% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 25725 % Primary Name: KOLOA (CGS) % Record Type: TAVG % Country: United States % State: HI % Latitude: 21.86700 +/- 0.00050 % Longitude: -159.45000 +/- 0.00050 % Elevation (m): 15.00 +/- 0.05 % # of Months: 21 % % IDs: gsod - 911665-99999 % icao - 1Z4 % usaf - 911665 % % Sources: Global Summary of the Day % % Site Hash: a1c9af1ec8565cc2ca1eab83db6dc0a4 % Raw Data Hash: 0253173e0d543cd57e492edd82251c42 % Adj Data Hash: 7bca6503a029103a91f4365dafb4cc59 % % 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 2 NaN NaN NaN NaN NaN NaN 22.538 0.942 1939 3 NaN NaN NaN NaN NaN NaN 21.921 0.110 1939 4 NaN NaN NaN NaN NaN NaN 21.910 -0.354 1939 5 NaN NaN NaN NaN NaN NaN 23.194 -0.217 1939 6 NaN NaN NaN NaN NaN NaN 23.572 -0.808 1939 7 NaN NaN NaN NaN NaN NaN 24.026 -0.879 1939 8 NaN NaN NaN NaN NaN NaN 24.784 -0.561 1939 9 NaN NaN NaN NaN NaN NaN 24.604 -0.863 1939 10 NaN NaN NaN NaN NaN NaN 24.509 -0.364 1939 11 NaN NaN NaN NaN NaN NaN 23.517 -0.518 1939 12 NaN NaN NaN NaN NaN NaN 22.452 -0.205 1940 1 NaN NaN NaN NaN NaN NaN 21.165 -0.693 1940 2 23.544 0.152 1 0 NaN NaN 22.097 0.500 1940 3 23.977 0.370 0 0 23.977 0.370 21.857 0.046 1940 4 25.450 1.391 0 0 25.450 1.391 23.054 0.790 1940 5 26.004 0.798 0 0 26.004 0.798 23.793 0.382 1940 6 26.580 0.404 0 0 26.580 0.404 25.073 0.692 1940 7 27.172 0.473 0 0 27.172 0.473 25.421 0.517 1940 8 27.844 0.704 0 0 27.844 0.704 26.009 0.664 1940 9 27.711 0.449 0 0 27.711 0.449 25.652 0.186 1940 10 26.923 0.255 0 0 26.923 0.255 25.228 0.356 1940 11 25.939 0.108 0 0 25.939 0.108 24.634 0.599 1940 12 NaN NaN NaN NaN NaN NaN 22.910 0.253 1941 1 24.237 0.584 0 0 24.237 0.584 22.424 0.566 1941 2 22.728 -0.663 0 0 22.728 -0.663 20.999 -0.597 1941 3 23.480 -0.127 0 0 23.480 -0.127 21.794 -0.017 1941 4 25.243 1.184 0 0 25.243 1.184 22.790 0.526 1941 5 26.047 0.841 0 0 26.047 0.841 23.127 -0.284 1941 6 26.969 0.794 0 0 26.969 0.794 24.822 0.442 1941 7 27.271 0.571 0 0 27.271 0.571 25.133 0.228 1941 8 27.520 0.379 0 0 27.520 0.379 25.964 0.619 1941 9 27.267 0.005 0 0 27.267 0.005 26.238 0.772 1941 10 25.783 -0.885 0 0 25.783 -0.885 25.099 0.226 1941 11 25.157 -0.673 0 0 25.157 -0.673 24.288 0.252 1941 12 NaN NaN NaN NaN NaN NaN 22.629 -0.028 1942 1 NaN NaN NaN NaN NaN NaN 21.518 -0.339 1942 2 NaN NaN NaN NaN NaN NaN 22.007 0.411 1942 3 NaN NaN NaN NaN NaN NaN 20.784 -1.027 1942 4 NaN NaN NaN NaN NaN NaN 21.331 -0.933 1942 5 NaN NaN NaN NaN NaN NaN 23.303 -0.108 1942 6 NaN NaN NaN NaN NaN NaN 24.354 -0.027 1942 7 NaN NaN NaN NaN NaN NaN 24.720 -0.185 1942 8 NaN NaN NaN NaN NaN NaN 25.565 0.220 1942 9 NaN NaN NaN NaN NaN NaN 25.506 0.040 1942 10 NaN NaN NaN NaN NaN NaN 25.179 0.307 1942 11 NaN NaN NaN NaN NaN NaN 24.871 0.836