% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 167174 % Primary Name: GUADALCANAL AAF % Record Type: TAVG % Country: Solomon Islands % State: ZZ % Latitude: -9.43330 +/- 0.00005 % Longitude: 160.05000 +/- 0.00005 % Elevation (m): 10.10 +/- 0.05 % # of Months: 10 % % IDs: faa - AGGH % ghcnd - BPW00080601 % ncdc - 20029988 % wban - 80601 % % Sources: US First Order Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: db5f67ea9da3fdfcbbdad980d6c2577d % Raw Data Hash: fab5f0dd1d839337172b52281d0eab4a % Adj Data Hash: 664f96aefe739954fe5736107c2a66f7 % % 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 1948 1 NaN NaN NaN NaN NaN NaN 27.729 0.524 1948 2 NaN NaN NaN NaN NaN NaN 27.013 -0.216 1948 3 NaN NaN NaN NaN NaN NaN 27.295 0.046 1948 4 NaN NaN NaN NaN NaN NaN 26.986 -0.153 1948 5 NaN NaN NaN NaN NaN NaN 26.871 -0.373 1948 6 NaN NaN NaN NaN NaN NaN 26.347 -0.571 1948 7 NaN NaN NaN NaN NaN NaN 26.131 -0.458 1948 8 NaN NaN NaN NaN NaN NaN 26.597 0.070 1948 9 NaN NaN NaN NaN NaN NaN 26.334 -0.219 1948 10 NaN NaN NaN NaN NaN NaN 26.472 -0.082 1948 11 NaN NaN NaN NaN NaN NaN 26.644 -0.311 1948 12 NaN NaN NaN NaN NaN NaN 26.876 -0.213 1949 1 27.060 -0.073 0 0 27.060 -0.073 26.928 -0.277 1949 2 27.295 0.139 1 0 NaN NaN 27.322 0.093 1949 3 26.871 -0.305 0 0 26.871 -0.305 27.076 -0.172 1949 4 27.348 0.282 0 0 27.348 0.282 27.335 0.196 1949 5 26.885 -0.285 0 0 26.885 -0.285 27.101 -0.143 1949 6 26.432 -0.413 0 0 26.432 -0.413 26.625 -0.293 1949 7 25.903 -0.613 0 0 25.903 -0.613 26.121 -0.469 1949 8 25.974 -0.479 0 0 25.974 -0.479 25.962 -0.564 1949 9 26.530 0.050 0 0 26.530 0.050 26.439 -0.114 1949 10 26.593 0.112 1 0 NaN NaN 26.614 0.060 1949 11 NaN NaN NaN NaN NaN NaN 26.544 -0.410 1949 12 NaN NaN NaN NaN NaN NaN 26.843 -0.245 1950 1 NaN NaN NaN NaN NaN NaN 26.707 -0.498 1950 2 NaN NaN NaN NaN NaN NaN 27.207 -0.022 1950 3 NaN NaN NaN NaN NaN NaN 27.281 0.033 1950 4 NaN NaN NaN NaN NaN NaN 26.820 -0.319 1950 5 NaN NaN NaN NaN NaN NaN 27.176 -0.068 1950 6 NaN NaN NaN NaN NaN NaN 27.074 0.156 1950 7 NaN NaN NaN NaN NaN NaN 26.620 0.031 1950 8 NaN NaN NaN NaN NaN NaN 26.331 -0.196 1950 9 NaN NaN NaN NaN NaN NaN 26.644 0.091 1950 10 NaN NaN NaN NaN NaN NaN 26.592 0.038