% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 38547 % Primary Name: BROOKFIELD % Record Type: TAVG % Country: United States % State: NY % Latitude: 42.80000 +/- 0.00005 % Longitude: -75.33330 +/- 0.00005 % Elevation (m): 396.24 +/- 0.15 % # of Months: 46 % % Alternate Names: Missing Station ID - 300957 % % IDs: coop - 300957 % ghcnd - USC00300957 % ncdc - 12003762 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 609db50142accfc004dffbcea77c5c02 % Raw Data Hash: b0bc694c65e57722dc9e200562de43c6 % Adj Data Hash: bcceecf85f6d9aa1855c3137e9ed7335 % % 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 1892 1 NaN NaN NaN NaN NaN NaN -6.323 -0.838 1892 2 NaN NaN NaN NaN NaN NaN -3.906 0.913 1892 3 NaN NaN NaN NaN NaN NaN -3.207 -3.481 1892 4 NaN NaN NaN NaN NaN NaN 5.975 -1.034 1892 5 NaN NaN NaN NaN NaN NaN 11.449 -1.673 1892 6 NaN NaN NaN NaN NaN NaN 19.377 1.075 1892 7 NaN NaN NaN NaN NaN NaN 20.088 -0.740 1892 8 NaN NaN NaN NaN NaN NaN 19.533 -0.340 1892 9 NaN NaN NaN NaN NaN NaN 15.031 -0.897 1892 10 NaN NaN NaN NaN NaN NaN 8.623 -1.151 1892 11 NaN NaN NaN NaN NaN NaN 2.492 -1.427 1892 12 NaN NaN NaN NaN NaN NaN -4.833 -2.117 1893 1 -9.403 -3.766 0 0 -9.403 -3.766 -9.592 -4.107 1893 2 -7.650 -2.680 0 0 -7.650 -2.680 -6.839 -2.021 1893 3 -2.463 -2.585 0 0 -2.463 -2.585 -1.397 -1.671 1893 4 4.517 -2.340 1 0 NaN NaN 5.591 -1.418 1893 5 11.505 -1.464 0 0 11.505 -1.464 12.204 -0.918 1893 6 19.241 1.091 0 0 19.241 1.091 19.567 1.265 1893 7 19.194 -1.482 0 0 19.194 -1.482 20.086 -0.742 1893 8 19.086 -0.634 0 0 19.086 -0.634 19.321 -0.552 1893 9 13.463 -2.313 0 0 13.463 -2.313 13.517 -2.411 1893 10 8.552 -1.070 0 0 8.552 -1.070 9.914 0.140 1893 11 1.230 -2.537 0 0 1.230 -2.537 2.848 -1.071 1893 12 -5.511 -2.643 1 0 NaN NaN -3.763 -1.047 1894 1 -4.037 1.600 0 0 -4.037 1.600 -2.770 2.715 1894 2 -6.944 -1.974 1 0 NaN NaN -6.948 -2.130 1894 3 1.613 1.491 0 0 1.613 1.491 3.284 3.010 1894 4 5.708 -1.149 0 0 5.708 -1.149 6.694 -0.314 1894 5 12.007 -0.962 0 0 12.007 -0.962 12.875 -0.246 1894 6 18.621 0.471 0 0 18.621 0.471 18.786 0.484 1894 7 20.506 -0.170 0 0 20.506 -0.170 21.150 0.322 1894 8 17.670 -2.050 0 0 17.670 -2.050 18.116 -1.757 1894 9 17.321 1.546 0 0 17.321 1.546 17.411 1.483 1894 10 10.036 0.414 0 0 10.036 0.414 10.362 0.588 1894 11 0.889 -2.878 0 0 0.889 -2.878 1.766 -2.153 1894 12 -2.389 0.479 0 0 -2.389 0.479 -2.183 0.533 1895 1 -5.878 -0.241 0 0 -5.878 -0.241 -7.227 -1.742 1895 2 -9.209 -4.239 1 0 NaN NaN -9.111 -4.292 1895 3 -3.924 -4.046 0 0 -3.924 -4.046 -2.966 -3.240 1895 4 6.759 -0.097 0 0 6.759 -0.097 6.945 -0.064 1895 5 14.714 1.744 0 0 14.714 1.744 14.307 1.186 1895 6 22.375 4.226 0 0 22.375 4.226 20.301 1.999 1895 7 21.705 1.030 0 0 21.705 1.030 18.768 -2.059 1895 8 20.047 0.327 0 0 20.047 0.327 19.700 -0.173 1895 9 17.677 1.901 0 0 17.677 1.901 17.106 1.178 1895 10 7.917 -1.704 0 0 7.917 -1.704 6.280 -3.494 1895 11 4.144 0.377 0 0 4.144 0.377 4.465 0.546 1895 12 -1.863 1.005 0 0 -1.863 1.005 -1.374 1.342 1896 1 -6.667 -1.030 0 0 -6.667 -1.030 -6.684 -1.199 1896 2 -4.932 0.039 0 0 -4.932 0.039 -5.308 -0.490 1896 3 -3.747 -3.868 0 0 -3.747 -3.868 -4.441 -4.715 1896 4 11.575 4.719 1 0 NaN NaN 9.377 2.369 1896 5 15.068 2.099 0 0 15.068 2.099 15.794 2.673 1896 6 17.121 -1.029 0 0 17.121 -1.029 17.640 -0.662 1896 7 22.189 1.514 1 0 NaN NaN 20.943 0.115 1896 8 20.916 1.196 0 0 20.916 1.196 19.987 0.115 1896 9 13.718 -2.057 0 0 13.718 -2.057 14.973 -0.955 1896 10 8.771 -0.851 0 0 8.771 -0.851 7.321 -2.453 1896 11 NaN NaN NaN NaN NaN NaN 6.203 2.284 1896 12 NaN NaN NaN NaN NaN NaN -3.965 -1.249 1897 1 NaN NaN NaN NaN NaN NaN -5.853 -0.368 1897 2 NaN NaN NaN NaN NaN NaN -4.318 0.500 1897 3 NaN NaN NaN NaN NaN NaN 0.662 0.388 1897 4 NaN NaN NaN NaN NaN NaN 7.190 0.182 1897 5 NaN NaN NaN NaN NaN NaN 12.190 -0.932 1897 6 NaN NaN NaN NaN NaN NaN 15.697 -2.605 1897 7 NaN NaN NaN NaN NaN NaN 21.923 1.095 1897 8 NaN NaN NaN NaN NaN NaN 18.228 -1.645 1897 9 NaN NaN NaN NaN NaN NaN 15.590 -0.338 1897 10 NaN NaN NaN NaN NaN NaN 10.352 0.578