% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 34072 % Primary Name: NOTTOWAY COURT HOUSE % Record Type: TAVG % Country: United States % State: VA % Latitude: 39.13330 +/- 0.00005 % Longitude: -78.11670 +/- 0.00005 % Elevation (m): 129.84 +/- 0.15 % # of Months: 52 % % Alternate Names: Missing Station ID - 446240 % % IDs: coop - 446240 % ghcnd - USC00446240 % ncdc - 12005768 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 79c7f4ccb792b4b3ac86ae632940e00a % Raw Data Hash: d9507247add93596fddc586d867e2a97 % Adj Data Hash: f7978bac4c5e07d85c0bb140386f9d13 % % 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 -3.541 -1.433 1892 2 NaN NaN NaN NaN NaN NaN -0.189 0.741 1892 3 NaN NaN NaN NaN NaN NaN 0.891 -3.129 1892 4 NaN NaN NaN NaN NaN NaN 8.667 -1.299 1892 5 NaN NaN NaN NaN NaN NaN 14.935 -0.316 1892 6 NaN NaN NaN NaN NaN NaN 21.582 2.054 1892 7 NaN NaN NaN NaN NaN NaN 21.328 -0.356 1892 8 NaN NaN NaN NaN NaN NaN 21.452 0.378 1892 9 NaN NaN NaN NaN NaN NaN 16.707 -0.804 1892 10 NaN NaN NaN NaN NaN NaN 9.846 -1.141 1892 11 NaN NaN NaN NaN NaN NaN 3.944 -1.436 1892 12 NaN NaN NaN NaN NaN NaN -2.288 -2.254 1893 1 -3.982 -6.401 0 0 -3.982 -6.401 -7.318 -5.210 1893 2 3.477 -0.119 0 0 3.477 -0.119 -1.271 -0.341 1893 3 6.846 -1.702 0 0 6.846 -1.702 3.195 -0.826 1893 4 14.074 -0.419 0 0 14.074 -0.419 10.234 0.268 1893 5 18.315 -1.462 0 0 18.315 -1.462 14.110 -1.141 1893 6 24.037 -0.019 0 0 24.037 -0.019 19.999 0.470 1893 7 26.595 0.385 0 0 26.595 0.385 22.091 0.408 1893 8 24.319 -1.282 0 0 24.319 -1.282 20.364 -0.710 1893 9 20.632 -1.406 0 0 20.632 -1.406 16.900 -0.612 1893 10 14.301 -1.213 0 0 14.301 -1.213 10.760 -0.227 1893 11 7.436 -2.470 0 0 7.436 -2.470 3.834 -1.546 1893 12 5.125 0.632 0 0 5.125 0.632 0.894 0.927 1894 1 5.444 3.025 0 0 5.444 3.025 0.712 2.820 1894 2 5.447 1.850 0 0 5.447 1.850 -1.544 -0.614 1894 3 9.928 1.380 0 0 9.928 1.380 6.574 2.553 1894 4 12.298 -2.195 0 0 12.298 -2.195 8.992 -0.974 1894 5 21.267 1.489 0 0 21.267 1.489 15.625 0.374 1894 6 24.157 0.101 0 0 24.157 0.101 20.060 0.532 1894 7 26.308 0.098 0 0 26.308 0.098 21.659 -0.024 1894 8 24.588 -1.013 0 0 24.588 -1.013 20.243 -0.832 1894 9 23.267 1.228 0 0 23.267 1.228 18.912 1.400 1894 10 14.952 -0.562 0 0 14.952 -0.562 11.104 0.117 1894 11 8.074 -1.833 0 0 8.074 -1.833 3.591 -1.789 1894 12 5.072 0.578 0 0 5.072 0.578 0.152 0.186 1895 1 2.115 -0.304 0 0 2.115 -0.304 -4.693 -2.585 1895 2 -5.259 -8.856 1 0 NaN NaN -7.312 -6.381 1895 3 10.029 1.481 1 0 NaN NaN 2.420 -1.601 1895 4 12.556 -1.937 1 0 NaN NaN 9.765 -0.201 1895 5 17.397 -2.381 0 0 17.397 -2.381 14.502 -0.749 1895 6 24.752 0.696 0 0 24.752 0.696 20.651 1.123 1895 7 24.409 -1.802 0 0 24.409 -1.802 19.515 -2.168 1895 8 26.152 0.551 0 0 26.152 0.551 21.408 0.334 1895 9 25.199 3.160 1 0 NaN NaN 19.898 2.387 1895 10 13.004 -2.510 0 0 13.004 -2.510 7.654 -3.333 1895 11 10.214 0.307 0 0 10.214 0.307 5.880 0.501 1895 12 4.571 0.077 0 0 4.571 0.077 0.468 0.502 1896 1 2.137 -0.282 0 0 2.137 -0.282 -2.222 -0.114 1896 2 5.590 1.994 1 0 NaN NaN -1.354 -0.423 1896 3 7.599 -0.949 0 0 7.599 -0.949 0.281 -3.740 1896 4 13.378 -1.115 0 0 13.378 -1.115 12.312 2.346 1896 5 NaN NaN NaN NaN NaN NaN 18.056 2.805 1896 6 NaN NaN NaN NaN NaN NaN 18.998 -0.531 1896 7 NaN NaN NaN NaN NaN NaN 21.639 -0.045 1896 8 26.490 0.889 0 0 26.490 0.889 21.062 -0.012 1896 9 22.004 -0.035 0 0 22.004 -0.035 17.343 -0.169 1896 10 14.686 -0.828 0 0 14.686 -0.828 8.651 -2.337 1896 11 13.384 3.477 0 0 13.384 3.477 7.942 2.562 1896 12 3.683 -0.810 0 0 3.683 -0.810 -0.516 -0.482 1897 1 1.190 -1.229 0 0 1.190 -1.229 -4.084 -1.976 1897 2 NaN NaN NaN NaN NaN NaN -0.491 0.439 1897 3 NaN NaN NaN NaN NaN NaN 5.818 1.797 1897 4 NaN NaN NaN NaN NaN NaN 9.558 -0.408 1897 5 NaN NaN NaN NaN NaN NaN 13.246 -2.005 1897 6 NaN NaN NaN NaN NaN NaN 18.555 -0.974 1897 7 NaN NaN NaN NaN NaN NaN 22.184 0.501 1897 8 25.533 -0.068 0 0 25.533 -0.068 19.865 -1.209 1897 9 21.733 -0.305 0 0 21.733 -0.305 17.697 0.186 1897 10 16.185 0.671 0 0 16.185 0.671 12.025 1.037 1897 11 10.500 0.593 0 0 10.500 0.593 5.359 -0.021 1897 12 5.860 1.367 0 0 5.860 1.367 0.706 0.739 1898 1 5.538 3.118 0 0 5.538 3.118 0.044 2.152 1898 2 NaN NaN NaN NaN NaN NaN -1.878 -0.948 1898 3 NaN NaN NaN NaN NaN NaN 7.392 3.371 1898 4 NaN NaN NaN NaN NaN NaN 7.371 -2.595 1898 5 NaN NaN NaN NaN NaN NaN 15.744 0.493 1898 6 NaN NaN NaN NaN NaN NaN 19.944 0.415 1898 7 NaN NaN NaN NaN NaN NaN 22.687 1.003 1898 8 NaN NaN NaN NaN NaN NaN 21.742 0.668 1898 9 NaN NaN NaN NaN NaN NaN 18.408 0.897 1898 10 NaN NaN NaN NaN NaN NaN 11.106 0.118 1898 11 NaN NaN NaN NaN NaN NaN 4.237 -1.143 1898 12 NaN NaN NaN NaN NaN NaN -1.510 -1.476 1899 1 NaN NaN NaN NaN NaN NaN -2.176 -0.068