% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 25575 % Primary Name: HALEAKALI % Record Type: TAVG % Country: United States % State: HI % Latitude: 20.71670 +/- 0.00005 % Longitude: -156.25000 +/- 0.00005 % Elevation (m): 2973.90 +/- 0.05 % # of Months: 21 % % Alternate Names: Missing Station ID - 510992 % % IDs: coop - 510992 % ghcnd - USC00510992 % ncdc - 20023365 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % US Cooperative Summary of the Month % Multi-network Metadata System % % Site Hash: 2780580d0bd8198495fbdd71ce66b17e % Raw Data Hash: f5a550b523b31e9f5741766d036cc8af % Adj Data Hash: 7d95023084d7ca5958476a0125a11c33 % % The data for this station is presented below in several columns and in % several forms. The temperature values are reported as "raw", % "adjusted", and "regional expectation". % % The "raw" values reflect the observations as originally ingested by % the Berkeley Earth system from one or more originating archive(s). % These "raw" values may reflect the merger of more than one temperature % time series if multiple archives reported values for this location. % Alongside the raw data we have also provided a flag indicating which % values failed initial quality control checks. A further column % dates at which the raw data may be subject to continuity "breaks" % due to documented station moves (denoted "1"), prolonged measurement % gaps (denoted "2"), documented time of observation changes (denoted "3") % and other empirically determined inhomogeneities (denoted "4"). % % In many cases, raw temperature data contains a number of artifacts, % caused by issues such as typographical errors, instrumentation changes, % station moves, and urban or agricultural development near the station. % The Berkeley Earth analysis process attempts to identify and estimate % the impact of various kinds of data quality problems by comparing each % time series to neighboring series. At the end of the analysis process, % the "adjusted" data is created as an estimate of what the weather at % this location might have looked like after removing apparent biases. % This "adjusted" data will generally to be free from quality control % issues and be regionally homogeneous. Some users may find this % "adjusted" data that attempts to remove apparent biases more % suitable for their needs, while other users may prefer to work % with raw values. % % Lastly, we have provided a "regional expectation" time series, based % on the Berkeley Earth expected temperatures in the neighborhood of the % station. This incorporates information from as many weather stations as % are available for the local region surrounding this location. Note % that the regional expectation may be a systematically a bit warmer or % colder than the weather stations by a few degrees due to differences % in mean elevation and other local characteristics. % % For each temperature time series, we have also included an "anomaly" % time series that removes both the seasonality and the long-term mean. % These anomalies may provide an easier way of seeing changes through % time. % % Reported temperatures are in Celsius and reflect monthly averages. As % these files are intended to be summaries for convenience, additional % information, including more detailed flagging and metadata, may be % available in our whole data set files. % % The Berkeley Earth analysis was run on 15-Nov-2013 19:55:48 % % Raw Data QC Continuity Adjusted Data Regional Expectation % Year, Month, Temperature, Anomaly, Failed, Breaks, Temperature, Anomaly, Temperature, Anomaly 1939 4 NaN NaN NaN NaN NaN NaN 21.352 -0.501 1939 5 NaN NaN NaN NaN NaN NaN 22.437 -0.376 1939 6 NaN NaN NaN NaN NaN NaN 22.750 -0.941 1939 7 NaN NaN NaN NaN NaN NaN 23.463 -0.812 1939 8 NaN NaN NaN NaN NaN NaN 24.144 -0.615 1939 9 NaN NaN NaN NaN NaN NaN 24.176 -0.737 1939 10 NaN NaN NaN NaN NaN NaN 24.264 -0.413 1939 11 NaN NaN NaN NaN NaN NaN 23.343 -0.796 1939 12 NaN NaN NaN NaN NaN NaN 22.773 -0.134 1940 1 NaN NaN NaN NaN NaN NaN 22.255 0.222 1940 2 NaN NaN NaN NaN NaN NaN 21.968 0.407 1940 3 NaN NaN NaN NaN NaN NaN 21.887 0.306 1940 4 9.222 1.772 0 0 9.222 1.772 22.870 1.017 1940 5 8.778 0.367 0 0 8.778 0.367 23.409 0.596 1940 6 11.000 1.712 0 0 11.000 1.712 24.131 0.440 1940 7 11.111 1.240 0 0 11.111 1.240 24.748 0.474 1940 8 10.222 -0.134 0 0 10.222 -0.134 25.189 0.430 1940 9 9.722 -0.788 0 0 9.722 -0.788 25.018 0.105 1940 10 9.944 -0.329 0 0 9.944 -0.329 25.023 0.346 1940 11 9.111 -0.625 0 0 9.111 -0.625 24.660 0.521 1940 12 9.167 0.662 0 0 9.167 0.662 23.248 0.341 1941 1 8.111 0.481 0 0 8.111 0.481 22.551 0.518 1941 2 7.278 0.120 0 0 7.278 0.120 21.184 -0.377 1941 3 7.222 0.044 0 0 7.222 0.044 21.138 -0.443 1941 4 9.444 1.994 0 0 9.444 1.994 22.045 0.191 1941 5 9.000 0.590 0 0 9.000 0.590 22.554 -0.259 1941 6 10.611 1.323 0 0 10.611 1.323 24.012 0.321 1941 7 10.667 0.795 0 0 10.667 0.795 24.434 0.159 1941 8 10.278 -0.078 0 0 10.278 -0.078 25.359 0.599 1941 9 9.667 -0.843 0 0 9.667 -0.843 25.370 0.458 1941 10 7.889 -2.384 0 0 7.889 -2.384 24.693 0.017 1941 11 9.333 -0.402 0 0 9.333 -0.402 24.202 0.064 1941 12 NaN NaN NaN NaN NaN NaN 22.376 -0.531 1942 1 NaN NaN NaN NaN NaN NaN 22.074 0.041 1942 2 -3.350 -10.508 1 0 NaN NaN 21.697 0.137 1942 3 NaN NaN NaN NaN NaN NaN 20.168 -1.413 1942 4 NaN NaN NaN NaN NaN NaN 20.991 -0.862 1942 5 NaN NaN NaN NaN NaN NaN 22.922 0.109 1942 6 NaN NaN NaN NaN NaN NaN 23.763 0.072 1942 7 NaN NaN NaN NaN NaN NaN 24.442 0.168 1942 8 NaN NaN NaN NaN NaN NaN 25.002 0.243 1942 9 NaN NaN NaN NaN NaN NaN 25.158 0.246 1942 10 NaN NaN NaN NaN NaN NaN 25.064 0.388 1942 11 NaN NaN NaN NaN NaN NaN 24.982 0.843 1942 12 NaN NaN NaN NaN NaN NaN 23.963 1.055 1943 1 NaN NaN NaN NaN NaN NaN 22.682 0.649 1943 2 NaN NaN NaN NaN NaN NaN 21.598 0.037