% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 174976 % Primary Name: VINGAKER % Record Type: TAVG % Country: Sweden % Latitude: 59.67000 +/- 0.00500 % Longitude: 15.96000 +/- 0.00500 % Elevation (m): 67.00 +/- 0.50 % # of Months: 29 % % IDs: ghcnd - SWE00138730 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: 7d17cef1675cf63f2e4aae4331373da5 % Raw Data Hash: 33c8211a3f9a2475e24b4274a5762a02 % Adj Data Hash: 4b2c00268ea47a34cec06bb2c8065357 % % 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 1969 5 NaN NaN NaN NaN NaN NaN 8.570 -0.605 1969 6 NaN NaN NaN NaN NaN NaN 16.293 1.825 1969 7 NaN NaN NaN NaN NaN NaN 16.431 0.572 1969 8 NaN NaN NaN NaN NaN NaN 16.449 1.846 1969 9 NaN NaN NaN NaN NaN NaN 10.216 0.058 1969 10 NaN NaN NaN NaN NaN NaN 6.604 1.562 1969 11 NaN NaN NaN NaN NaN NaN -2.229 -1.889 1969 12 NaN NaN NaN NaN NaN NaN -7.234 -3.189 1970 1 NaN NaN NaN NaN NaN NaN -9.925 -3.889 1970 2 NaN NaN NaN NaN NaN NaN -14.401 -8.404 1970 3 NaN NaN NaN NaN NaN NaN -2.148 -0.236 1970 4 NaN NaN NaN NaN NaN NaN 1.624 -1.473 1970 5 10.223 0.294 0 0 10.223 0.294 9.278 0.103 1970 6 16.115 0.894 0 0 16.115 0.894 16.699 2.231 1970 7 15.435 -1.177 0 0 15.435 -1.177 14.637 -1.222 1970 8 15.003 -0.352 0 0 15.003 -0.352 14.647 0.045 1970 9 NaN NaN NaN NaN NaN NaN 9.541 -0.618 1970 10 6.413 0.618 0 0 6.413 0.618 5.679 0.637 1970 11 -0.783 -1.197 0 0 -0.783 -1.197 -1.897 -1.557 1970 12 -1.700 1.591 0 0 -1.700 1.591 -2.380 1.664 1971 1 -2.340 2.943 0 0 -2.340 2.943 -3.164 2.872 1971 2 -1.252 3.992 1 0 NaN NaN -3.240 2.757 1971 3 -2.144 -0.985 0 0 -2.144 -0.985 -3.281 -1.370 1971 4 3.435 -0.416 0 0 3.435 -0.416 2.416 -0.682 1971 5 11.260 1.331 0 0 11.260 1.331 10.394 1.218 1971 6 13.637 -1.584 0 0 13.637 -1.584 13.892 -0.576 1971 7 16.519 -0.093 0 0 16.519 -0.093 15.550 -0.309 1971 8 14.808 -0.547 0 0 14.808 -0.547 14.227 -0.376 1971 9 9.932 -0.980 0 0 9.932 -0.980 8.986 -1.172 1971 10 7.168 1.373 0 0 7.168 1.373 5.756 0.714 1971 11 -0.048 -0.462 0 0 -0.048 -0.462 -1.675 -1.336 1971 12 0.926 4.217 0 0 0.926 4.217 -0.733 3.311 1972 1 -6.229 -0.946 0 0 -6.229 -0.946 -7.516 -1.480 1972 2 -1.788 3.456 1 0 NaN NaN -3.669 2.328 1972 3 0.318 1.476 0 0 0.318 1.476 -0.420 1.491 1972 4 3.865 0.014 0 0 3.865 0.014 2.959 -0.139 1972 5 NaN NaN NaN NaN NaN NaN 9.088 -0.088 1972 6 NaN NaN NaN NaN NaN NaN 15.570 1.102 1972 7 17.908 1.296 0 0 17.908 1.296 17.987 2.128 1972 8 14.485 -0.870 0 0 14.485 -0.870 14.244 -0.358 1972 9 9.137 -1.775 0 0 9.137 -1.775 9.028 -1.131 1972 10 6.100 0.305 0 0 6.100 0.305 5.509 0.467 1972 11 2.103 1.690 0 0 2.103 1.690 1.087 1.426 1972 12 2.792 6.083 0 0 2.792 6.083 2.101 6.145 1973 1 NaN NaN NaN NaN NaN NaN -0.040 5.996 1973 2 NaN NaN NaN NaN NaN NaN -3.007 2.990 1973 3 NaN NaN NaN NaN NaN NaN 2.276 4.187 1973 4 NaN NaN NaN NaN NaN NaN 3.103 0.005 1973 5 NaN NaN NaN NaN NaN NaN 9.783 0.607 1973 6 NaN NaN NaN NaN NaN NaN 15.940 1.472 1973 7 NaN NaN NaN NaN NaN NaN 17.832 1.973 1973 8 NaN NaN NaN NaN NaN NaN 14.174 -0.428 1973 9 NaN NaN NaN NaN NaN NaN 8.253 -1.905 1973 10 NaN NaN NaN NaN NaN NaN 2.895 -2.146 1973 11 NaN NaN NaN NaN NaN NaN -3.270 -2.930 1973 12 NaN NaN NaN NaN NaN NaN -5.304 -1.260