% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 38195 % Primary Name: DEERFIELD % Record Type: TAVG % Country: United States % State: MA % Latitude: 42.51667 +/- 0.00833 % Longitude: -72.61667 +/- 0.00833 % Elevation (m): 53.34 +/- 0.15 % # of Months: 82 % % Alternate Names: Missing Station ID - 191860 % % IDs: coop - 191860 % ncdc - 12002401 % % Sources: US Cooperative Summary of the Day % Multi-network Metadata System % % Site Hash: e7e98a0d6104ee0b48d6b571c341f49a % Raw Data Hash: bcb45e1f718ba7cee9f199f057131f0c % Adj Data Hash: 3c70e6c3ac35f9c2350f7a56282fb20d % % 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 1884 4 NaN NaN NaN NaN NaN NaN 5.692 -1.314 1884 5 NaN NaN NaN NaN NaN NaN 11.843 -1.391 1884 6 NaN NaN NaN NaN NaN NaN 18.324 0.030 1884 7 NaN NaN NaN NaN NaN NaN 18.834 -2.154 1884 8 NaN NaN NaN NaN NaN NaN 19.144 -0.685 1884 9 NaN NaN NaN NaN NaN NaN 16.410 0.979 1884 10 NaN NaN NaN NaN NaN NaN 8.755 -0.642 1884 11 NaN NaN NaN NaN NaN NaN 2.764 -0.905 1884 12 NaN NaN NaN NaN NaN NaN -3.666 -0.327 1885 1 NaN NaN NaN NaN NaN NaN -6.351 -0.606 1885 2 NaN NaN NaN NaN NaN NaN -10.298 -5.631 1885 3 NaN NaN NaN NaN NaN NaN -5.276 -5.859 1885 4 7.537 -0.832 0 0 7.537 -0.832 6.731 -0.275 1885 5 13.961 -0.636 0 0 13.961 -0.636 11.734 -1.499 1885 6 19.352 -0.306 0 0 19.352 -0.306 17.992 -0.303 1885 7 22.168 -0.182 0 0 22.168 -0.182 21.071 0.083 1885 8 19.319 -1.873 0 0 19.319 -1.873 18.309 -1.520 1885 9 14.907 -1.887 0 0 14.907 -1.887 13.398 -2.034 1885 10 9.265 -1.495 0 0 9.265 -1.495 8.454 -0.944 1885 11 4.148 -0.884 0 0 4.148 -0.884 3.921 0.252 1885 12 -1.828 0.148 0 0 -1.828 0.148 -3.553 -0.214 1886 1 -6.201 -1.819 0 0 -6.201 -1.819 -6.644 -0.899 1886 2 -4.444 -1.140 1 0 NaN NaN -6.373 -1.706 1886 3 0.376 -1.570 0 0 0.376 -1.570 -1.035 -1.618 1886 4 10.000 1.631 0 0 10.000 1.631 8.599 1.593 1886 5 14.462 -0.134 0 0 14.462 -0.134 12.725 -0.508 1886 6 NaN NaN NaN NaN NaN NaN 16.431 -1.864 1886 7 21.523 -0.827 0 0 21.523 -0.827 20.188 -0.799 1886 8 NaN NaN NaN NaN NaN NaN 18.696 -1.133 1886 9 16.519 -0.276 0 0 16.519 -0.276 14.946 -0.485 1886 10 9.964 -0.796 0 0 9.964 -0.796 8.804 -0.594 1886 11 3.611 -1.421 0 0 3.611 -1.421 3.665 -0.004 1886 12 -4.677 -2.701 0 0 -4.677 -2.701 -6.371 -3.032 1887 1 -7.056 -2.674 0 0 -7.056 -2.674 -7.848 -2.103 1887 2 -3.948 -0.644 0 0 -3.948 -0.644 -5.191 -0.524 1887 3 -1.398 -3.344 0 0 -1.398 -3.344 -2.906 -3.489 1887 4 5.093 -3.276 0 0 5.093 -3.276 4.677 -2.329 1887 5 17.814 3.217 0 0 17.814 3.217 15.091 1.858 1887 6 19.722 0.064 0 0 19.722 0.064 17.661 -0.634 1887 7 24.606 2.255 0 0 24.606 2.255 22.781 1.794 1887 8 19.337 -1.855 0 0 19.337 -1.855 17.970 -1.859 1887 9 14.426 -2.369 0 0 14.426 -2.369 12.907 -2.524 1887 10 8.943 -1.818 0 0 8.943 -1.818 7.870 -1.528 1887 11 2.037 -2.995 0 0 2.037 -2.995 2.739 -0.929 1887 12 -2.849 -0.873 0 0 -2.849 -0.873 -4.037 -0.698 1888 1 -9.946 -5.565 0 0 -9.946 -5.565 -10.786 -5.042 1888 2 -5.441 -2.137 0 0 -5.441 -2.137 -6.124 -1.457 1888 3 -2.278 -4.224 0 0 -2.278 -4.224 -3.044 -3.627 1888 4 5.222 -3.147 0 0 5.222 -3.147 3.926 -3.080 1888 5 14.014 -0.582 0 0 14.014 -0.582 11.354 -1.879 1888 6 20.148 0.490 0 0 20.148 0.490 18.038 -0.257 1888 7 20.735 -1.615 0 0 20.735 -1.615 18.797 -2.190 1888 8 20.717 -0.475 0 0 20.717 -0.475 19.075 -0.754 1888 9 15.204 -1.591 0 0 15.204 -1.591 13.310 -2.122 1888 10 6.398 -4.363 0 0 6.398 -4.363 5.547 -3.851 1888 11 3.796 -1.235 0 0 3.796 -1.235 3.696 0.027 1888 12 -0.878 1.098 0 0 -0.878 1.098 -2.942 0.397 1889 1 -1.237 3.145 0 0 -1.237 3.145 -2.272 3.472 1889 2 -6.071 -2.767 0 0 -6.071 -2.767 -7.276 -2.609 1889 3 2.849 0.904 0 0 2.849 0.904 1.103 0.520 1889 4 9.463 1.094 0 0 9.463 1.094 7.716 0.710 1889 5 16.685 2.088 0 0 16.685 2.088 14.543 1.310 1889 6 20.833 1.175 0 0 20.833 1.175 18.682 0.387 1889 7 21.434 -0.917 0 0 21.434 -0.917 19.688 -1.299 1889 8 19.211 -1.980 0 0 19.211 -1.980 17.871 -1.958 1889 9 17.407 0.613 0 0 17.407 0.613 15.345 -0.087 1889 10 7.921 -2.839 0 0 7.921 -2.839 6.737 -2.660 1889 11 4.833 -0.198 0 0 4.833 -0.198 4.559 0.890 1889 12 0.556 2.532 0 0 0.556 2.532 -1.033 2.306 1890 1 -0.591 3.790 0 0 -0.591 3.790 -2.903 2.842 1890 2 -0.655 2.649 0 0 -0.655 2.649 -2.397 2.270 1890 3 -0.573 -2.519 0 0 -0.573 -2.519 -1.478 -2.061 1890 4 NaN NaN NaN NaN NaN NaN 6.251 -0.755 1890 5 14.032 -0.564 0 0 14.032 -0.564 12.619 -0.614 1890 6 19.519 -0.139 0 0 19.519 -0.139 16.997 -1.298 1890 7 21.523 -0.827 0 0 21.523 -0.827 19.908 -1.079 1890 8 20.233 -0.959 0 0 20.233 -0.959 18.722 -1.106 1890 9 16.037 -0.758 0 0 16.037 -0.758 14.863 -0.569 1890 10 9.677 -1.083 0 0 9.677 -1.083 7.706 -1.691 1890 11 2.574 -2.458 0 0 2.574 -2.458 2.446 -1.222 1890 12 -5.932 -3.956 0 0 -5.932 -3.956 -7.944 -4.605 1891 1 -3.405 0.977 0 0 -3.405 0.977 -4.531 1.214 1891 2 -2.401 0.903 0 0 -2.401 0.903 -3.565 1.102 1891 3 0.215 -1.731 0 0 0.215 -1.731 -1.021 -1.604 1891 4 8.944 0.576 0 0 8.944 0.576 7.426 0.421 1891 5 14.158 -0.438 0 0 14.158 -0.438 11.938 -1.296 1891 6 20.037 0.379 0 0 20.037 0.379 17.406 -0.889 1891 7 20.036 -2.314 0 0 20.036 -2.314 18.712 -2.275 1891 8 21.290 0.099 0 0 21.290 0.099 19.611 -0.217 1891 9 18.556 1.761 0 0 18.556 1.761 17.027 1.595 1891 10 8.943 -1.818 0 0 8.943 -1.818 7.899 -1.498 1891 11 2.389 -2.643 0 0 2.389 -2.643 2.676 -0.993 1891 12 1.900 3.876 0 0 1.900 3.876 0.409 3.748 1892 1 -4.695 -0.314 0 0 -4.695 -0.314 -5.608 0.137 1892 2 -3.410 -0.106 0 0 -3.410 -0.106 -4.690 -0.023 1892 3 -0.426 -2.372 0 0 -0.426 -2.372 -1.887 -2.470 1892 4 7.889 -0.480 0 0 7.889 -0.480 6.668 -0.338 1892 5 NaN NaN NaN NaN NaN NaN 11.756 -1.477 1892 6 NaN NaN NaN NaN NaN NaN 19.636 1.341 1892 7 NaN NaN NaN NaN NaN NaN 20.731 -0.256 1892 8 NaN NaN NaN NaN NaN NaN 19.502 -0.327 1892 9 NaN NaN NaN NaN NaN NaN 14.400 -1.032 1892 10 NaN NaN NaN NaN NaN NaN 8.379 -1.018 1892 11 NaN NaN NaN NaN NaN NaN 2.808 -0.861 1892 12 NaN NaN NaN NaN NaN NaN -5.351 -2.012 1893 1 NaN NaN NaN NaN NaN NaN -10.011 -4.266 1893 2 NaN NaN NaN NaN NaN NaN -6.301 -1.634 1893 3 NaN NaN NaN NaN NaN NaN -1.588 -2.171 1893 4 NaN NaN NaN NaN NaN NaN 4.902 -2.104