Empirically based studies of glacier meteorology, especially for the Southern Hemisphere, are relatively sparse in the literature. Here, we use an innovative network of highly portable, low-cost thermometers to report on high-frequency (1-min time resolution) surface air temperature fluctuations and lapse rates (LR) in a ~800-m elevational range (from 3,675 to 4,492 m a.s.l.) across the glacier Olivares Gamma in the central Andes, Chile. Temperatures were measured during an intense field campaign in late Southern summer, 19–27 March 2015, under varying weather conditions. We found a complex dependence of high-frequency LR on time of day, topography, and wider meteorological conditions, with hourly temperature variations during this week that were probably mainly associated with short- and long-wave radiation changes and not with wind speed/direction changes. Using various pairs of sites within our station network, we also analyze spatial variations in LR. Uniquely in this study, we compare temperatures measured at heights of 1-m and 2-m above the glacier surface for the network of five sites and found that temperatures at these two heights occasionally differed by more than ±4°C during the early afternoons, although the mean temperature difference is much smaller (~0.3°C). An implication of our results is that daily, hourly, or even monthly averaged LR may be insufficient for feeding into accurate melt models of glacier change, with the adoption of subhourly (ideally 1–10-min) resolution LR likely to prove fruitful in developing new innovative high-time-resolution melt modelling. Our results are potentially useful as input LR for local glacier melt models and for improving the understanding of lapse rate fluctuations and glacier response to climate change.

1. Introduction

In recent decades, land-terminating glaciers and ice caps have thinned and receded in many regions of the world including Chile (e.g., [16]). This is a visible response to climate variability and climate change, or more specifically changes in precipitation/snow accumulation and atmospheric warming. Glaciers in Central Chile in the central dry Andes have shrunk and retreated rapidly during the last few decades due to a warming climate [79], with serious impacts on water resources including drinking water and water for irrigation purposes, hydroelectric power, and future global and regional sea-level rise [10]. In Central Chile the most notable feature of the changing climate from 1979 to 2006 was a strong contrast between the coastal region (surface cooling: −0.2°C decade−1) and the Andes region (surface warming: 0.25°C decade−1) [9, 11].

From a hydrological perspective glaciers are a reservoir of freshwater stored as ice, affecting water balance conditions (e.g., [5]). In the central part of Chile (taken as the region between 30 and 38°S), hydrological and climatological research studies highlight a lack of information on glaciological mass-balance observations and processes [2, 1214]; yet such knowledge is crucial for understanding the role of glaciers in current climate and hydrological perspectives. In a generally warming climate, the annual glacier runoff will ultimately decline as reduced glacier area outweighs the effect of increased glacier melting [15]. According to the World Glacier Monitoring Service (WGMS) (the organization maintaining and collecting information about glacier mass-balance observations globally), few glaciers in South America have meteorological and mass-balance observations for recent decades [16, 17], and this implies a fundamental lack of understanding of climatological and glaciological conditions in complex high mountain terrain.

High-frequency observed surface air temperature lapse rates (LR) on glaciers and in complex terrain are seldom reported. Lundquist and Cayan [18] analyzed surface temperature patterns in complex terrain in Sierra Nevada, indicating that a simple lapse rate often gives a poor description of a high-frequency spatial temperature structure. Blandford et al. [19] evaluated daily and seasonal variations of surface air temperature LR in southcentral Idaho emphasizing high variability on both daily and seasonal timescales. According to Minder et al. [20], high-resolution gridding of climate data often relies on assumptions such as a constant surface temperature lapse rate of −6.5°C km−1, ignoring high-frequency fluctuations in LR. This may have consequences for numerical weather prediction models when forecasting surface air temperatures and LR in complex terrains mainly during the winter season [21]. It may also have implications for understanding the impacts from inversion and Foehn effects in these terrains. Therefore, many snow and glacier surface melt models use an assumed linear LR, for example, on mean monthly or annual timescales, to distribute near-surface air temperature observations from automatic weather stations to locations at different elevations where meteorological observations are not available (e.g., [22]).

The present study arises from a four-year-long Fondecyt project using a multidisciplinary approach for the Rio Olivares basin, Central Chile, to significantly improve our overall understanding of meteorological, glaciological, and hydrological conditions. One of the aims of the project is to observe and analyze high-frequency near-surface air temperature fluctuations and conditions (not free-air lapse rates), including LR on Olivares Gamma Glacier [near-surface lapse rates are more variable than free-air lapse rates [23]]. This feeds into further aims to develop and set up meteorological, glacier surface mass-balance (SMB), and freshwater runoff models to determine the impact of high-frequent fluctuations in surface air temperature LR and of climate change upon glacier SMB and spatiotemporal freshwater runoff conditions under present day climate change conditions. The present work on glacier micrometeorology, together with improved models of meteorological and glacier SMB, will allow us to better understand the impacts from present climate conditions on glaciological and hydrological conditions in Central Chile and the complex interactions between these elements.

2. Study Site

The Olivares Gamma Glacier (11.5 km2 in 2012; 33°07′S, 70°10′W) (Figure 1) is located in the Rio Olivares basin (548 km2), in Central Chile, ca. 50 km northeast of Santiago de Chile, the capital city of Chile (7–8 mill. inhabitants). The Rio Olivares basin contains ca. a quarter of all the glacierised area feeding into the Rio Maipo basin, which provides water to Santiago de Chile and a substantial part of the Central Valley. The Olivares Gamma Glacier (hereafter referred to as Gamma) is a temperate glacier with a maximum thickness of 183 m water equivalent (w.e.) and an estimated water volume of 0.62 km3 w.e. [24]. Gamma extends from 3,650 to 4,800 m a.s.l. and is facing south (Figure 1) [5]. No debris-covered glacier ice is present at Gamma. The glacier surface is characterised by fields of penitentes (ice pinnacles formed by evaporation-melt processes on high-altitude, low-latitude glaciers), generally less than 0.5 m in height.

3. Methods

We used ten Tinytag sensors, model Tinytag Plus 2 = TGP-4017, deployed in small plastic radiation shields (model no. ACS-5050) mounted on individual stakes, with sensors placed at 1-m and 2-m height above the glacier surface at each site. The relatively low cost of a Tinytag temperature sensor, in comparison to an automatic weather station, meant that it was practicable to deploy ten Tinytags at five sites across the glacier (Figure 1). The equipment setup for two stations is shown in Figure 2. Station locations spanned an elevational range of ~800 m, which covered most of the glacier (Figure 1); elevation, slope, aspect, sensor ID numbers, and observation times are given in Table 1. These temperature loggers can store up to 32,000 readings and are suitable for deployment in the field for ~6–12 months; they have successfully been deployed in the sub-Arctic in previous studies (e.g., [25]).

Temperatures were logged at 1-min intervals, loggers were synchronised before deployment in the field, and all times reported in this paper are GMT/UTC (during the Austral, summer Chile is GMT −4 hours). Before being used in the field, the Tinytags were calibrated and validated against a full United Kingdom Accreditation Service (UKAS) Calibrated Max Min Thermometer, which had been calibrated to national standards using an independent calibration laboratory and was supplied with a traceable three-point calibration certificate taken at 0°C, 10°C, and 25°C full UKAS standards and a cited accuracy of 0.1°C. Over a 15°C temperature range, the Tinytags agreed on average to within +0.1–0.4°C of the reference thermometer, with a mean difference of +0.2°C. These combined accuracies are within the Tinytag manufacturer’s quoted accuracy of ±0.5°C for a 0–20°C temperature range.

We also used a supplementary LogTag TRIX-8 Temperature Recorder in each screen, which automatically logged air temperature at 2-min intervals, to support the main temperature dataset. The LogTags store a slightly lower number of readings (8,000; hence the lower time resolution used here) but are considered by the manufacturer to be accurate to ±0.5°C for −20°C to +40°C, that is, similar to the quoted accuracy of the Tinytags.

The Tinytag and LogTag temperature data were supplemented by an automatic weather station (AWS) (Station DGA) located at 3,631-m elevation in the proglacial landscape in front of the glacier (Figure 1). This provided hourly readings not just of air temperature but also of relative humidity, barometric pressure, wind speed and direction, and incoming/outgoing short- and long-wave radiation, which helped place our distributed air temperature records in a wider meteorological context.

We use standard descriptive statistics and correlation analysis to summarise observational results and compare key datasets. Lapse rates are expressed as negative when temperatures decrease with height and positive when temperatures increase with height.

4. Results and Discussion

4.1. General Weather Conditions

Figure 3(a) shows the meteorological data recorded at DGA during the fieldwork campaign. Daily temperatures ranged from ~3-4°C (during night) to ~12-13°C (during day) during the first few days then declined to −3–0°C to ~4–10°C during the latter part of the campaign. These temperature changes were mirrored by opposite changes in relative humidity (RH) to near-saturated air masses (~70–100% RH) during the latter half of the period, with RH having risen from a relatively dry air mass of 20–50% saturation during the first few days (Figure 3(a)). Surface air pressure dropped from ~666 hPa in the first two days to ~658–662 hPa in the days thereafter, reaching a minimum of <658 hPa on 25 March (Figure 3(b)). Winds were generally fairly light (~1–6 m s−1 for 10-min averages) and the wind was predominantly northwesterly during the first half of the period, turning more variable and mainly to a southerly point afterwards (Figure 3(c)). Incoming solar radiation peaked at between 700 and 900 W m−2 during the first half of the period, with relatively low peaks around 500–600 W m−2 on 23 and 24 March. Long-wave radiation, both incoming and outgoing, varied most during the first few days, reflecting clearer skies, stronger surface heating during daylight hours, and greater heat loss in night time (Figure 3(d)).

4.2. Glacier Near-Surface Hourly Temperatures and Lapse Rates and Comparison with DGA Meteorological Data

A comparison of DGA hourly surface air temperature with 2-m temperatures at the five Tinytag sites is shown in Figure 4. Figure 4(a) confirms a steady temperature decrease at all sites throughout the week-long period. DGA daytime peaks tended to occur 1-2 hours after temperature peaks at the Tinytag sites (Figure 4(b)). Mean hourly temperatures data for the DGA and Tinytag sites for 22–26 March 2015 are shown in Table 2 and Figure 4(b). DGA temperature ranged from 0.2°C at 10:00 to 7.0°C at 18:00; the nearest Tinytag 2-m Station S2 ranged from −0.1°C at 11:00 to 8.5°C at 17:00. At 11:00, on average, 2-m temperatures at five out of six sites were below freezing (except for DGA = 0.5°C). Overall, mean hourly temperatures (mean of all 24 hours) for these five days were similar at 2.7°C and 2.5°C for DGA and S2, although temperature variations were greater at S2, with a standard deviation of 2.5°C for all hourly data compared with 1.9°C at DGA. Mean hourly temperatures at the highest site S4 (4,492 m) were only slightly above freezing (0.2–1.0°C) at three hours, 16:00–18:00, compared with 23 hours for the lowest Tinytag site S2 and all hours at DGA (Figure 4(b)). This suggests that there was not much melting on the upper reaches of the glacier around Station 1 (S9/S4) during the study period. However, mean daily 2-m temperatures were above freezing (1.1°C at S6 and 2.5°C at S2) for the lowest two Tinytag stations. The highest mean hourly temperatures (at 17:00) of 8.5°C and 8.1°C at the same two sites were substantially above the mean hourly temperature of 5.4°C at the lower DGA site (which occupies much darker moraine and bedrock well below the glacier terminus). This could be due to strong reflected solar radiation enhancing surface air temperature readings (even though they were obtained from properly screened thermometers) at the Tinytag sites.

Mean hourly (22–26 March 2015) lapse rate data for various pairs of 2-m sensors are given in Table 3. In that table, the second from left column LR (S4-S2) shows the full-range lapse rate between the 2-m Tinytags at Stations 1 and 5, which are separated by 817 m in elevation (Figure 1; Table 1). This shows the strongest lapse rates, commonly −10.0°C km−1, during the early afternoon hours, with hourly lapse rates generally between about −7 and −8°C km−1 at other times. Therefore, these lapse rates were mainly slightly smaller than the dry adiabatic lapse rate (DALR) of −9.8°C km−1, and it was only at 15:00 that the DALR was on average exceeded (greater negative values). These super-adiabatic lapse rates could be due to preferential warming of lower slopes under conditions there of greater ice-melt and lower albedo, hence more absorption of incoming solar radiation. Subprofiles between pairs of stations reveal occasional much stronger mean hourly lapse rates, for example, −16.6°C km−1 for S5-S6 (Stations 3 and 4) at 17:00 and −13.0°C km−1 for S6–S2 (Stations 4 and 5) at 15:00 for the six days. Large reductions (smaller negative values) in lapse rates at some sites were evident for the mid-afternoon hours. These include most notably reductions in the S3-S2 (Stations 2–5) lapse rate from −10.1°C km−1 at 15:00 to −0.3°C km−1 at 18:00, the S3–S6 (Stations 2–4) lapse rate from −11.5°C km−1 at 17:00 to −1.2°C km−1 at 18:00, and the S6–S2 (Stations 4 and 5) lapse rate from −13.0°C km−1 at 15:00 to 1.5°C km−1 at 18:00 (Table 3). The latter case is the only reversed (positive) lapse rate value in the whole of Table 3, where the normal lapse rate profile (temperature decrease with height) temporarily changes sign at 18:00 on average over the six days (there is another, already mentioned near-neutral lapse rate of −0.3°C km−1 for S3-S2 at the same time).

These early afternoon large drops/reversals in lapse rates are mainly related to the diurnal temperature peaking one hour later at S3 (Station 2) compared with the lower S6 (Station 4) and S2 (Station 5)—and indeed the other two S4 and S5 2-m LogTags—sites; the only other site with peak temperature at 18:00 (in common with S3/Station 2) is DGA. Why do these two sites’ daily temperatures peak later than the others? There is nothing especially unusual about the slope and aspect of Station 2 compared with the other four stations (Table 1). As is clear from Figure 1, both Stations 2 and 3 are located fairly near the mid-point/centre line of the glacier, so anomalous shading from surrounding topography at Station 2 is not an issue [especially at this time of the year/local time of day, early afternoon, when the Sun was high in the (northern) sky]. Based on site photos, for example, Figure 2(b) for Station 3, the glacier surface at Station 3 appears significantly rougher and possibly consequently darker than Station 2, so it could be that a local effect of the glaciomorphology influences the surface energy balance, and this effect may delay the timing of the peak daily temperature at Station 2. We postulate that this is because the generally smoother, brighter ice surface at Station 2 takes longer to respond to increasing solar radiation during the first half of the day. The 2-m night-time temperatures at S3 (Station 2) and S5 (Station 3) are very similar but mid-afternoon temperatures are much higher at S3 (by over 2°C at 18:00, Table 2), even though they peak slightly later. These differences emphasize the importance of local glacier surface microstructure on the 1 cm to 10 m spatial scale, compared with broader-scale topography, in affecting surface air temperature daily peaks and the timings of these. Heterogeneous surface microstructure has an impact on both the spatial and temporal variability in lapse rates, as illustrated above. In agreement, Blandford et al. [19], working in mountainous regions in southcentral Idaho, showed that different synoptic weather types influenced surface lapse rates, where, for example, warmer air temperatures were associated with steeper lapse rates and vice versa.

Correlations between hourly temperature data and meteorological parameters recorded by the DGA AWS are given in Table 4. These show significant strong positive correlations between Tinytag temperatures and DGA air temperature, incoming shortwave radiation, and outgoing long-wave radiation but little/insignificant correlation between Tinytag temperatures, for any of the sites, and wind speed and direction recorded at DGA. This suggests that glacier surface air temperatures during the week-long period in question were regulated mainly by key radiative components of the surface energy balance and very little by advective processes (wind). While the wind speed data recorded at DGA suggest that wind does not have an impact on lapse rate, we cannot exclude the possibility that there could be microscale advection occurring along the glacier—particularly in those short periods when lapse rates become very high for a few minutes. Some kind of upslope convection is necessary to stabilize the atmosphere along slope. Given that there are no high-frequency wind measurements along the slope of the glacier in this study, advection cannot be entirely discounted. Although our findings are only for a week-long period due to practical fieldwork constraints, Pepin et al. [26] conducted a study in the uplands of northern England evaluating surface air temperature lapse rates, highlighting that steep lapse rates occurred with higher levels of solar radiation, but also that wind speed during the day had relatively little impact on lapse rates, in agreement with our results.

4.3. Comparison of Temperatures at 1-m and 2-m Heights above Glacier Surface

We also compare Tinytag temperatures recorded at 2-m and 1-m heights. Differences between these are generally small 0.1–0.4°C, but occasionally exceed 1°C based on mean hourly data (Table 5). Figure 5(a) shows occasional 2-1 m air temperature differences for individual days as great as ±4°C based on 1-min data. For the mean daily profile, greatest differences were between 13:00 and 20:00 UTC, and briefly exceed 1.5°C at S6-S7 (Station 4) based on 1-min data (Figure 5(b)). Figure 5(a) shows occasional 2-1 m air temperature differences for individual days as great as ±4°C based on 1-min data. Differences are generally negative (higher temperatures at 2 m) but positive in mid-afternoon (local time) at S5-S10 and S3-S8 (Stations 2 and 3). The greatest negative differences are for S6-S7, S4-S9, and S2-S1 (Stations 4, 1, and 5) in mid-afternoon.

The generally greater temperatures at 2-m can be attributed to boundary-layer effects of a cold ice surface having a stronger influence on suppressing air temperatures nearer the surface during daytime, especially under conditions of strong solar radiation, and heat loss through infrared radiational cooling lowering the surface temperature more during night time. The latter effect appears to have prevailed under clear night skies during the first half of the period (19–23 March 2015), as thereafter the night-time temperature bias was mainly much closer to zero (Figure 5(a)). Local site characteristics, such as albedo and topographic roughness, and/or meteorological changes, for example, local-scale microadvection, may explain the opposite sign of 2-1 m temperature differences during mid-afternoon at Stations 2 and 3, since temperature differences at all five sites were systematically slightly positive at other times of the day.

The good agreement of the systematic positive temperature bias from 23:00 to 12:00 supports the good relative accuracy/calibration of the Tinytags (discussed above). The 1-min data also show rapid variation of 2-1 m vertical lapse rates for several hours in mid-afternoon, reflecting rapid changes in the boundary-layer profile and energy exchanges between the atmosphere and surface: this effect was most marked on 24 and 25 March—a time of more unsettled weather conditions, lower solar radiation, and more variable wind (Figure 3).

4.4. Analysis of High-Frequency (1-min) Temperature and Lapse Rate Data

In this section we carry out a more detailed analysis of the 1-min data from the Tinytags, which are presented in Figures 68. Daily mean and mean daily (22–26 March 2015) temperatures for all ten Tinytag sensors (1-m and 2-m elevation at five sites) are reported in Table 6, and daily mean and mean daily lapse rates between various pairs of Tinytags are given in Table 7. Near-surface air temperature lapse rates for the full elevation profile (S4-S2 at 2-m and S9-S1 at 1-m height above the surface) were on average ~1.5–2.0°C km−1 lower on 24 and 25 March than the other days. This was during the unsettled weather period when relative humidity (as indicated by DGA) was much higher, indicating a near-saturated air mass. Since saturated air cools at a lower rate as it rises than nonsaturated air (as latent heat is released to its surroundings), this may explain the smaller lapse rates measured on 24/25 March. Although here we are looking at the near-surface lapse rate of the glacier surface rather than the free-air lapse rate of a rising air parcel, these two lapse rates can be related. The smallest daily mean lapse rates of −3.1°C km−1 and −3.3°C km−1 are seen for S6-S2 and S7-S1 (both are Stations 4 and 5) on 24 March (Table 7). This more moderate lapse rate on the lower reaches of the glacier may also be related to changes in the surface energy balance under more cloudy, humid weather conditions. The lapse rates on the upper reaches on the glacier (S4-S3 and S9-S8) are below −10°C km−1, which are some of the steepest lapse rates recorded. Figure 6(a) is a much higher-time resolution version of the temperature data in Figure 4(a) (but does not include DGA data). Although the two graphs look rather similar, Figure 6(a) shows striking short-term (minutes-timescale) temperature fluctuations that are hidden in Figure 4(a). For example, a ~4°C temperature drop at S2 is clearly visible just before the daily temperature peak on 26 March in Figure 6(a) is almost completely smoothed out in Figure 4(a); a similar feature is seen in the S1 profile in Figure 6(b).

These short-term temperature fluctuations contribute to brief blips in the lapse rates shown in Figure 7 of as high as ±30–50°C km−1 for several minutes, generally in the early afternoons: these are most marked for the S6-S2 and S7-S1 (Stations 4 and 5) subprofile on the lower part of the glacier and are much more modest (~0–−20°C km−1) for the full vertical profile (S4-S2 and S9-S1, Stations 1 and 5). Figure 8 shows the mean daily lapse rate profiles for various pairs of sites (e.g., between 2-m Tinytags in Figures 8(a) and 8(c) and 1-m Tinytags in Figures 8(b) and 8(d)). Figure 8(e) shows lapse rates for both the 2-m and 1-m Tinytags for the upper half of the glacier. Large fluctuations in the lapse rates in the early mid-afternoon (local time) dominate all the plots in Figure 8, in contrast to relatively stable lapse rates at other times of the day. The temporary lapse rate reversal from negative values to positive values for the lower two sites, best shown here for the S6-S2 2-m profile (Figure 8(a)), has been remarked on (Section 4.2) but is now shown in much more detail—especially regarding the extreme values reached—based on the 1-min Tinytag data. Here, for S6-S2, we see a spike going up to +5°C km−1 (Figure 8(a)), which, because it occurred between hours, is not apparent in the mean hourly lapse rate data in Table 3. The relatively large fluctuations in the afternoon lapse rates tend to be greater for the Tinytags at 2 m compared with those at 1 m (Figures 8(a)8(d)), indicating an atmospheric influence with stronger decoupling from the surface at the higher height.

4.5. Comparison of Tinytag and LogTag Temperature Data

The main Tinytag temperature data were compared with a supplementary LogTag temperature sensor that was also included in each screen. Mean temperature differences of LogTag minus Tinytag temperatures for 22–26 March are shown in Table 8 and Figure S2, and the whole time series are in Figure S1 (Supplementary Material, available online at https://doi.org/10.1155/2017/6581537). For nine out of ten instrument sites, these differences are within ±0.3°C, with an overall mean difference of +0.2°C. This small temperature difference was analyzed by time of day and was found to be greatest at +0.5°C for 12:00–15:00 GMT, that is, mid-late morning local time, and least at 0.0°C at 18:00–21:00 GMT. These differences are mainly within instrument error but the LogTag mid-late morning warm bias was accentuated at a couple of sites, that is, for S7 was +1.0°C at 12:00–15:00, +1.3°C at 15:00–18:00, and +0.9°C at 18:00–21:00. The S9 LogTag warm bias was +0.7°C at 12:00–15:00 and +0.8°C at 15:00–18:00. These slightly larger temperature differences at a couple of sites are either on the threshold of or slightly exceed instrument error and show an occasional tendency for the LogTags to give slightly higher temperatures than the Tinytags around midday. However, this small difference is apparently spatially random and not systematic across all sites. Figures S1 and S2, respectively, show comparisons of the Tinytag and LogTag temperature time series and mean daily temperature cycles, showing generally very good agreement at all sites. This very good agreement between the two independent sets of instruments, in addition to the absolute calibration procedure for the Tinytags described above, gives us high confidence in our results regarding near-surface glacier temperature lapse rate values and changes.

5. Summary and Conclusions

Our results show that near-surface lapse rates on Glacier Gamma were generally greater under clear/sunny weather conditions—especially in early afternoon—and decreased during a period of more unsettled, cloudy weather later on in the fieldwork, displaying similar trends to those reported for a mountainous region in southcentral Idaho [19]. Temperatures at 1-m and 2-m heights above the surface are generally similar, within 0.5°C, but occasionally vary by as much as ±4°C, depending on changes in the surface energy budget and in the ambient meteorological conditions. This makes it critical to document at what height temperatures are being recorded in any study of high-resolution glacier meteorology (most such studies do not measure air temperature at multiple heights). Our relatively low-cost Tinytag network was able to resolve these vertical temperature changes, as well as spatial/elevational changes in temperatures and lapse rates, at the 1-min timescale, in a dataset that is rarely available for whole glaciers, let alone a glacier in South America or Chile. A natural extension of this study could use suitably mounted and shielded Tinytags to acquire temperature data over the course of 6–12 months, albeit at a slightly decreased sampling time resolution (e.g., 15–30 min), due to the large Tinytag logger capacity (32,000, number of readings). This will provide a better understanding of the monthly, seasonal, and higher-time-resolution variabilities in lapse rates, since most models use linear LR assumptions on mean monthly to annual scales. Another consequence of our findings is that lapse rates—especially in daytime—can be highly spatially and temporally variable (at the 1-min to 1-hour timescale) across a small glacier, and therefore computer models of glacier melt can benefit significantly through having this kind of high-resolution information on surface air temperature lapse rates.

Moreover, we suggest that the assumption of linear lapse rates in glacier melt models appears not to be valid, at least on the subhourly timescale, and meteorological monitoring of a glacier should ideally include multiple temperature loggers along the vertical profile to capture these spatial/temporal inhomogeneities. Therefore, the kind of data here—especially if extended to longer time periods and/or more glaciers—can be used in a sensitivity study to help trial and develop glacier melt models as well as for improving understanding of glacier meteorology and glacier interaction with climate change.

Conflicts of Interest

The authors declare that they have no conflicts of interest.


The authors acknowledge financial project support from the Chilean government (Fondecyt Regular Project no. 1140172). Also, they thank JSPS (Japan Society for Promote Science) for support, under Project no. S17096. Edward Hanna would like to thank the University of Sheffield for the granting of a sabbatical, which enabled him to join the fieldwork team and pursue this research.

Supplementary Materials

Figure S1: Surface air temperature profiles for all ten Tinytag sensors, with accompanying Logtag temperature profiles.

Figure S2: Mean daily air temperature cycles (22–26 March 2015) for all ten Tinytag and Logtag sensors.

  1. Supplementary Material