Presentation is loading. Please wait.

Presentation is loading. Please wait.

Fig. 4 States of the Antarctic Ice Sheet after 10,000 years.

Published byLiana Lesmana Modified over 5 years ago

Similar presentations

Presentation on theme: "Fig. 4 States of the Antarctic Ice Sheet after 10,000 years."— Presentation transcript:

1 Fig. 4 States of the Antarctic Ice Sheet after 10,000 years.
States of the Antarctic Ice Sheet after 10,000 years. (A to F) Shown is the ice thickness for (A) present-day Antarctica and the states of the ice sheet after forcing it for 10,000 years with cumulative emissions of (B) 500 GtC, (C) 1000 GtC, (D) 2500 GtC, (E) 5000 GtC, and (F) 10,000 GtC, simulated with the ice-sheet model PISM. Ice-free bedrock is shown in brown. For each scenario, the grounding line position after 100, 300, and 1000 years is shown in green, light green, and yellow, respectively. In the 1000 GtC scenario, both the West Antarctic Ice Sheet (red rectangular) and the Wilkes Basin (green rectangular) become unstable. For the 10,000 GtC scenario, the Antarctic continent is almost ice-free. Ricarda Winkelmann et al. Sci Adv 2015;1:e Copyright © 2015, The Authors

Download ppt "Fig. 4 States of the Antarctic Ice Sheet after 10,000 years."

Similar presentations

Fig. 4 Pupil shape and image quality in the model sheep eye.

Fig. 4 Pupil shape and image quality in the model sheep eye.
Fig. 5 In vivo MIP imaging of lipid and protein in C. elegans.

Fig. 5 In vivo MIP imaging of lipid and protein in C. elegans.
Fig. 1 Upward emission functions used to compute the maps.

Fig. 1 Upward emission functions used to compute the maps.
Fig. 1 Eastern Beringia during the LGM and retreat of the ice sheets.

Fig. 1 Eastern Beringia during the LGM and retreat of the ice sheets.
Fig. 4 Estimations of nonlinear functionals of a single-qubit state with the quantum Fredkin gate. Estimations of nonlinear functionals of a single-qubit.

Fig. 4 Estimations of nonlinear functionals of a single-qubit state with the quantum Fredkin gate. Estimations of nonlinear functionals of a single-qubit.
Fig. 1 Characterization of decellularized zECM.

Fig. 1 Characterization of decellularized zECM.
Fig. 5 MicroLED array with 3D liquid metal interconnects.

Fig. 5 MicroLED array with 3D liquid metal interconnects.
Fig. 2 The arrangements of metal core and ligands.

Fig. 2 The arrangements of metal core and ligands.
Fig. 2 Changes in ice surface elevation, h, of Thwaites Glacier.

Fig. 2 Changes in ice surface elevation, h, of Thwaites Glacier.
Fig. 3 Evolution of absorber with annealing.

Fig. 3 Evolution of absorber with annealing.
Fig. 5 Time evolution results of the MIROC climate model simulation with freshwater hosing. Time evolution results of the MIROC climate model simulation.

Fig. 5 Time evolution results of the MIROC climate model simulation with freshwater hosing. Time evolution results of the MIROC climate model simulation.
Fig. 1 Demographic shifts in knowledge producers.

Fig. 1 Demographic shifts in knowledge producers.
Fig. 4 Aβ16–22 fibrils increase the aggregation rate of Aβ40 to a greater extent than Aβ16–22 monomers. Aβ16–22 fibrils increase the aggregation rate of.

Fig. 4 Aβ16–22 fibrils increase the aggregation rate of Aβ40 to a greater extent than Aβ16–22 monomers. Aβ16–22 fibrils increase the aggregation rate of.
Fig. 3 Aβ16–22 can interact with Aβ40 monomers and dimers.

Fig. 3 Aβ16–22 can interact with Aβ40 monomers and dimers.
Order parameter θ as a function of time for the five events analyzed

Order parameter θ as a function of time for the five events analyzed
Fig. 2 Fluence-dependent emission characteristics of CH3NH3PbI3 recorded at 15 and 300 K. Fluence-dependent emission characteristics of CH3NH3PbI3 recorded.

Fig. 2 Fluence-dependent emission characteristics of CH3NH3PbI3 recorded at 15 and 300 K. Fluence-dependent emission characteristics of CH3NH3PbI3 recorded.
Fig. 2 Principle of attenuation-compensation for a Bessel light sheet.

Fig. 2 Principle of attenuation-compensation for a Bessel light sheet.
Fig. 1 Cryo-EM structure of yeast Elp123 showing its active site.

Fig. 1 Cryo-EM structure of yeast Elp123 showing its active site.
Destabilization of the WAIS in the unperturbed reference simulation

Destabilization of the WAIS in the unperturbed reference simulation
Fig. 3 Controlled phase shift.

Fig. 3 Controlled phase shift.

Similar presentations

Ads by Google