% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 9238 % Primary Name: SWANSON BAY % Record Type: TAVG % Country: Canada % Latitude: 50.62000 +/- 0.00500 % Longitude: -126.88000 +/- 0.00500 % Elevation (m): 0.00 +/- 0.50 % # of Months: 58 % % IDs: ghcnd - CA001067881 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: ee9de822af0c27d4af5081fdddfc99f0 % Raw Data Hash: 8d0dd40508282fd1c45a9f346556e14d % Adj Data Hash: 63e9545a40cb2618ed1b997943fd260c % % 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 1907 8 NaN NaN NaN NaN NaN NaN 12.750 -0.634 1907 9 NaN NaN NaN NaN NaN NaN 12.356 0.300 1907 10 NaN NaN NaN NaN NaN NaN 9.906 0.860 1907 11 NaN NaN NaN NaN NaN NaN 6.534 0.589 1907 12 NaN NaN NaN NaN NaN NaN 4.181 0.071 1908 1 NaN NaN NaN NaN NaN NaN 2.412 -0.505 1908 2 NaN NaN NaN NaN NaN NaN 3.346 -1.000 1908 3 NaN NaN NaN NaN NaN NaN 3.906 -0.563 1908 4 NaN NaN NaN NaN NaN NaN 5.599 -0.540 1908 5 NaN NaN NaN NaN NaN NaN 7.759 -0.970 1908 6 NaN NaN NaN NaN NaN NaN 10.243 -0.686 1908 7 NaN NaN NaN NaN NaN NaN 12.588 -0.271 1908 8 15.066 2.240 0 0 15.066 2.240 12.997 -0.387 1908 9 10.240 -1.257 0 0 10.240 -1.257 10.530 -1.526 1908 10 7.692 -0.796 0 0 7.692 -0.796 8.296 -0.751 1908 11 6.097 0.710 0 0 6.097 0.710 6.933 0.989 1908 12 2.239 -1.313 0 0 2.239 -1.313 3.436 -0.675 1909 1 -3.866 -6.225 0 0 -3.866 -6.225 -2.153 -5.070 1909 2 -0.125 -3.913 0 0 -0.125 -3.913 2.796 -1.550 1909 3 3.529 -0.382 0 0 3.529 -0.382 3.850 -0.619 1909 4 4.400 -1.181 0 0 4.400 -1.181 4.625 -1.515 1909 5 7.723 -0.449 0 0 7.723 -0.449 7.266 -1.463 1909 6 11.727 1.355 0 0 11.727 1.355 9.752 -1.178 1909 7 12.755 0.455 0 0 12.755 0.455 11.630 -1.228 1909 8 12.211 -0.614 0 0 12.211 -0.614 11.569 -1.815 1909 9 11.727 0.229 0 0 11.727 0.229 11.652 -0.403 1909 10 7.337 -1.151 0 0 7.337 -1.151 8.614 -0.432 1909 11 2.172 -3.215 0 0 2.172 -3.215 4.145 -1.800 1909 12 -0.965 -4.517 0 0 -0.965 -4.517 1.336 -2.774 1910 1 0.042 -2.316 0 0 0.042 -2.316 1.417 -1.499 1910 2 -1.750 -5.538 0 0 -1.750 -5.538 1.811 -2.535 1910 3 3.060 -0.851 0 0 3.060 -0.851 4.329 -0.140 1910 4 3.347 -2.235 0 0 3.347 -2.235 4.633 -1.506 1910 5 7.032 -1.139 0 0 7.032 -1.139 8.658 -0.072 1910 6 8.983 -1.388 1 0 NaN NaN 8.835 -2.095 1910 7 12.892 0.592 0 0 12.892 0.592 12.080 -0.779 1910 8 13.426 0.600 0 0 13.426 0.600 12.370 -1.014 1910 9 12.637 1.139 0 0 12.637 1.139 12.123 0.068 1910 10 NaN NaN NaN NaN NaN NaN 8.469 -0.578 1910 11 3.328 -2.058 0 0 3.328 -2.058 5.028 -0.917 1910 12 2.603 -0.949 0 0 2.603 -0.949 5.194 1.083 1911 1 -4.569 -6.928 0 0 -4.569 -6.928 -1.625 -4.541 1911 2 -1.741 -5.529 0 0 -1.741 -5.529 2.066 -2.280 1911 3 1.837 -2.074 0 0 1.837 -2.074 4.007 -0.462 1911 4 2.842 -2.740 1 0 NaN NaN 3.559 -2.580 1911 5 7.247 -0.925 0 0 7.247 -0.925 7.385 -1.345 1911 6 9.923 -0.448 0 0 9.923 -0.448 9.088 -1.841 1911 7 15.121 2.821 0 0 15.121 2.821 12.941 0.083 1911 8 15.284 2.458 0 0 15.284 2.458 13.444 0.060 1911 9 12.640 1.143 0 0 12.640 1.143 11.721 -0.335 1911 10 9.242 0.754 0 0 9.242 0.754 9.121 0.074 1911 11 1.945 -3.441 0 0 1.945 -3.441 4.197 -1.747 1911 12 2.216 -1.336 0 0 2.216 -1.336 4.180 0.070 1912 1 0.069 -2.289 0 0 0.069 -2.289 2.524 -0.393 1912 2 3.505 -0.283 0 0 3.505 -0.283 5.894 1.548 1912 3 4.265 0.353 0 0 4.265 0.353 4.363 -0.107 1912 4 6.068 0.487 0 0 6.068 0.487 6.062 -0.077 1912 5 10.724 2.553 0 0 10.724 2.553 9.780 1.051 1912 6 12.680 2.309 0 0 12.680 2.309 11.074 0.144 1912 7 15.713 3.413 0 0 15.713 3.413 13.217 0.358 1912 8 14.042 1.216 0 0 14.042 1.216 13.154 -0.230 1912 9 12.503 1.006 0 0 12.503 1.006 12.146 0.091 1912 10 7.926 -0.563 0 0 7.926 -0.563 8.284 -0.763 1912 11 4.138 -1.248 0 0 4.138 -1.248 5.859 -0.086 1912 12 2.755 -0.797 0 0 2.755 -0.797 4.457 0.346 1913 1 -2.248 -4.607 0 0 -2.248 -4.607 0.236 -2.681 1913 2 1.179 -2.609 0 0 1.179 -2.609 3.843 -0.503 1913 3 1.598 -2.313 0 0 1.598 -2.313 2.955 -1.514 1913 4 4.575 -1.006 0 0 4.575 -1.006 4.958 -1.181 1913 5 8.485 0.314 0 0 8.485 0.314 7.743 -0.987 1913 6 13.368 2.997 0 0 13.368 2.997 10.336 -0.594 1913 7 NaN NaN NaN NaN NaN NaN 12.244 -0.614 1913 8 NaN NaN NaN NaN NaN NaN 13.074 -0.310 1913 9 NaN NaN NaN NaN NaN NaN 11.069 -0.987 1913 10 NaN NaN NaN NaN NaN NaN 7.739 -1.308 1913 11 NaN NaN NaN NaN NaN NaN 5.509 -0.435 1913 12 NaN NaN NaN NaN NaN NaN 5.700 1.590 1914 1 NaN NaN NaN NaN NaN NaN 2.646 -0.271 1914 2 NaN NaN NaN NaN NaN NaN 5.015 0.669 1914 3 NaN NaN NaN NaN NaN NaN 5.186 0.717 1914 4 NaN NaN NaN NaN NaN NaN 6.950 0.811 1914 5 NaN NaN NaN NaN NaN NaN 9.097 0.367 1914 6 NaN NaN NaN NaN NaN NaN 9.914 -1.016