% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 7375 % Primary Name: MONT TREMBLANT INTL % Record Type: TAVG % Country: Canada % State: QC % Latitude: 46.40000 +/- 0.00050 % Longitude: -74.76700 +/- 0.00050 % Elevation (m): 252.00 +/- 0.05 % # of Months: 287 % % IDs: ghcnd - CA002100100 % gsod - 710351-99999 % icao - CYFJ % usaf - 710351 % % Sources: Global Historical Climatology Network - Daily % Global Summary of the Day % % Site Hash: 11114d76475d9d1d9cf9eefd3daf65ba % Raw Data Hash: 0c6591d19a2858ada1dd484618eca395 % Adj Data Hash: c7e568550067479b2762a6f6cf3b36c2 % % 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 1941 9 NaN NaN NaN NaN NaN NaN 13.562 0.576 1941 10 NaN NaN NaN NaN NaN NaN 6.341 -0.501 1941 11 NaN NaN NaN NaN NaN NaN 1.258 1.067 1941 12 NaN NaN NaN NaN NaN NaN -8.123 0.914 1942 1 NaN NaN NaN NaN NaN NaN -12.087 0.228 1942 2 NaN NaN NaN NaN NaN NaN -10.754 0.123 1942 3 NaN NaN NaN NaN NaN NaN -0.734 3.315 1942 4 NaN NaN NaN NaN NaN NaN 6.303 2.224 1942 5 NaN NaN NaN NaN NaN NaN 13.186 1.762 1942 6 NaN NaN NaN NaN NaN NaN 17.101 0.470 1942 7 NaN NaN NaN NaN NaN NaN 18.454 -0.611 1942 8 NaN NaN NaN NaN NaN NaN 17.462 -0.293 1942 9 7.068 0.647 0 0 7.068 0.647 12.935 -0.052 1942 10 -0.790 -1.067 1 0 NaN NaN 7.635 0.792 1942 11 -18.889 -12.515 1 0 NaN NaN 0.600 0.408 1942 12 -29.973 -14.371 1 0 NaN NaN -12.437 -3.400 1943 1 -25.052 -6.172 0 0 -25.052 -6.172 -15.217 -2.903 1943 2 -15.558 1.885 0 0 -15.558 1.885 -10.027 0.850 1943 3 -13.882 -3.267 0 0 -13.882 -3.267 -6.648 -2.598 1943 4 -11.482 -8.996 1 0 NaN NaN -0.074 -4.153 1943 5 NaN NaN NaN NaN NaN NaN 10.812 -0.611 1943 6 11.086 1.020 1 0 NaN NaN 16.826 0.195 1943 7 11.334 -1.166 1 0 NaN NaN 19.419 0.354 1943 8 9.142 -2.048 1 0 NaN NaN 17.146 -0.609 1943 9 5.460 -0.961 1 0 NaN NaN 11.694 -1.292 1943 10 -2.737 -3.014 1 0 NaN NaN 7.126 0.283 1943 11 -7.577 -1.203 0 0 -7.577 -1.203 0.548 0.357 1943 12 -9.332 6.270 0 0 -9.332 6.270 -12.584 -3.547 1944 1 -13.315 5.565 0 0 -13.315 5.565 -9.066 3.249 1944 2 -13.024 4.418 0 0 -13.024 4.418 -11.711 -0.834 1944 3 -10.369 0.245 0 0 -10.369 0.245 -6.628 -2.578 1944 4 -3.922 -1.436 0 0 -3.922 -1.436 2.049 -2.031 1944 5 5.205 0.346 0 0 5.205 0.346 14.469 3.046 1944 6 10.487 0.421 0 0 10.487 0.421 16.736 0.104 1944 7 11.969 -0.530 1 0 NaN NaN 19.877 0.812 1944 8 9.656 -1.533 1 0 NaN NaN 19.931 2.176 1944 9 5.655 -0.766 1 0 NaN NaN 13.758 0.771 1944 10 -1.469 -1.747 1 0 NaN NaN 6.464 -0.378 1944 11 -12.625 -6.252 1 0 NaN NaN 1.763 1.571 1944 12 -15.616 -0.014 0 0 -15.616 -0.014 -12.147 -3.110 1945 1 -14.656 4.223 0 0 -14.656 4.223 -16.146 -3.832 1945 2 -13.064 4.378 0 0 -13.064 4.378 -9.162 1.715 1945 3 -9.100 1.515 0 0 -9.100 1.515 1.579 5.628 1945 4 -6.793 -4.307 1 0 NaN NaN 7.250 3.171 1945 5 4.505 -0.354 0 0 4.505 -0.354 9.268 -2.156 1945 6 8.577 -1.489 1 0 NaN NaN 15.867 -0.764 1945 7 10.532 -1.967 1 0 NaN NaN 18.845 -0.220 1945 8 10.250 -0.940 1 0 NaN NaN 18.405 0.650 1945 9 3.290 -3.131 1 0 NaN NaN 13.872 0.886 1945 10 -1.903 -2.180 1 0 NaN NaN 6.172 -0.670 1945 11 -19.342 -12.968 1 0 NaN NaN 0.711 0.519 1945 12 -20.445 -4.843 0 0 -20.445 -4.843 -11.074 -2.037 1946 1 -19.435 -0.556 0 0 -19.435 -0.556 -11.873 0.441 1946 2 -14.452 2.991 0 0 -14.452 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