}{\mathit{n}}_{\mathrm{1}}}{{\mathit{\tau}}_{\mathrm{f}}}},\end{array}$$

and

$$\begin{array}{}\text{(13)}& {\displaystyle}{\displaystyle}{\mathit{\theta}}_{\mathrm{3}}={\displaystyle \frac{{\mathit{n}}_{\mathrm{2}}\cdot \mathit{\tau}{\mathit{n}}_{\mathrm{2}}}{{\mathit{\tau}}_{\mathrm{f}}}},\end{array}$$

where *n*_{2} is the direction of ice flow at the grounding line and

$$\begin{array}{}\text{(14)}& {\displaystyle}{\displaystyle}\mathit{\tau}=\left(\begin{array}{cc}{\mathit{\tau}}_{xx}& {\mathit{\tau}}_{xy}\\ {\mathit{\tau}}_{xy}& {\mathit{\tau}}_{yy}\end{array}\right),\end{array}$$

is the (horizontal) deviatoric stress tensor, and

$$\begin{array}{}\text{(15)}& {\displaystyle}{\displaystyle}\mathbf{R}=\left(\begin{array}{ll}\mathrm{2}{\mathit{\tau}}_{xx}+{\mathit{\tau}}_{yy}& {\mathit{\tau}}_{xy}\\ {\mathit{\tau}}_{xy}& {\mathit{\tau}}_{xx}+\mathrm{2}{\mathit{\tau}}_{yy}\end{array}\right),\end{array}$$

is the tensor of resistive stresses. In the 1HD unbuttressed case where
*n*_{1}=*n*_{2}, ${\mathit{\tau}}_{xx}={\mathit{\rho}}_{\mathrm{i}}gh(\mathrm{1}-{\mathit{\rho}}_{\mathrm{i}}/{\mathit{\rho}}_{\mathrm{w}})/\mathrm{4}$,
and ${\mathit{\tau}}_{yy}={\mathit{\tau}}_{xy}=\mathrm{0}$, all these three
definitions of *θ* result in ${\mathit{\theta}}_{\mathrm{1}}={\mathit{\theta}}_{\mathrm{2}}={\mathit{\theta}}_{\mathrm{3}}=\mathrm{1}$. The first
definition (i.e. *θ*_{1}) has, for example, been used by
Gudmundsson (2013) to diagnose buttressing at the grounding line of an
idealised set-up. The second definition has, for example, been used by Pollard and DeConto (2012),
Thoma et al. (2014), and Pattyn (2017) as a flux condition, and the
third one has been used by Fürst et al. (2016) to diagnose “flow buttressing” within
Antarctic ice shelves. Note, however, that Pollard and DeConto (2012), Thoma et al. (2014, see Sect. 4.4),
Fürst et al. (2016, see Supplementary Eq. 2), and Pattyn (2017; see
Eq. 20) appear to use a different expression for *τ*_{f}, with
${\mathit{\tau}}_{\mathrm{f}}={\mathit{\rho}}_{\mathrm{i}}gh(\mathrm{1}-{\mathit{\rho}}_{\mathrm{i}}/{\mathit{\rho}}_{\mathrm{w}})/\mathrm{2}$, in which case $\mathit{\theta}=\mathrm{1}/\mathrm{2}$ in the
unbuttressed case and *θ* in Eq. (6)
must be replaced by 2*θ*.

The definition of *θ*_{1} is motivated by the form of the boundary
condition at the calving front in the shallow ice-stream approximation (see
Appendix A). For *θ*_{1}=1 the normal traction at the grounding
line equals that of a calving front. In the general 2HD situation, this same
interpretation does not hold for the definitions of *θ*_{2} and *θ*_{3}.
If *θ*_{1}>1 the ice shelf can be considered to be “pulling”
the ice at the grounding line, while *θ*_{1}<1 implies that the ice shelf
causes a reduction in normal traction at the grounding line; i.e. the ice
shelf “holds the ice back”. Note that, for all these three different
definitions, it is possible for *θ* to become negative. If, however, a
negative *θ* value is inserted into
Eq. (6), the resulting value for the flux *q*
is a negative or even a complex number for most combinations of *n* and *m* – a
clear indication that the analytical flux formula fails in such
situations. Only the specific combinations of *n* and *m*, such that $nm/(m+\mathrm{1})=\mathrm{2}k$
for *k*∈ℕ (for instance the combination *n*=3 and *m*=2),
“fix” the flux to a positive real number; however they introduce a
non-substantiated dependency between the flow law and the sliding law.
Furthermore, for these combinations and *θ*<0, enhanced
buttressing inconsistently yields an increase in ice flux. Physically, *θ*_{1}<0
corresponds to a situation where the traction vector at the grounding line
points in upstream direction. One possible situation giving rise to
*θ*_{1}<0 would be *τ*_{xx}<0 while *τ*_{yy}=0, with *x* being the
flow direction and the grounding line aligned with the *y* axis. In this
case, the ice at the grounding line experiences compression in the along-flow
direction and, hence, longitudinal strain rates are negative and ice
velocities become smaller as the grounding line is approached from upstream
direction. Another situation giving rise to *θ*_{1}<0 is that of equal
transversal compression and vertical extension of the ice column at the
grounding line; i.e. ${\mathit{\tau}}_{yy}=-{\mathit{\tau}}_{zz}<\mathrm{0}$ while *τ*_{xx}=0.

4 Results

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From the numerically modelled stress field we calculate the buttressing
parameter *θ*_{1} (given by Eq. 11) for all grounding lines
of the Antarctic set-up described in Sect. 2.1. While here we
focus on the buttressing parameter *θ*_{1}, our findings are
independent of the exact definition of *θ*, the choice of the sliding
law exponent *m*, the mesh and the details of the inverse methodology
applied (see Appendix B).

We find that the grounding lines of the Filchner–Ronne and Ross ice shelves are,
in general, highly buttressed with buttressing values significantly different
from unity (see Fig. 2). Typically, *θ*_{1}≤0.4,
and in many cases *θ*_{1}<0. Among the ice streams of these two
biggest ice shelves of the AIS, the dormant Kamb Ice Stream is the
least buttressed one, with *θ*_{1}≈0.4. Over all other ice streams
*θ* values are even smaller. Negative *θ* values are also found
over grounding-line segments located between active ice streams, for example
along the grounding line running between the Rutford and Institute ice streams.

An example of an ice stream where *θ*_{1}<0 over most of its grounding
line is the Institute Ice Stream (see Figs. 3
and 4). Inspection of the velocity field in the
vicinity of the grounding line of that ice stream reveals that ice flow
velocities decrease with distance as the grounding line is approached from
upstream direction (see also Fig. 1d). Consequently, both along-flow strain rates and along-flow deviatoric
stresses are negative (compressive). This general feature of ice flow around
the grounding line of Institute Ice Stream implies that its grounding line is
“over-buttressed” with the traction vector at the grounding line pointing in
an inland direction. Hence, independently of our numerical simulation of the
stress field, it is clear that for this ice stream a negative value for *θ* is obtained.

As discussed in Sect. 3 the analytical flux formula
(Eq. 6) is clearly not applicable in
situations where *θ* becomes negative. As *θ* is found to become
negative over large sections of the grounding lines of many the ice streams
of the two largest Antarctic ice shelves, i.e. Ross and Filchner–Ronne ice
shelves, it follows that the formula cannot be used to calculate
grounding-line ice fluxes over significant parts of the AIS.

We furthermore compare analytical and numerically modelled grounding-line ice
fluxes in all regions where *θ*_{1}≥0, i.e. where the application of
the analytical flux formula (Eq. 6)
results in real-valued ice fluxes. In particular, we compare both the flux
values pointwise along all grounding lines
(Fig. 5) and the total cumulative fluxes over
grounding lines of ice streams and ice shelves
(Table 1). When comparing cumulative
analytical fluxes, we are forced to assume values for those sections of
grounding lines for which *θ* is negative (and *q* complex). There we
assume *q*=0, which is equivalent to setting *θ*=0.

In general, we find significant differences between analytically calculated
and numerically modelled flux values. Analytical fluxes are much lower than
modelled in many locations of the Filchner–Ronne Ice Shelf, especially along the
grounding lines of the Rutford, Institute and Moeller ice streams
(Fig. 5). However, cumulative analytical fluxes
over all grounding lines of the Filchner–Ronne Ice Shelf are about 30 %
larger than modelled for *θ*_{1}, and this difference is considerably
larger for *θ*_{2} and *θ*_{3} (Table 1). A similar disagreement between
analytical and modelled fluxes is found for the Siple Coast ice streams such
as Bindschadler and MacAyeal ice streams, and for Byrd Glacier
(Fig. 5b). For Ross Ice Shelf the overall
difference is only 5 %, but, given the fact that *θ*_{1} is negative over
significant sections of its grounding line (where we set the analytical flux
values to zero), this agreement appears somewhat fortuitous.

For other ice shelves, cumulative fluxes are generally underestimated by the flux formula. Analytical fluxes for Pine Island Glacier and Thwaites Glacier, for example, deviate by −33 % and −52 % from the modelled fluxes, respectively. For George VI ice shelf, cumulative analytical fluxes are several times smaller than modelled ones (Table 1).

The analytical flux formula tends to strongly overestimate fluxes over grounding lines where ice flow is approximately tangential to the grounding line. The failure of the flux formula to correctly predict fluxes in such circumstances is not surprising, as the underlying assumptions of the formula are clearly not met in these situations. Nevertheless, this demonstrates the inherent conceptual difficulties in applying the formula to the Antarctic Ice Sheet.

Moreover, the analytical formula produces much higher spatial variability in fluxes than the numerically modelled ones. This can be clearly seen in Fig. 4, where analytical and modelled ice fluxes are plotted along the grounding lines of Rutford, Institute, Foundation and Recovery ice streams. Here, the grey background indicates sections of the respective grounding lines where the flux formula yields unphysical results. Variability in fluxes calculated with Úa occurs when ice flow is nearly aligned with the grounding line. We calculate fluxes within each triangular element using the normal of the piecewise-linear grounding-line curve, which may vary among individual line segments.

We test the sensitivity of our analytical flux calculations to different
degrees of regularisation (*γ*_{s} and *γ*_{a}), different values of
the sliding law stress exponent (*m*) and relaxation of the ice geometry, for
which our findings are summarised in Appendix B.
Numerically modelled fluxes are, as expected, mostly independent of the value
of the sliding law stress exponent *m*. This can be considered to be a
consequence of the inversion procedure, which ensures that modelled velocity
fields agree closely with measured data, independently of the value of *m*.
On the other hand, analytically calculated flux values are highly sensitive
to the value of *m* (see Fig. B3). For example, cumulative
analytical fluxes for Filchner–Ronne Ice Shelf increase by about a factor of
5 as *m* is changed from 1 to 7, while numerically modelled fluxes change
by less than 10 %. Numerically modelled fluxes are also insensitive to the
exact degree of regularisation applied, whereas analytically calculated flux
values change significantly (Fig. B5). The
dependency of the analytically calculated fluxes on the amount of
regularisation used in the numerical model is due to the impact
regularisation has on modelled stresses and, therefore, on the value of *θ*.

We also compare analytical fluxes as calculated using the three different
definitions (Eqs. 11, 12 and 13) for *θ*.
While overall spatial variability of *θ* is similar for these
three definitions, with all definitions giving rise to extended areas of
negative *θ* values, the cumulative flux for the alternative
definitions *θ*_{2} and *θ*_{3} are generally higher than for *θ*_{1} (see also
Fig. B4). Extended negative *θ* values and large
flux deviations are consistently found after a short relaxation period (see
Figs. S6 and S7).

5 Discussion

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The analytical grounding-line flux formula
Eq. (6) was derived for a flow-line
configuration (Schoof, 2007a), and there is no reason to doubt its validity
in that particular case. When applied to a flow-line configuration, many
current ice-flow models employing the shallow ice-stream approximation (SSA)
with Weertman-type sliding law, have demonstrated excellent agreement
between modelled and analytical grounding-line fluxes (Pattyn et al., 2012).
Ice fluxes and grounding-line positions calculated with the ice flow model
Úa also agree closely with those predicted by
Eq. (6), where such an agreement is to be
expected. The inclusion of the buttressing parameter *θ* was used by
Schoof (2007a) to illustrate the potential impacts of ice-shelf
buttressing on ice flux, provided its effects were sufficiently small
to not invalidate the basic assumption of a flow-line setting too strongly.
However, we find that most of the grounding lines of the AIS are highly
buttressed, with *θ* significantly different from unity. It seems likely
that at least part of the reason that the analytical flux formula fails
relates to the high degree of buttressing that we find to be characteristic
for most Antarctic ice streams.

When applied to the current geometry and the current flow field of the AIS, the flux formula predicts either unphysical or highly inaccurate flux values when compared to modelled ones. While we have done the comparison with numerically modelled fluxes, a comparison with observed fluxes – calculated from measured surface velocities, observed grounding-line positions, and measured ice thicknesses – would not alter our conclusions as, due to our inversion procedure, observed and modelled surface velocities are in good agreement.

The strongest indication that the analytical flux formula fails when applied
to the Antarctic Ice Sheet is arguably the fact that it predicts non-real
valued fluxes over significant parts of Antarctic grounding lines. This
happens whenever *θ* becomes negative. Although for specific
combinations of *n* and *m* (such as *n*=3 and *m*=2) the resulting exponents
in the flux formula are even numbers – in which case the analytical fluxes
are always real positive numbers – the flux values are still unphysical
(see Sect. 3). As we point out above, even a cursory
inspection of the velocity field of the AIS suffices to show that *θ* is
negative for a number of grounding lines (e.g. the Institute Ice Stream
grounding line). Hence, the occurrence of negative *θ* values is not
simply a feature of our particular numerical approach, but a general aspect
of the current ice-flow regime of the AIS.

As analytical ice fluxes are strongly dependent on ice thickness (*h*) at the
grounding line, they depend somewhat on the specifications of the numerical
model: the exact location of the grounding line is influenced by the mesh
resolution used by the model. The resulting error is an example of a
discretization error that becomes smaller as the mesh is refined. Other
numerical models using a different computational mesh may locate the
grounding line differently and hence calculate different ice flux values. We
tested the dependency of our modelled ice fluxes to grid resolution by using
several different meshes – an example of two such meshes is given in
Fig. B1 – and found none of our main conclusions to
be affected by differences in mesh resolution.

As measured by the buttressing parameter *θ*_{1}, almost all grounding
lines of the AIS can be considered to be strongly buttressed with, in most
cases, *θ*<0.4. Hence, theoretical concepts based on the assumption of
none, or insignificant, ice-shelf buttressing may not apply to present-day
Antarctica. One such theoretical prediction of considerable relevance for the
possible future of the AIS relates to the stability of its grounding lines.
In the absence of ice-shelf buttressing, grounding-line stability is
predicted to be related to local bed slope
(Schoof, 2007a, b, 2011; Thomas and Bentley, 1978; Weertman, 1974). However, in
the presence of ice-shelf buttressing no such simple conclusions can be drawn
(Goldberg et al., 2009; Gudmundsson, 2013; Gudmundsson et al., 2012; Pegler, 2016; Schoof et al., 2017).
Possibly, rather than being dominated by local bed slope, the stability
regime of the Antarctic Ice Sheet is to a leading order dependent on the
properties of the ice shelves downstream of its grounding lines
(e.g. geometry and structural integrity), as also supported by
Pegler et al. (2013) and Haseloff and Sergienko (2018). Further work is needed to address the
question of the stability of Antarctica's grounding lines.

6 Conclusions

Back to toptop
In our study, we compare grounding-line ice fluxes obtained by an ice-sheet
model with fluxes predicted by an analytical flux formula based on
Schoof (2007a, b). The formula includes a parameter (*θ*) to
account for ice-shelf buttressing, and the resulting flux is sometimes
applied as a grounding-line flux condition in numerical simulations. We find
that the formula results in unphysical and grossly inaccurate grounding-line
fluxes for most of the AIS. We furthermore find that almost all Antarctic
grounding lines are highly buttressed, suggesting that the underlying
assumptions of the analytical flux formula are not met for the current
configuration of the Antarctic Ice Sheet.

Code and data availability

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Code and data availability.

The data and code that support the findings of this study are available from the corresponding author upon request.

Appendix A: Vertically integrated stress boundary condition at a free calving front

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A derivation of the boundary condition at the calving front for the momentum equations in 2HD can be found in Cuffey and Paterson (2010) and van der Veen (1999), for example. At the calving face it holds that

$$}{\displaystyle}\underset{b}{\overset{s}{\int}}\mathit{\sigma}\cdot {\mathit{n}}_{\mathrm{cf}}\mathrm{d}z=-\underset{b}{\overset{S}{\int}}{p}_{\mathrm{w}}\cdot {\mathit{n}}_{\mathrm{cf}}\mathrm{d}z,$$

where *n*_{cf}=(*n*_{x}, *n*_{y}, 0) is the normal of the calving front pointing outwards,
*s* is the ice surface, *S* is the sea-level and *p*_{w} is hydrostatic pressure in
the ocean ${p}_{\mathrm{w}}={\mathit{\rho}}_{\mathrm{w}}g(S-z)$. The balance in *x* direction reads

$$\begin{array}{ll}{\displaystyle}\underset{b}{\overset{s}{\int}}\left({\mathit{\sigma}}_{xx}{n}_{x}+{\mathit{\sigma}}_{xy}{n}_{y}\right)\mathrm{d}z& {\displaystyle}=\underset{b}{\overset{S}{\int}}-{\mathit{\rho}}_{\mathrm{w}}g(S-z){n}_{x}\mathrm{d}z\\ \text{(A1)}& {\displaystyle}& {\displaystyle}=-{\displaystyle \frac{{\mathit{\rho}}_{\mathrm{i}}^{\mathrm{2}}g}{\mathrm{2}{\mathit{\rho}}_{\mathrm{w}}}}{h}^{\mathrm{2}}{n}_{x}.\end{array}$$

We can rewrite ${\mathit{\sigma}}_{xx}=\mathrm{2}{\mathit{\tau}}_{xx}+{\mathit{\tau}}_{yy}+{\mathit{\sigma}}_{zz}$ (since ${\mathit{\sigma}}_{xx}={\mathit{\tau}}_{xx}+p$, ${\mathit{\sigma}}_{zz}={\mathit{\tau}}_{zz}+p$ and ${\mathit{\tau}}_{xx}+{\mathit{\tau}}_{yy}=-{\mathit{\tau}}_{zz}$). Under the assumptions of the cryostatic stress approximation, ${\mathit{\sigma}}_{zz}=-{\mathit{\rho}}_{\mathrm{i}}g(s-z)$. The vertically integrated horizontal stress balance equals

$$\begin{array}{ll}{\displaystyle}\underset{b}{\overset{s}{\int}}\left({\mathit{\sigma}}_{xx}{n}_{x}+{\mathit{\sigma}}_{xy}{n}_{y}\right)\mathrm{d}z& {\displaystyle}=\mathrm{2}h{\mathit{\tau}}_{xx}{n}_{x}+h{\mathit{\tau}}_{yy}{n}_{x}+h{\mathit{\tau}}_{xy}{n}_{y}\\ \text{(A2)}& {\displaystyle}& {\displaystyle}-{\displaystyle \frac{{\mathit{\rho}}_{\mathrm{i}}g}{\mathrm{2}}}{h}^{\mathrm{2}}{n}_{x},\end{array}$$

since *τ*_{xx}, *τ*_{yy}, *n*_{x} and *n*_{y} do not vary vertically.
Inserting this in Eq. (A1) yields the following:

$$\begin{array}{}\text{(A3)}& {\displaystyle}{\displaystyle}\left(\mathrm{2}{\mathit{\tau}}_{xx}+{\mathit{\tau}}_{yy}\right){n}_{x}+{\mathit{\tau}}_{xy}{n}_{y}={\displaystyle \frac{{\mathit{\rho}}_{\mathrm{i}}g}{\mathrm{2}}}\left(\mathrm{1}-{\displaystyle \frac{{\mathit{\rho}}_{\mathrm{i}}}{{\mathit{\rho}}_{\mathrm{w}}}}\right)h{n}_{x}.\end{array}$$

A similar expression is obtained for the *y* direction. This can be abbreviated as

$$\begin{array}{}\text{(A4)}& {\displaystyle}{\displaystyle}\mathbf{R}\cdot \mathit{n}={\displaystyle \frac{{\mathit{\rho}}_{\mathrm{i}}g}{\mathrm{2}}}\left(\mathrm{1}-{\displaystyle \frac{{\mathit{\rho}}_{\mathrm{i}}}{{\mathit{\rho}}_{\mathrm{w}}}}\right)h\mathit{n}.\end{array}$$

Following Gudmundsson (2013) we obtain the normal buttressing value,
which compares the RHS and LHS of the equation above in the direction of the
normal ** n** at the grounding line:

$$\begin{array}{}\text{(A5)}& {\displaystyle}{\displaystyle}\mathit{\theta}={\displaystyle \frac{\mathit{n}\cdot \mathbf{R}\mathit{n}}{\frac{{\mathit{\rho}}_{\mathrm{i}}g}{\mathrm{2}}\left(\mathrm{1}-\frac{{\mathit{\rho}}_{\mathrm{i}}}{{\mathit{\rho}}_{\mathrm{w}}}\right)h}}={\displaystyle \frac{\mathit{n}\cdot \mathbf{R}\mathit{n}}{\mathrm{2}{\mathit{\tau}}_{\mathrm{f}}}}.\end{array}$$

In the case of a laterally uniform unconfined ice shelf with *τ*_{yy}=0
and *τ*_{xy}=0, this reduces to *τ*_{xx}∕*τ*_{f}.

A different approach that defines *θ* would be based on this vertically
integrated stress boundary condition in 1HD with ${\mathit{\theta}}^{\mathrm{1}\mathrm{HD}}={\mathit{\tau}}_{xx}/{\mathit{\tau}}_{\mathrm{f}}$.
In 1HD the normal at the grounding line is equal to the
flow direction. In 2HD, this is not necessarily true. Thus, to generalize the
longitudinal direction in the 1HD buttressing ratio, a choice needs to be
made. The longitudinal direction can either be generalized as the normal at
the grounding line (*θ*_{2}) or as the flow direction (*θ*_{3}).

Appendix B: Consistent results using different model parameters

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We test the robustness of our findings with respect to the mesh, the sliding
law stress exponent *m*, the definition of the buttressing parameter *θ*,
the regularisation parameter *γ*_{s} and relaxation of the ice
geometry. In a second pan-Antarctic set-up, based on a different mesh with quadratic base functions (instead of linear elements; see
Fig. B1), we find a similar pattern of
*θ*_{1}≤0,
which yields similar flux differences as exemplified in
Fig. B2 for the Filchner–Ronne Ice Shelf. In this case,
inversion was done for element-based basal slipperiness and ice softness
(instead of inverting on a nodal basis) using a Bayesian methodology (instead
of Tikhonov regularisation) and the MEASURES velocity data set
(Rignot et al., 2011 instead of Landsat 8, Gardner et al., 2018).
This set-up is further described in Reese et al. (2018). In this
set-up, Bedmap2 bathymetry is not adjusted around the grounding line. This
indicates that the exact location of the grounding line does not affect our findings.

For the Antarctic-wide set-up described in Sect. 2.1, we
test the choice of the stress exponent *m* in the sliding law. Different
choices of *m*=1, 3, 7 yield good agreement in modelled fluxes but large
disagreement between analytical fluxes; see Fig. B3.
Comparing shelf-wide integrated fluxes for major Antarctic ice shelves shows
that the definitions *θ*_{2} and *θ*_{3} of the buttressing
parameter also yield large deviations from the modelled fluxes; see
Fig. B4. Similarly, we find that the choice of the
regularisation parameter *γ*_{s} does not influence the results
significantly; see Fig. B5. Extended areas of
negative *θ* values and large flux deviations are consistently found
after a short relaxation run; see Figs. S6 and S7. Our findings are hence
independent of the details of numerical modelling choices.

Supplement

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Supplement.

The supplement related to this article is available online at: https://doi.org/10.5194/tc-12-3229-2018-supplement.

Author contributions

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Author contributions.

All authors designed the study. RR carried out the analysis based on an Antarctic set-up and using the ice-flow model Úa, both developed by GHG. RR prepared the manuscript with contributions from GHG and RW.

Competing interests

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Competing interests.

The authors declare that they have no conflict of interest.

Acknowledgements

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Acknowledgements.

We would like to thank Christian Schoof, the anonymous reviewer and the
editor Olivier Gagliardini for their helpful comments on the manuscript.
Ronja Reese was supported by the COMNAP Antarctic Research
Fellowship 2016–2017, the German Academic National Foundation, the
postgraduate scholarship programme of the state of Brandenburg and the
Evangelisches Studienwerk Villigst.

The article processing charges for this open-access

publication
were covered by the Potsdam Institute

for Climate Impact Research (PIK).

Edited by: Olivier Gagliardini

Reviewed by: Christian Schoof and one anonymous referee

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Short summary

Accurately representing grounding-line flux is essential for modelling the evolution of the Antarctic Ice Sheet. Currently, in some large-scale ice-flow modelling studies a condition on ice flux across grounding lines is imposed using an analytically motivated parameterisation. Here we test this expression for Antarctic grounding lines and find that it provides inaccurate and partly unphysical estimates of ice flux for the highly buttressed ice streams.

Accurately representing grounding-line flux is essential for modelling the evolution of the...

The Cryosphere

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