2015
DOI: 10.3189/2015jog14j204
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Reconstructing thermal properties of firn at Summit, Greenland, from a temperature profile time series

Abstract: We have constrained the value for thermal diffusivity of near-surface snow and firn at Summit Station, Greenland, using a Fourier-type analysis applied to hourly temperature measurements collected from eight thermistors in a closed-off, air-filled borehole between May 2004 and July 2008. An implicit, finite-difference method suggests that a bulk diffusivity of ∼25 ± 3m2 a−1 is the most reasonable for representing macroscale heat transport in the top 30 m of firn and snow. This value represents an average diffu… Show more

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Cited by 14 publications
(27 citation statements)
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“…Similar behavior has been observed in some alpine glaciers, which exhibit thermal fracturing in response to cold nighttime temperatures (Podolskiy et al, 2018;Zhang et al, 2019). Because short-period temperature fluctuations only propagate to a depth of several meters in glacial ice (Giese & Hawley, 2015), shallow icequake locations are consistent with the correlation between icequake activity and surface air temperatures. Since both the tidal and the thermal mechanisms produce horizontal tensional stress, it is likely that they act in concert.…”
Section: Temperature Controls Multiday and Seasonal Patterns In Seismsupporting
confidence: 78%
“…Similar behavior has been observed in some alpine glaciers, which exhibit thermal fracturing in response to cold nighttime temperatures (Podolskiy et al, 2018;Zhang et al, 2019). Because short-period temperature fluctuations only propagate to a depth of several meters in glacial ice (Giese & Hawley, 2015), shallow icequake locations are consistent with the correlation between icequake activity and surface air temperatures. Since both the tidal and the thermal mechanisms produce horizontal tensional stress, it is likely that they act in concert.…”
Section: Temperature Controls Multiday and Seasonal Patterns In Seismsupporting
confidence: 78%
“…Overall, Figure 3. Comparison of the evolution of the thermal conductivity with density between (a) our computations at −20 • C and the data of Giese and Hawley (2015) and Marchenko et al (2019), and (b) our computations at −3 • C and estimates from the commonly used parameterizations described in Table 1, the SC model, as well as equation (5). The bulk thermal diffusivity provided by Giese and Hawley (2015) (25 m 2 /year) was converted in terms of thermal conductivity (0.48 W·m −1 ·K −1 ) using a bulk density of 425 kg/m 3 and a density-dependent specific heat capacity at −30 • C of 1,412 J·kg −1 ·K −1 .…”
Section: Comparison With Predictive Formulas 351 Estimates At −3 • Cmentioning
confidence: 99%
“…We can estimate the diffusive e-folding timescale τ to 200 m depth for the temperature perturbation by nondimensionalizing the heat equation: τ ≈ z 2 /κ. Approximating the thermal diffusivity of firn κ ¼ 8 × 10 À7 m 2 s À1 (Giese and Hawley, 2015):…”
Section: Temperature Variabilitymentioning
confidence: 99%