% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 8824 % Primary Name: EDGEWOOD % Record Type: TAVG % Country: Canada % Latitude: 49.83000 +/- 0.00500 % Longitude: -118.13000 +/- 0.00500 % Elevation (m): 428.00 +/- 0.50 % # of Months: 80 % % IDs: ghcnd - CA001142640 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: 1797df1033f083a4510f4f7fc43183ce % Raw Data Hash: 4cd83d5b57ee4a135696a31c573d6746 % Adj Data Hash: 7a66d955de6a82483fbb9b3c55c953b4 % % 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 11 NaN NaN NaN NaN NaN NaN -6.153 -1.101 1950 12 NaN NaN NaN NaN NaN NaN -6.228 2.858 1951 1 NaN NaN NaN NaN NaN NaN -13.006 -1.414 1951 2 NaN NaN NaN NaN NaN NaN -9.192 -1.616 1951 3 NaN NaN NaN NaN NaN NaN -8.488 -4.142 1951 4 NaN NaN NaN NaN NaN NaN 0.205 -0.761 1951 5 NaN NaN NaN NaN NaN NaN 6.823 0.473 1951 6 NaN NaN NaN NaN NaN NaN 8.817 -1.336 1951 7 NaN NaN NaN NaN NaN NaN 13.729 0.709 1951 8 NaN NaN NaN NaN NaN NaN 11.816 -0.313 1951 9 NaN NaN NaN NaN NaN NaN 7.259 -0.087 1951 10 NaN NaN NaN NaN NaN NaN 0.716 -0.498 1951 11 1.070 0.377 0 0 1.070 0.377 -5.432 -0.380 1951 12 -5.795 -2.455 0 0 -5.795 -2.455 -13.049 -3.963 1952 1 -6.005 -0.159 0 0 -6.005 -0.159 -14.044 -2.452 1952 2 -2.616 -0.785 0 0 -2.616 -0.785 -6.473 1.104 1952 3 1.044 -0.356 0 0 1.044 -0.356 -5.202 -0.856 1952 4 7.375 0.663 0 0 7.375 0.663 1.195 0.228 1952 5 11.426 -0.671 0 0 11.426 -0.671 6.376 0.025 1952 6 13.978 -1.920 0 0 13.978 -1.920 8.667 -1.486 1952 7 17.729 -1.037 0 0 17.729 -1.037 12.397 -0.623 1952 8 17.732 -0.143 0 0 17.732 -0.143 12.390 0.261 1952 9 14.215 1.124 0 0 14.215 1.124 8.761 1.415 1952 10 NaN NaN NaN NaN NaN NaN 3.490 2.276 1952 11 0.430 -0.263 0 0 0.430 -0.263 -5.587 -0.534 1952 12 -0.192 3.148 0 0 -0.192 3.148 -6.319 2.767 1953 1 1.229 7.075 0 0 1.229 7.075 -7.343 4.249 1953 2 0.125 1.956 0 0 0.125 1.956 -4.437 3.140 1953 3 3.282 1.882 0 0 3.282 1.882 -2.943 1.403 1953 4 6.188 -0.524 0 0 6.188 -0.524 -0.455 -1.421 1953 5 11.632 -0.464 0 0 11.632 -0.464 6.656 0.305 1953 6 14.093 -1.805 0 0 14.093 -1.805 8.699 -1.454 1953 7 17.366 -1.400 0 0 17.366 -1.400 12.069 -0.952 1953 8 17.300 -0.575 0 0 17.300 -0.575 12.229 0.100 1953 9 11.090 -2.001 0 0 11.090 -2.001 7.239 -0.107 1953 10 6.887 -0.073 0 0 6.887 -0.073 2.824 1.610 1953 11 2.677 1.983 0 0 2.677 1.983 -2.186 2.866 1953 12 -0.055 3.285 0 0 -0.055 3.285 -5.874 3.212 1954 1 -6.856 -1.010 0 0 -6.856 -1.010 -14.724 -3.132 1954 2 1.129 2.959 0 0 1.129 2.959 -3.387 4.190 1954 3 0.648 -0.751 0 0 0.648 -0.751 -6.506 -2.160 1954 4 5.133 -1.579 0 0 5.133 -1.579 -2.510 -3.476 1954 5 11.835 -0.261 0 0 11.835 -0.261 6.048 -0.302 1954 6 13.045 -2.854 0 0 13.045 -2.854 7.725 -2.428 1954 7 16.735 -2.031 0 0 16.735 -2.031 11.570 -1.450 1954 8 16.058 -1.817 0 0 16.058 -1.817 10.807 -1.322 1954 9 12.347 -0.745 0 0 12.347 -0.745 7.294 -0.052 1954 10 4.790 -2.170 0 0 4.790 -2.170 0.234 -0.980 1954 11 4.614 3.921 1 0 NaN NaN -1.065 3.987 1954 12 -0.752 2.589 0 0 -0.752 2.589 -6.622 2.464 1955 1 -2.813 3.033 0 0 -2.813 3.033 -9.909 1.683 1955 2 -4.704 -2.873 0 0 -4.704 -2.873 -9.219 -1.643 1955 3 -3.374 -4.774 0 0 -3.374 -4.774 -9.667 -5.321 1955 4 4.743 -1.969 0 0 4.743 -1.969 -1.284 -2.250 1955 5 9.861 -2.235 0 0 9.861 -2.235 4.155 -2.195 1955 6 14.877 -1.022 0 0 14.877 -1.022 9.671 -0.482 1955 7 17.426 -1.340 0 0 17.426 -1.340 12.436 -0.585 1955 8 16.634 -1.241 0 0 16.634 -1.241 11.756 -0.373 1955 9 12.420 -0.671 0 0 12.420 -0.671 7.518 0.172 1955 10 6.802 -0.158 0 0 6.802 -0.158 1.748 0.534 1955 11 -3.107 -3.800 0 0 -3.107 -3.800 -11.118 -6.065 1955 12 -5.674 -2.334 0 0 -5.674 -2.334 -11.998 -2.911 1956 1 -3.895 1.951 0 0 -3.895 1.951 -11.285 0.307 1956 2 -6.479 -4.648 0 0 -6.479 -4.648 -11.281 -3.705 1956 3 0.094 -1.306 0 0 0.094 -1.306 -6.213 -1.866 1956 4 7.535 0.823 0 0 7.535 0.823 0.818 -0.149 1956 5 12.752 0.655 0 0 12.752 0.655 7.374 1.024 1956 6 13.895 -2.004 0 0 13.895 -2.004 8.461 -1.692 1956 7 18.706 -0.060 0 0 18.706 -0.060 13.933 0.913 1956 8 18.090 0.215 0 0 18.090 0.215 13.102 0.972 1956 9 13.155 0.064 0 0 13.155 0.064 7.719 0.373 1956 10 6.850 -0.110 0 0 6.850 -0.110 1.269 0.055 1956 11 -0.188 -0.882 0 0 -0.188 -0.882 -5.907 -0.854 1956 12 -3.335 0.005 0 0 -3.335 0.005 -9.299 -0.213 1957 1 -11.774 -5.928 0 0 -11.774 -5.928 -19.069 -7.477 1957 2 -5.693 -3.862 0 0 -5.693 -3.862 -10.588 -3.011 1957 3 1.119 -0.280 0 0 1.119 -0.280 -4.792 -0.446 1957 4 7.415 0.703 0 0 7.415 0.703 0.854 -0.112 1957 5 14.671 2.575 0 0 14.671 2.575 9.255 2.905 1957 6 15.645 -0.254 0 0 15.645 -0.254 9.883 -0.270 1957 7 17.068 -1.698 0 0 17.068 -1.698 11.568 -1.452 1957 8 14.847 -3.028 0 0 14.847 -3.028 9.756 -2.374 1957 9 14.138 1.047 0 0 14.138 1.047 8.591 1.246 1957 10 5.542 -1.418 0 0 5.542 -1.418 0.308 -0.906 1957 11 1.428 0.735 0 0 1.428 0.735 -4.219 0.833 1957 12 -0.247 3.094 0 0 -0.247 3.094 -5.571 3.515 1958 1 -0.229 5.617 0 0 -0.229 5.617 -6.963 4.629 1958 2 1.420 3.251 0 0 1.420 3.251 -3.542 4.035 1958 3 3.590 2.191 0 0 3.590 2.191 -3.586 0.760 1958 4 7.508 0.796 0 0 7.508 0.796 0.805 -0.161 1958 5 15.250 3.154 0 0 15.250 3.154 9.623 3.272 1958 6 17.435 1.536 0 0 17.435 1.536 12.371 2.218 1958 7 NaN NaN NaN NaN NaN NaN 14.883 1.862 1958 8 20.792 2.917 1 0 NaN NaN 14.382 2.253 1958 9 NaN NaN NaN NaN NaN NaN 7.209 -0.137 1958 10 NaN NaN NaN NaN NaN NaN 1.577 0.363 1958 11 NaN NaN NaN NaN NaN NaN -6.632 -1.580 1958 12 NaN NaN NaN NaN NaN NaN -7.671 1.415 1959 1 NaN NaN NaN NaN NaN NaN -11.158 0.434 1959 2 NaN NaN NaN NaN NaN NaN -8.492 -0.916 1959 3 NaN NaN NaN NaN NaN NaN -3.621 0.725 1959 4 NaN NaN NaN NaN NaN NaN 0.402 -0.564 1959 5 NaN NaN NaN NaN NaN NaN 4.885 -1.465 1959 6 NaN NaN NaN NaN NaN NaN 9.083 -1.070 1959 7 NaN NaN NaN NaN NaN NaN 13.268 0.248 1959 8 NaN NaN NaN NaN NaN NaN 10.242 -1.887