% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 18821 % Primary Name: RADE - TOMB % Record Type: TAVG % Country: Norway % Latitude: 59.31670 +/- 0.00005 % Longitude: 10.81670 +/- 0.00005 % Elevation (m): 14.00 +/- 0.50 % # of Months: 58 % % IDs: ghcnd - NOE00109822 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: 9f3d2927507fc4b28709dea4f53361c7 % Raw Data Hash: 36a41441068f536e55c41ac10ef7db7e % Adj Data Hash: 6b5dfa8b2891f6ca2c5bb8bf2e6b0ece % % 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 1956 1 NaN NaN NaN NaN NaN NaN -5.001 -1.127 1956 2 NaN NaN NaN NaN NaN NaN -9.285 -5.268 1956 3 NaN NaN NaN NaN NaN NaN -1.155 -0.686 1956 4 NaN NaN NaN NaN NaN NaN 3.015 -1.295 1956 5 NaN NaN NaN NaN NaN NaN 10.836 0.436 1956 6 NaN NaN NaN NaN NaN NaN 14.403 -0.731 1956 7 NaN NaN NaN NaN NaN NaN 16.155 -0.228 1956 8 NaN NaN NaN NaN NaN NaN 13.180 -2.257 1956 9 NaN NaN NaN NaN NaN NaN 10.979 -0.506 1956 10 NaN NaN NaN NaN NaN NaN 6.573 -0.083 1956 11 NaN NaN NaN NaN NaN NaN -0.476 -2.016 1956 12 NaN NaN NaN NaN NaN NaN 0.501 2.401 1957 1 -1.719 2.448 0 0 -1.719 2.448 -0.958 2.916 1957 2 -2.168 2.142 0 0 -2.168 2.142 -2.179 1.838 1957 3 -0.337 0.425 0 0 -0.337 0.425 -0.213 0.256 1957 4 4.633 0.616 0 0 4.633 0.616 4.536 0.226 1957 5 8.637 -1.470 0 0 8.637 -1.470 9.349 -1.052 1957 6 13.395 -1.446 0 0 13.395 -1.446 14.477 -0.657 1957 7 16.611 0.521 0 0 16.611 0.521 16.829 0.446 1957 8 14.760 -0.384 0 0 14.760 -0.384 15.181 -0.256 1957 9 10.100 -1.092 0 0 10.100 -1.092 9.798 -1.687 1957 10 7.208 0.845 0 0 7.208 0.845 7.546 0.890 1957 11 1.980 0.732 0 0 1.980 0.732 2.042 0.501 1957 12 -0.842 1.351 0 0 -0.842 1.351 -0.851 1.049 1958 1 -4.502 -0.335 0 0 -4.502 -0.335 -4.244 -0.370 1958 2 -7.939 -3.629 0 0 -7.939 -3.629 -7.382 -3.365 1958 3 -4.619 -3.857 0 0 -4.619 -3.857 -4.249 -3.780 1958 4 2.682 -1.336 0 0 2.682 -1.336 2.721 -1.589 1958 5 8.448 -1.659 0 0 8.448 -1.659 9.220 -1.181 1958 6 13.957 -0.884 0 0 13.957 -0.884 14.820 -0.314 1958 7 16.813 0.723 0 0 16.813 0.723 16.457 0.074 1958 8 14.579 -0.565 0 0 14.579 -0.565 14.692 -0.745 1958 9 11.885 0.693 0 0 11.885 0.693 12.409 0.924 1958 10 8.581 2.217 0 0 8.581 2.217 8.679 2.022 1958 11 3.050 1.802 0 0 3.050 1.802 3.380 1.840 1958 12 -3.152 -0.958 0 0 -3.152 -0.958 -2.081 -0.180 1959 1 -7.845 -3.678 0 0 -7.845 -3.678 -5.586 -1.712 1959 2 -2.729 1.582 0 0 -2.729 1.582 -2.665 1.352 1959 3 2.000 2.762 0 0 2.000 2.762 2.198 2.667 1959 4 5.697 1.679 0 0 5.697 1.679 5.813 1.502 1959 5 10.939 0.831 0 0 10.939 0.831 11.588 1.188 1959 6 14.228 -0.612 0 0 14.228 -0.612 15.379 0.246 1959 7 17.481 1.391 0 0 17.481 1.391 17.862 1.479 1959 8 17.248 2.104 0 0 17.248 2.104 17.348 1.911 1959 9 11.942 0.749 0 0 11.942 0.749 11.977 0.492 1959 10 6.794 0.430 0 0 6.794 0.430 7.287 0.630 1959 11 3.890 2.642 0 0 3.890 2.642 3.659 2.118 1959 12 0.334 2.527 0 0 0.334 2.527 0.186 2.086 1960 1 -4.044 0.123 0 0 -4.044 0.123 -3.896 -0.022 1960 2 -6.602 -2.292 1 0 NaN NaN -6.179 -2.161 1960 3 0.242 1.004 0 0 0.242 1.004 0.336 0.805 1960 4 4.935 0.918 0 0 4.935 0.918 4.542 0.231 1960 5 11.445 1.338 0 0 11.445 1.338 11.912 1.512 1960 6 15.418 0.578 0 0 15.418 0.578 16.115 0.982 1960 7 14.852 -1.239 0 0 14.852 -1.239 15.001 -1.382 1960 8 14.895 -0.249 0 0 14.895 -0.249 15.116 -0.321 1960 9 11.340 0.148 0 0 11.340 0.148 11.334 -0.151 1960 10 4.810 -1.554 0 0 4.810 -1.554 5.211 -1.446 1960 11 1.637 0.389 0 0 1.637 0.389 1.879 0.338 1960 12 -1.032 1.161 0 0 -1.032 1.161 -0.430 1.470 1961 1 -4.000 0.167 0 0 -4.000 0.167 -3.635 0.238 1961 2 0.405 4.716 0 0 0.405 4.716 0.123 4.140 1961 3 4.447 5.209 0 0 4.447 5.209 4.090 4.559 1961 4 5.300 1.283 0 0 5.300 1.283 5.789 1.479 1961 5 10.335 0.228 0 0 10.335 0.228 10.635 0.235 1961 6 15.575 0.734 0 0 15.575 0.734 16.100 0.966 1961 7 15.869 -0.221 0 0 15.869 -0.221 15.506 -0.877 1961 8 13.950 -1.194 0 0 13.950 -1.194 14.185 -1.252 1961 9 12.517 1.324 0 0 12.517 1.324 12.410 0.924 1961 10 10.119 3.756 0 0 10.119 3.756 10.391 3.735 1961 11 NaN NaN NaN NaN NaN NaN 2.968 1.427 1961 12 NaN NaN NaN NaN NaN NaN -3.251 -1.351 1962 1 NaN NaN NaN NaN NaN NaN -1.323 2.551 1962 2 NaN NaN NaN NaN NaN NaN -1.576 2.442 1962 3 NaN NaN NaN NaN NaN NaN -4.235 -3.766 1962 4 NaN NaN NaN NaN NaN NaN 4.838 0.528 1962 5 NaN NaN NaN NaN NaN NaN 8.752 -1.649 1962 6 NaN NaN NaN NaN NaN NaN 13.690 -1.444 1962 7 NaN NaN NaN NaN NaN NaN 14.383 -2.000 1962 8 NaN NaN NaN NaN NaN NaN 13.326 -2.111 1962 9 NaN NaN NaN NaN NaN NaN 10.221 -1.264 1962 10 NaN NaN NaN NaN NaN NaN 8.065 1.409