Ocean variability contributing to basal melt rate near the ice front of Ross Ice Shelf, Antarctica

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Ocean variability contributing to basal melt rate near the ice front of Ross Ice Shelf, Antarctica Laurie Padman I. Arzeno, R.C. Beardsley, R. Limeburner, B. Owens, S.R. Springer, C.L. Stewart, M.J.M. Williams + G. Moholdt, H.A. Fricker, M.S. Dinniman, S.L. Howard Sponsored by NSF & NASA

Focus of talk Basal melt in the Ross Ice Shelf Frontal Zone (ISFZ) ICESat repeat-track surface heights ~20-50 km Arzeno et al. (2014; JGR-Oceans) Moholdt et al. (in revision; JGR-ES) Horgan et al. (2011; JGR-Oceans) Stern et al. (2013; JGR-Oceans)

Explain high melt rate (M b ) near RIS front Ice front Moholdt et al. [in revision] Horgan et al. [2011] Lagrangian analysis of ICESat

Ocean melt modes: Focus on Mode 3 Graphic courtesy of Mike Craven

Modeled M b Entire RIS Mean M b ~ 0.25 m a -1 M b (m/yr) RIS average

Melt rate is seasonal; highest in summer (JFM) Average M b (m a -1 ) for entire RIS, and ISFZ * only Mean ISFZ M b ~ 1.9 m a -1 More melt * ISFZ defined as within 30 km of ice front

Why seasonal? (1) Polynya insolation T S Polynya net surface heat flux (W/m 2 ) Ross Polynya ISFZ

Why seasonal? (2) Southward flow of MCDW Bathymetry Summer Winter

Cross-ice-front hydrographic contrasts Polynya ISFZ Summer Winter

What we know from satellites High annual-average M b near ice front ISFZ melt ~40% of total RIS melt Inferred from models Melt near an ice front is seasonal Upper-ocean heat in Ross Polynya in summer due to insolation + increased southward MCDW transport

Speculation Mode 3 melt is more responsive to annual variability of forcing than Mode 1 (grounding-line melt) Rapid ice-front thinning & retreat driven by enhanced Mode 3 melt would accelerate dynamic ice loss Climatological changes in summer ocean and sea-ice state in the Ross Polynya may affect dynamic ice loss Now we want In situ evidence for Mode 3 melt and seasonality Improved understanding of processes determining seasonality, to better represent ISFZ melt in future climate states Do we even know the sign of expected Mode 3 melt rate change?

In situ measurements ANDRILL: Coulman High sites

Sub-ice-shelf hydrography

Time series measurements AWS AWS GPS Moorings

M b from mooring u Ocean heat flux Q O =ρ w C p C H u ΔT Where u*=c 1/2 D u ΔT=T-T freeze All signal Tidal currents only To get M b, equate Q O to latent heat, with correction for through-ice conduction (~20%)

VM-2 (model) T Summer Current speed ΔT Winter No tides Tides Summer Warm, low u Winter Cold, high u Melt rate Tides change M b time dependence and average

Model output (no tides) Highest M b at this site is in winter, not summer, since extra u dominates over reduced ΔT 2 y @ 5-day averages 6 mo @ 4-h averages

Not shown Weather-band (period of days) variability is not correlated with local winds: Eddies and/or topographic-trapped waves along the ice front Strength of these processes depends on density gradients: cross-front, and vertical: These change with stratification in Ross Polynya and buoyant meltwater fluxes to and within the ISFZ

Summary (Ross ISFZ basal melt rate M b ) High M b near ice front (~2 m a -1 cf <0.3 m a -1 overall) ISFZ melt ~40% of net RIS melt Seasonal cycle of warm upper-ocean water near the ice front; insolation + MCDW southward advection But M b depends on high-frequency ocean variability (tides, eddies, frontal instabilities) with energy that is out of phase with upper-ocean T; => more complex M b (t) signal Implies sensitivity to interactions between atmosphere, ocean, ice shelf and sea ice at short time and space scales

Thank you

End formal talk

Explain high melt rates near RIS front Moholdt et al. [in revision] Lagrangian analysis of ICESat Horgan et al. [2011]

Annual cycle: 5-day averages No Tides Tides

Summer (2004/05) only: 4-h averages No Tides Tides

Summary (Ross ISFZ melt) High melt rate near ice front (~2 m a -1 cf <0.3 m a -1 overall) ISFZ melt ~40% of net RIS melt Seasonal cycle as warm upper-ocean water gets to ice front; insolation + MCDW southward advection Dependence on tides (~50%) and weather-band (~50%) W-B appears to be frontal instability, not local wind forcing, and so depends on ocean stratification differences between Ross Polynya water and water under ISFZ Implies sensitivity to interactions between atmosphere, ocean, ice shelf and sea ice