Abstract

The structure of lee‐side warming during foehn events is investigated as a function of cross‐barrier flow regime linearity. Two contrasting cases of westerly flow over the Antarctic Peninsula (AP) are considered – one highly nonlinear, the other relatively linear. Westerly flow impinging on the AP provides one of the best natural laboratories in the world for the study of foehn, owing to its maritime setting and the Larsen C Ice Shelf (LCIS) providing an expansive, homogeneous and smooth surface on its east side. Numerical simulations with the Met Office Unified Model (at 1.5 km grid size) and aircraft observations are utilized. In case A, relatively weak southwesterly cross‐Peninsula flow and an elevated upwind inversion dictate a highly nonlinear foehn event, with mountain wave breaking observed. The consequent strongly accelerated downslope flow leads to high‐amplitude warming and ice‐shelf melt in the immediate lee of the AP. However this foehn warming diminishes rapidly downwind due to upward ascent of the foehn flow via a hydraulic jump. In case C, strong northwesterly winds dictate a relatively linear flow regime. There is no hydraulic jump and strong foehn winds are able to flow at low levels across the entire ice shelf, mechanically mixing the near‐surface flow, preventing the development of a strong surface inversion and delivering large fluxes of sensible heat to the ice shelf. Consequently, in case C ice‐melt rates are considerably greater over the LCIS as a whole than in case A. Our results imply that although nonlinear foehn events cause intense warming in the immediate lee of mountains, linear foehn events will commonly cause more extensive lee‐side warming and, over an ice surface, higher melt rates. This has major implications for the AP, where recent east‐coast warming has led to the collapse of two ice shelves immediately north of the LCIS.

Highlights

  • The Antarctic Peninsula (AP) has been identified as one of the fastest warming regions on Earth since 1950 (Vaughan et al, 2003)

  • Journal of the Royal Meteorological Society published by John Wiley & Sons Ltd on behalf of the Royal Meteorological Society

  • The implication is that foehn in linear flow regimes can drive high melt rates over the Larsen C Ice Shelf (LCIS). This is accentuated when one considers that: (i) our modelled melt rates appear to be underestimates for case C – implied by comparison with Kuipers-Munneke et al.’s (2012) observed melt rate of 7.7 mm day−1 and confirmed in Elvidge (2013), who finds simulated daily melt during case C to be 65% that of automatic weather station (AWS) observations at Larsen Camp; and (ii) case C occurred in early summer when incoming solar radiation was relatively small for the summer melt periods the climatological values are averaged over

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Summary

Introduction

The Antarctic Peninsula (AP) has been identified as one of the fastest warming regions on Earth since 1950 (Vaughan et al, 2003). The use of a high-resolution model and the relative orographic simplicity of the AP (a ‘natural laboratory’), allows this article to provide, in companionship with E2014, new insight into the nature and dynamics of real foehn events It affords (as far as we are aware) the first in-depth analysis of foehn warming structure – in particular the spatial distribution of warming – and how it varies depending on the major mode of foehn variability, i.e. the linearity of the flow regime.

Theoretical context: flow-regime linearity
Observations and modelling
Identification of case studies
Case A
Case C
Lee-side structure: differences between cases A and C
Cross-peninsula flow dynamics
66 S 65 S Longitude
Discussion
Model sensitivity
Implications for Larsen C Ice Shelf melt
Conclusions and implications
Full Text
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