% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 35898 % Primary Name: LEXINGTON % Record Type: TAVG % Country: United States % State: IL % Latitude: 40.64140 +/- 0.00005 % Longitude: -88.78330 +/- 0.00005 % Elevation (m): 228.90 +/- 0.15 % # of Months: 44 % % Alternate Names: Missing Station ID - 115043 % % IDs: coop - 115043 % ghcnd - USC00115043 % ncdc - 12001713 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 507b3f03d221347f22d929fad86aca71 % Raw Data Hash: 8c1f4ca58d57140cd66e1361fa0c9b3b % Adj Data Hash: 7c667f0b2aad4bd435b58c167c0154a1 % % 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 1894 1 NaN NaN NaN NaN NaN NaN -4.003 1.823 1894 2 NaN NaN NaN NaN NaN NaN -5.274 -2.372 1894 3 NaN NaN NaN NaN NaN NaN 6.055 3.201 1894 4 NaN NaN NaN NaN NaN NaN 11.801 1.327 1894 5 NaN NaN NaN NaN NaN NaN 16.006 -0.552 1894 6 NaN NaN NaN NaN NaN NaN 23.484 1.747 1894 7 NaN NaN NaN NaN NaN NaN 23.974 0.231 1894 8 NaN NaN NaN NaN NaN NaN 22.574 -0.063 1894 9 NaN NaN NaN NaN NaN NaN 19.268 0.604 1894 10 NaN NaN NaN NaN NaN NaN 11.996 -0.161 1894 11 NaN NaN NaN NaN NaN NaN 1.614 -2.815 1894 12 NaN NaN NaN NaN NaN NaN -0.203 2.143 1895 1 -6.907 -1.596 0 0 -6.907 -1.596 -9.270 -3.444 1895 2 -7.063 -4.677 0 0 -7.063 -4.677 -8.916 -6.014 1895 3 2.312 -1.057 0 0 2.312 -1.057 1.722 -1.132 1895 4 10.833 -0.156 0 0 10.833 -0.156 11.765 1.290 1895 5 17.491 0.419 0 0 17.491 0.419 16.984 0.427 1895 6 23.574 1.321 0 0 23.574 1.321 23.264 1.526 1895 7 22.563 -1.696 1 0 NaN NaN 22.512 -1.231 1895 8 23.728 0.576 0 0 23.728 0.576 23.098 0.461 1895 9 20.278 1.098 0 0 20.278 1.098 20.563 1.899 1895 10 7.706 -4.966 0 0 7.706 -4.966 8.472 -3.685 1895 11 3.056 -1.889 0 0 3.056 -1.889 2.744 -1.685 1895 12 -0.484 1.347 0 0 -0.484 1.347 -1.555 0.791 1896 1 -2.704 2.607 0 0 -2.704 2.607 -3.572 2.254 1896 2 -2.460 -0.073 0 0 -2.460 -0.073 -2.905 -0.003 1896 3 0.832 -2.538 0 0 0.832 -2.538 0.370 -2.484 1896 4 14.130 3.140 0 0 14.130 3.140 14.214 3.740 1896 5 20.344 3.271 0 0 20.344 3.271 20.197 3.640 1896 6 21.043 -1.209 0 0 21.043 -1.209 21.611 -0.127 1896 7 23.320 -0.938 1 0 NaN NaN 23.223 -0.520 1896 8 NaN NaN NaN NaN NaN NaN 22.624 -0.012 1896 9 NaN NaN NaN NaN NaN NaN 16.449 -2.215 1896 10 NaN NaN NaN NaN NaN NaN 9.901 -2.256 1896 11 5.347 0.403 1 0 NaN NaN 3.364 -1.065 1896 12 1.231 3.062 0 0 1.231 3.062 0.289 2.636 1897 1 NaN NaN NaN NaN NaN NaN -6.703 -0.877 1897 2 -0.478 1.908 1 0 NaN NaN -2.083 0.818 1897 3 3.852 0.483 0 0 3.852 0.483 2.102 -0.752 1897 4 10.192 -0.798 0 0 10.192 -0.798 9.649 -0.826 1897 5 15.964 -1.109 0 0 15.964 -1.109 14.793 -1.765 1897 6 21.746 -0.507 0 0 21.746 -0.507 21.461 -0.277 1897 7 24.767 0.509 0 0 24.767 0.509 24.669 0.926 1897 8 21.352 -1.800 0 0 21.352 -1.800 21.244 -1.392 1897 9 21.232 2.053 0 0 21.232 2.053 21.713 3.048 1897 10 14.769 2.097 1 0 NaN NaN 15.332 3.175 1897 11 4.588 -0.356 0 0 4.588 -0.356 3.761 -0.669 1897 12 -3.046 -1.215 1 0 NaN NaN -4.748 -2.401 1898 1 -1.389 3.922 0 0 -1.389 3.922 -3.534 2.292 1898 2 -1.211 1.176 0 0 -1.211 1.176 -2.677 0.225 1898 3 6.060 2.691 0 0 6.060 2.691 4.629 1.775 1898 4 9.615 -1.375 0 0 9.615 -1.375 9.335 -1.139 1898 5 16.878 -0.194 1 0 NaN NaN 15.695 -0.862 1898 6 22.278 0.025 0 0 22.278 0.025 22.419 0.681 1898 7 23.208 -1.050 1 0 NaN NaN 23.608 -0.135 1898 8 22.782 -0.370 0 0 22.782 -0.370 22.193 -0.444 1898 9 20.237 1.057 0 0 20.237 1.057 20.093 1.429 1898 10 10.487 -2.185 0 0 10.487 -2.185 10.617 -1.540 1898 11 1.992 -2.953 0 0 1.992 -2.953 2.147 -2.283 1898 12 -3.937 -2.106 0 0 -3.937 -2.106 -4.683 -2.337 1899 1 NaN NaN NaN NaN NaN NaN -5.795 0.031 1899 2 NaN NaN NaN NaN NaN NaN -8.503 -5.601 1899 3 NaN NaN NaN NaN NaN NaN -1.034 -3.888 1899 4 NaN NaN NaN NaN NaN NaN 11.387 0.912 1899 5 NaN NaN NaN NaN NaN NaN 16.728 0.171 1899 6 NaN NaN NaN NaN NaN NaN 22.226 0.488 1899 7 NaN NaN NaN NaN NaN NaN 23.315 -0.429 1899 8 NaN NaN NaN NaN NaN NaN 23.625 0.988 1899 9 NaN NaN NaN NaN NaN NaN 17.776 -0.889 1899 10 NaN NaN NaN NaN NaN NaN 14.728 2.571 1899 11 NaN NaN NaN NaN NaN NaN 7.342 2.912 1899 12 NaN NaN NaN NaN NaN NaN -3.242 -0.895