% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 23367 % Primary Name: GUNNARN SOL (AUT) % Record Type: TAVG % Country: Sweden % Latitude: 64.96700 +/- 0.00050 % Longitude: 17.70000 +/- 0.00050 % Elevation (m): 278.00 +/- 0.05 % # of Months: 54 % % IDs: gsod - 021290-99999 % usaf - 21290 % % Sources: Global Summary of the Day % % Site Hash: 7816778c49e63ab3c871891c7401d670 % Raw Data Hash: 1a173c57fb3f86d1a987ab1faa1b9b2a % Adj Data Hash: 377dad055a5fe36d4164215f96637411 % % 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 1972 1 NaN NaN NaN NaN NaN NaN -15.065 -1.491 1972 2 NaN NaN NaN NaN NaN NaN -10.919 1.598 1972 3 NaN NaN NaN NaN NaN NaN -4.803 2.407 1972 4 NaN NaN NaN NaN NaN NaN -0.919 0.821 1972 5 NaN NaN NaN NaN NaN NaN 4.686 -0.090 1972 6 NaN NaN NaN NaN NaN NaN 13.011 2.162 1972 7 NaN NaN NaN NaN NaN NaN 15.003 2.135 1972 8 NaN NaN NaN NaN NaN NaN 11.065 -0.201 1972 9 NaN NaN NaN NaN NaN NaN 5.366 -0.827 1972 10 NaN NaN NaN NaN NaN NaN 1.637 1.375 1972 11 NaN NaN NaN NaN NaN NaN -6.283 0.437 1972 12 NaN NaN NaN NaN NaN NaN -4.040 7.030 1973 1 1.230 8.779 0 0 1.230 8.779 -5.010 8.563 1973 2 -0.730 5.762 1 0 NaN NaN -11.381 1.136 1973 3 2.505 3.690 0 0 2.505 3.690 -2.672 4.538 1973 4 2.891 -1.394 0 0 2.891 -1.394 -2.499 -0.759 1973 5 8.758 -2.043 0 0 8.758 -2.043 4.590 -0.186 1973 6 15.913 -0.960 0 0 15.913 -0.960 11.643 0.794 1973 7 18.876 -0.016 0 0 18.876 -0.016 16.132 3.264 1973 8 15.427 -1.865 0 0 15.427 -1.865 10.040 -1.227 1973 9 9.526 -2.692 0 0 9.526 -2.692 3.599 -2.594 1973 10 4.769 -1.518 0 0 4.769 -1.518 -2.209 -2.471 1973 11 -0.107 0.588 0 0 -0.107 0.588 -9.251 -2.531 1973 12 -2.668 2.377 0 0 -2.668 2.377 -13.654 -2.584 1974 1 0.192 7.741 0 0 0.192 7.741 -7.202 6.372 1974 2 0.663 7.155 0 0 0.663 7.155 -8.238 4.280 1974 3 0.073 1.258 0 0 0.073 1.258 -5.586 1.624 1974 4 4.022 -0.263 0 0 4.022 -0.263 0.892 2.632 1974 5 7.278 -3.523 0 0 7.278 -3.523 5.466 0.689 1974 6 13.698 -3.175 0 0 13.698 -3.175 11.824 0.975 1974 7 14.982 -3.910 0 0 14.982 -3.910 12.034 -0.834 1974 8 15.326 -1.965 0 0 15.326 -1.965 10.951 -0.315 1974 9 12.400 0.182 0 0 12.400 0.182 7.891 1.698 1974 10 5.690 -0.596 0 0 5.690 -0.596 0.284 0.022 1974 11 3.574 4.269 0 0 3.574 4.269 -7.100 -0.380 1974 12 1.317 6.363 0 0 1.317 6.363 -9.484 1.586 1975 1 1.341 8.890 0 0 1.341 8.890 -10.175 3.398 1975 2 -0.712 5.780 0 0 -0.712 5.780 -6.058 6.459 1975 3 0.873 2.058 0 0 0.873 2.058 -3.775 3.434 1975 4 3.276 -1.009 0 0 3.276 -1.009 -2.101 -0.361 1975 5 8.969 -1.833 0 0 8.969 -1.833 5.532 0.756 1975 6 13.228 -3.646 0 0 13.228 -3.646 9.097 -1.751 1975 7 17.502 -1.391 0 0 17.502 -1.391 12.138 -0.730 1975 8 17.194 -0.098 0 0 17.194 -0.098 10.978 -0.288 1975 9 13.506 1.288 0 0 13.506 1.288 7.031 0.838 1975 10 7.289 1.002 0 0 7.289 1.002 2.029 1.767 1975 11 3.743 4.438 0 0 3.743 4.438 -3.502 3.218 1975 12 0.425 5.470 0 0 0.425 5.470 -8.106 2.964 1976 1 -5.249 2.300 0 0 -5.249 2.300 -17.429 -3.855 1976 2 -2.330 4.163 0 0 -2.330 4.163 -9.399 3.119 1976 3 -3.222 -2.037 0 0 -3.222 -2.037 -8.488 -1.279 1976 4 2.759 -1.525 0 0 2.759 -1.525 -1.750 -0.010 1976 5 8.796 -2.005 0 0 8.796 -2.005 6.869 2.093 1976 6 12.583 -4.290 0 0 12.583 -4.290 10.159 -0.690 1976 7 15.375 -3.518 0 0 15.375 -3.518 11.987 -0.880 1976 8 15.473 -1.818 0 0 15.473 -1.818 11.568 0.302 1976 9 9.398 -2.820 0 0 9.398 -2.820 3.233 -2.960 1976 10 5.559 -0.727 0 0 5.559 -0.727 -0.836 -1.098 1976 11 2.481 3.177 0 0 2.481 3.177 -6.026 0.694 1976 12 -2.124 2.922 0 0 -2.124 2.922 -11.478 -0.408 1977 1 -2.004 5.546 0 0 -2.004 5.546 -13.736 -0.162 1977 2 -5.079 1.413 0 0 -5.079 1.413 -16.236 -3.719 1977 3 0.344 1.529 0 0 0.344 1.529 -4.244 2.966 1977 4 1.944 -2.340 0 0 1.944 -2.340 -3.658 -1.918 1977 5 7.801 -3.000 0 0 7.801 -3.000 3.313 -1.463 1977 6 12.883 -3.990 0 0 12.883 -3.990 9.671 -1.178 1977 7 NaN NaN NaN NaN NaN NaN 11.842 -1.026 1977 8 NaN NaN NaN NaN NaN NaN 10.393 -0.874 1977 9 NaN NaN NaN NaN NaN NaN 5.144 -1.049 1977 10 NaN NaN NaN NaN NaN NaN 1.589 1.327 1977 11 NaN NaN NaN NaN NaN NaN -6.139 0.581 1977 12 NaN NaN NaN NaN NaN NaN -6.672 4.398 1978 1 NaN NaN NaN NaN NaN NaN -13.343 0.231 1978 2 NaN NaN NaN NaN NaN NaN -17.434 -4.917 1978 3 NaN NaN NaN NaN NaN NaN -7.253 -0.044 1978 4 NaN NaN NaN NaN NaN NaN -2.879 -1.139 1978 5 NaN NaN NaN NaN NaN NaN 4.275 -0.501 1978 6 NaN NaN NaN NaN NaN NaN 11.638 0.789