% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 6342 % Primary Name: OIL CITY % Record Type: TAVG % Country: Canada % Latitude: 42.92000 +/- 0.00500 % Longitude: -82.03000 +/- 0.00500 % Elevation (m): 208.00 +/- 0.50 % # of Months: 73 % % IDs: ghcnd - CA006125766 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: de0f8a0937c75de8dc21d2a3868beb78 % Raw Data Hash: d901e681eb3be94c327102bddb6f0f90 % Adj Data Hash: 2b5fdbea254f2a5416c89105b4f46bc1 % % 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 1952 11 NaN NaN NaN NaN NaN NaN 5.531 1.465 1952 12 NaN NaN NaN NaN NaN NaN -0.171 2.263 1953 1 NaN NaN NaN NaN NaN NaN -2.336 3.058 1953 2 NaN NaN NaN NaN NaN NaN -1.375 2.814 1953 3 NaN NaN NaN NaN NaN NaN 2.580 1.605 1953 4 NaN NaN NaN NaN NaN NaN 6.518 -1.288 1953 5 NaN NaN NaN NaN NaN NaN 14.353 0.253 1953 6 NaN NaN NaN NaN NaN NaN 20.807 1.113 1953 7 NaN NaN NaN NaN NaN NaN 22.330 0.124 1953 8 NaN NaN NaN NaN NaN NaN 22.138 0.844 1953 9 NaN NaN NaN NaN NaN NaN 17.559 0.291 1953 10 NaN NaN NaN NaN NaN NaN 12.926 2.115 1953 11 6.054 2.992 1 0 NaN NaN 6.266 2.200 1953 12 -0.913 2.525 0 0 -0.913 2.525 -0.500 1.935 1954 1 -5.516 0.880 0 0 -5.516 0.880 -4.837 0.556 1954 2 -0.616 4.577 0 0 -0.616 4.577 -0.328 3.862 1954 3 -1.427 -1.399 0 0 -1.427 -1.399 0.076 -0.898 1954 4 8.513 1.711 0 0 8.513 1.711 9.614 1.809 1954 5 10.884 -2.213 0 0 10.884 -2.213 11.766 -2.334 1954 6 20.172 1.480 0 0 20.172 1.480 21.087 1.392 1954 7 19.981 -1.221 1 0 NaN NaN 21.344 -0.861 1954 8 19.063 -1.228 0 0 19.063 -1.228 20.453 -0.841 1954 9 16.252 -0.014 0 0 16.252 -0.014 17.926 0.658 1954 10 11.089 1.280 0 0 11.089 1.280 11.892 1.081 1954 11 4.262 1.199 0 0 4.262 1.199 4.761 0.696 1954 12 -2.994 0.444 0 0 -2.994 0.444 -2.603 -0.168 1955 1 -5.332 1.064 0 0 -5.332 1.064 -4.777 0.617 1955 2 -4.107 1.085 0 0 -4.107 1.085 -3.632 0.557 1955 3 0.300 0.329 0 0 0.300 0.329 1.347 0.373 1955 4 10.237 3.434 0 0 10.237 3.434 11.805 4.000 1955 5 14.271 1.175 0 0 14.271 1.175 15.496 1.397 1955 6 17.870 -0.821 0 0 17.870 -0.821 19.346 -0.348 1955 7 24.300 3.098 0 0 24.300 3.098 25.030 2.825 1955 8 22.790 2.500 0 0 22.790 2.500 23.683 2.390 1955 9 16.378 0.113 0 0 16.378 0.113 18.010 0.742 1955 10 11.065 1.256 0 0 11.065 1.256 12.317 1.505 1955 11 1.745 -1.318 0 0 1.745 -1.318 2.767 -1.298 1955 12 -4.387 -0.950 0 0 -4.387 -0.950 -3.837 -1.403 1956 1 -4.869 1.527 0 0 -4.869 1.527 -4.699 0.694 1956 2 -4.595 0.598 0 0 -4.595 0.598 -3.630 0.560 1956 3 -1.668 -1.639 0 0 -1.668 -1.639 -0.436 -1.410 1956 4 5.577 -1.226 0 0 5.577 -1.226 6.838 -0.967 1956 5 11.403 -1.693 0 0 11.403 -1.693 12.582 -1.517 1956 6 18.417 -0.275 0 0 18.417 -0.275 20.146 0.452 1956 7 20.027 -1.175 1 0 NaN NaN 21.163 -1.042 1956 8 20.048 -0.242 0 0 20.048 -0.242 20.950 -0.343 1956 9 13.782 -2.484 0 0 13.782 -2.484 15.383 -1.885 1956 10 12.500 2.692 0 0 12.500 2.692 13.460 2.649 1956 11 3.620 0.557 0 0 3.620 0.557 4.517 0.451 1956 12 -0.063 3.375 0 0 -0.063 3.375 0.057 2.491 1957 1 -8.874 -2.478 0 0 -8.874 -2.478 -7.740 -2.346 1957 2 -3.629 1.564 0 0 -3.629 1.564 -2.482 1.707 1957 3 0.890 0.919 0 0 0.890 0.919 1.677 0.703 1957 4 8.043 1.241 0 0 8.043 1.241 8.876 1.071 1957 5 11.856 -1.240 0 0 11.856 -1.240 12.862 -1.237 1957 6 19.078 0.387 0 0 19.078 0.387 20.088 0.393 1957 7 20.366 -0.836 0 0 20.366 -0.836 21.909 -0.296 1957 8 18.798 -1.492 0 0 18.798 -1.492 20.468 -0.826 1957 9 15.497 -0.769 0 0 15.497 -0.769 16.822 -0.446 1957 10 9.140 -0.668 0 0 9.140 -0.668 9.943 -0.869 1957 11 3.853 0.791 0 0 3.853 0.791 4.588 0.523 1957 12 -0.676 2.762 0 0 -0.676 2.762 -0.220 2.215 1958 1 -4.531 1.866 0 0 -4.531 1.866 -4.485 0.909 1958 2 -7.068 -1.875 0 0 -7.068 -1.875 -6.590 -2.400 1958 3 1.037 1.066 0 0 1.037 1.066 1.678 0.704 1958 4 8.105 1.303 0 0 8.105 1.303 9.094 1.288 1958 5 12.410 -0.687 0 0 12.410 -0.687 13.638 -0.461 1958 6 15.675 -3.016 0 0 15.675 -3.016 17.151 -2.544 1958 7 20.803 -0.399 0 0 20.803 -0.399 21.898 -0.307 1958 8 19.147 -1.144 0 0 19.147 -1.144 20.782 -0.512 1958 9 15.797 -0.469 0 0 15.797 -0.469 17.274 0.006 1958 10 10.716 0.908 0 0 10.716 0.908 11.980 1.169 1958 11 4.308 1.246 0 0 4.308 1.246 5.494 1.429 1958 12 -7.632 -4.195 0 0 -7.632 -4.195 -6.979 -4.544 1959 1 -8.087 -1.691 0 0 -8.087 -1.691 -7.642 -2.248 1959 2 -5.934 -0.741 0 0 -5.934 -0.741 -5.085 -0.895 1959 3 -0.556 -0.528 0 0 -0.556 -0.528 0.423 -0.551 1959 4 8.139 1.336 1 0 NaN NaN 8.691 0.886 1959 5 14.594 1.497 0 0 14.594 1.497 15.813 1.713 1959 6 18.315 -0.376 0 0 18.315 -0.376 20.382 0.688 1959 7 21.252 0.050 0 0 21.252 0.050 22.471 0.265 1959 8 22.585 2.295 0 0 22.585 2.295 23.798 2.505 1959 9 17.938 1.673 0 0 17.938 1.673 19.041 1.773 1959 10 9.685 -0.123 0 0 9.685 -0.123 10.603 -0.208 1959 11 1.543 -1.519 0 0 1.543 -1.519 2.141 -1.925 1959 12 NaN NaN NaN NaN NaN NaN -0.219 2.216 1960 1 NaN NaN NaN NaN NaN NaN -3.473 1.920 1960 2 NaN NaN NaN NaN NaN NaN -3.819 0.371 1960 3 NaN NaN NaN NaN NaN NaN -4.287 -5.262 1960 4 NaN NaN NaN NaN NaN NaN 9.510 1.704 1960 5 NaN NaN NaN NaN NaN NaN 13.581 -0.518 1960 6 NaN NaN NaN NaN NaN NaN 18.808 -0.887 1960 7 NaN NaN NaN NaN NaN NaN 20.871 -1.334 1960 8 NaN NaN NaN NaN NaN NaN 21.278 -0.016 1960 9 NaN NaN NaN NaN NaN NaN 18.821 1.553 1960 10 NaN NaN NaN NaN NaN NaN 11.095 0.284 1960 11 NaN NaN NaN NaN NaN NaN 5.824 1.759