% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 8971 % Primary Name: MACDONALD A % Record Type: TAVG % Country: Canada % Latitude: 50.08000 +/- 0.00500 % Longitude: -98.45000 +/- 0.00500 % Elevation (m): 255.00 +/- 0.50 % # of Months: 95 % % IDs: ghcnd - CA005011680 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: 57d4007d95a2220a90331737918b06a3 % Raw Data Hash: 918c7c87259cd92ebda7f11d10b51355 % Adj Data Hash: 6f2aa23a24f3ae48b34e227ffb27b472 % % 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 1950 7 NaN NaN NaN NaN NaN NaN 17.735 -1.129 1950 8 NaN NaN NaN NaN NaN NaN 15.598 -1.838 1950 9 NaN NaN NaN NaN NaN NaN 12.138 0.623 1950 10 NaN NaN NaN NaN NaN NaN 7.128 1.797 1950 11 NaN NaN NaN NaN NaN NaN -7.681 -2.682 1950 12 NaN NaN NaN NaN NaN NaN -17.869 -3.024 1951 1 NaN NaN NaN NaN NaN NaN -21.459 -1.339 1951 2 NaN NaN NaN NaN NaN NaN -14.779 1.402 1951 3 NaN NaN NaN NaN NaN NaN -12.356 -3.415 1951 4 NaN NaN NaN NaN NaN NaN 1.674 -0.484 1951 5 NaN NaN NaN NaN NaN NaN 12.162 1.819 1951 6 NaN NaN NaN NaN NaN NaN 13.790 -2.157 1951 7 19.914 0.039 1 0 NaN NaN 17.895 -0.968 1951 8 16.133 -2.315 1 0 NaN NaN 15.719 -1.717 1951 9 10.484 -2.043 1 0 NaN NaN 9.588 -1.926 1951 10 3.924 -2.419 0 0 3.924 -2.419 4.426 -0.905 1951 11 -7.073 -3.086 0 0 -7.073 -3.086 -7.696 -2.697 1951 12 -15.181 -1.348 0 0 -15.181 -1.348 -17.319 -2.474 1952 1 -18.574 0.534 0 0 -18.574 0.534 -21.325 -1.206 1952 2 -10.417 4.752 0 0 -10.417 4.752 -11.764 4.417 1952 3 -7.853 0.075 0 0 -7.853 0.075 -9.938 -0.998 1952 4 8.615 5.445 0 0 8.615 5.445 7.885 5.726 1952 5 11.426 0.070 0 0 11.426 0.070 10.720 0.377 1952 6 16.638 -0.320 0 0 16.638 -0.320 15.708 -0.239 1952 7 18.665 -1.211 0 0 18.665 -1.211 18.362 -0.501 1952 8 18.052 -0.397 0 0 18.052 -0.397 17.241 -0.196 1952 9 14.002 1.475 0 0 14.002 1.475 12.302 0.788 1952 10 5.303 -1.040 0 0 5.303 -1.040 4.912 -0.418 1952 11 -1.945 2.042 0 0 -1.945 2.042 -2.771 2.228 1952 12 -8.197 5.636 0 0 -8.197 5.636 -9.969 4.876 1953 1 -14.715 4.393 0 0 -14.715 4.393 -18.210 1.910 1953 2 -13.366 1.803 0 0 -13.366 1.803 -14.245 1.936 1953 3 -7.453 0.475 0 0 -7.453 0.475 -8.404 0.536 1953 4 1.433 -1.737 0 0 1.433 -1.737 1.219 -0.939 1953 5 10.192 -1.164 0 0 10.192 -1.164 9.842 -0.502 1953 6 16.172 -0.787 0 0 16.172 -0.787 15.224 -0.722 1953 7 18.500 -1.375 0 0 18.500 -1.375 18.341 -0.522 1953 8 19.027 0.579 0 0 19.027 0.579 19.221 1.785 1953 9 12.263 -0.263 0 0 12.263 -0.263 10.565 -0.950 1953 10 9.490 3.148 0 0 9.490 3.148 9.773 4.443 1953 11 0.138 4.125 0 0 0.138 4.125 -0.079 4.920 1953 12 -9.734 4.099 0 0 -9.734 4.099 -12.103 2.742 1954 1 -22.939 -3.831 0 0 -22.939 -3.831 -25.404 -5.285 1954 2 -5.652 9.517 0 0 -5.652 9.517 -6.972 9.209 1954 3 -7.777 0.151 0 0 -7.777 0.151 -10.394 -1.454 1954 4 -0.490 -3.660 0 0 -0.490 -3.660 -0.758 -2.917 1954 5 7.489 -3.867 0 0 7.489 -3.867 7.178 -3.166 1954 6 15.640 -1.318 0 0 15.640 -1.318 14.992 -0.954 1954 7 19.995 0.120 0 0 19.995 0.120 19.368 0.505 1954 8 17.542 -0.907 0 0 17.542 -0.907 16.810 -0.627 1954 9 11.492 -1.035 0 0 11.492 -1.035 10.329 -1.185 1954 10 6.192 -0.151 0 0 6.192 -0.151 6.301 0.970 1954 11 0.092 4.079 0 0 0.092 4.079 -0.794 4.205 1954 12 -6.623 7.210 0 0 -6.623 7.210 -8.881 5.964 1955 1 -16.777 2.330 0 0 -16.777 2.330 -18.992 1.127 1955 2 -16.811 -1.642 0 0 -16.811 -1.642 -17.824 -1.643 1955 3 -13.594 -5.665 0 0 -13.594 -5.665 -15.386 -6.446 1955 4 7.545 4.375 0 0 7.545 4.375 7.025 4.867 1955 5 12.061 0.706 0 0 12.061 0.706 11.615 1.272 1955 6 17.158 0.200 0 0 17.158 0.200 16.591 0.645 1955 7 20.958 1.083 0 0 20.958 1.083 20.813 1.950 1955 8 20.458 2.010 0 0 20.458 2.010 19.816 2.379 1955 9 11.953 -0.573 0 0 11.953 -0.573 10.773 -0.741 1955 10 6.615 0.272 0 0 6.615 0.272 7.226 1.895 1955 11 -9.838 -5.851 0 0 -9.838 -5.851 -9.611 -4.612 1955 12 -18.835 -5.002 0 0 -18.835 -5.002 -19.607 -4.762 1956 1 -17.805 1.303 0 0 -17.805 1.303 -19.111 1.008 1956 2 -16.026 -0.857 0 0 -16.026 -0.857 -16.801 -0.620 1956 3 -10.550 -2.622 0 0 -10.550 -2.622 -12.266 -3.325 1956 4 -1.463 -4.634 0 0 -1.463 -4.634 -1.563 -3.722 1956 5 8.469 -2.886 0 0 8.469 -2.886 7.895 -2.449 1956 6 19.318 2.360 0 0 19.318 2.360 18.576 2.629 1956 7 17.905 -1.971 0 0 17.905 -1.971 17.487 -1.377 1956 8 17.831 -0.618 0 0 17.831 -0.618 17.387 -0.049 1956 9 10.135 -2.391 0 0 10.135 -2.391 8.779 -2.735 1956 10 7.423 1.080 0 0 7.423 1.080 8.179 2.848 1956 11 -2.755 1.232 0 0 -2.755 1.232 -3.398 1.600 1956 12 -13.261 0.572 0 0 -13.261 0.572 -15.261 -0.416 1957 1 -20.023 -0.915 0 0 -20.023 -0.915 -22.894 -2.775 1957 2 -14.921 0.248 0 0 -14.921 0.248 -15.965 0.216 1957 3 -6.134 1.794 0 0 -6.134 1.794 -8.153 0.787 1957 4 3.442 0.271 0 0 3.442 0.271 2.942 0.783 1957 5 12.177 0.822 0 0 12.177 0.822 11.302 0.958 1957 6 14.345 -2.613 0 0 14.345 -2.613 13.384 -2.563 1957 7 21.639 1.763 0 0 21.639 1.763 21.119 2.255 1957 8 17.842 -0.607 0 0 17.842 -0.607 17.390 -0.046 1957 9 11.617 -0.910 0 0 11.617 -0.910 10.239 -1.275 1957 10 6.637 0.294 0 0 6.637 0.294 7.414 2.084 1957 11 -3.627 0.360 0 0 -3.627 0.360 -4.264 0.735 1957 12 -10.353 3.480 0 0 -10.353 3.480 -12.251 2.594 1958 1 -11.381 7.727 0 0 -11.381 7.727 -14.425 5.695 1958 2 -15.284 -0.115 0 0 -15.284 -0.115 -16.092 0.089 1958 3 -3.621 4.307 0 0 -3.621 4.307 -5.318 3.622 1958 4 5.228 2.058 0 0 5.228 2.058 4.889 2.730 1958 5 11.829 0.474 0 0 11.829 0.474 10.940 0.596 1958 6 13.937 -3.022 0 0 13.937 -3.022 13.133 -2.814 1958 7 18.389 -1.487 0 0 18.389 -1.487 17.828 -1.035 1958 8 17.831 -0.618 0 0 17.831 -0.618 17.115 -0.322 1958 9 12.463 -0.063 0 0 12.463 -0.063 11.185 -0.329 1958 10 7.310 0.967 0 0 7.310 0.967 7.414 2.083 1958 11 -4.265 -0.278 0 0 -4.265 -0.278 -4.616 0.383 1958 12 -15.915 -2.081 0 0 -15.915 -2.081 -18.484 -3.639 1959 1 -20.047 -0.939 0 0 -20.047 -0.939 -23.050 -2.930 1959 2 -15.489 -0.320 0 0 -15.489 -0.320 -17.211 -1.030 1959 3 -4.218 3.710 0 0 -4.218 3.710 -6.873 2.067 1959 4 3.462 0.291 0 0 3.462 0.291 2.454 0.296 1959 5 8.632 -2.723 1 0 NaN NaN 8.668 -1.675 1959 6 NaN NaN NaN NaN NaN NaN 16.183 0.237 1959 7 NaN NaN NaN NaN NaN NaN 19.610 0.746 1959 8 NaN NaN NaN NaN NaN NaN 18.652 1.216 1959 9 NaN NaN NaN NaN NaN NaN 10.469 -1.045 1959 10 NaN NaN NaN NaN NaN NaN 2.226 -3.105 1959 11 NaN NaN NaN NaN NaN NaN -9.345 -4.346 1959 12 NaN NaN NaN NaN NaN NaN -8.828 6.017 1960 1 NaN NaN NaN NaN NaN NaN -19.284 0.836 1960 2 NaN NaN NaN NaN NaN NaN -14.810 1.371 1960 3 NaN NaN NaN NaN NaN NaN -12.658 -3.717 1960 4 NaN NaN NaN NaN NaN NaN 1.226 -0.932 1960 5 NaN NaN NaN NaN NaN NaN 11.460 1.116