% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 30651 % Primary Name: CHANNING 11 NE % Record Type: TAVG % Country: United States % State: TX % Latitude: 35.76670 +/- 0.00005 % Longitude: -102.15000 +/- 0.00005 % Elevation (m): 1135.40 +/- 0.05 % # of Months: 17 % % IDs: coop - 411650 % faa - CHAT % ghcnd - USC00411650 % ncdc - 20026037 % nws - CHAT % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % US Cooperative Summary of the Month % Multi-network Metadata System % % Site Hash: 3a5792729ccb799864529200f386388e % Raw Data Hash: 1fd9744aef403ce82298eb7ed2b70fd4 % Adj Data Hash: 1fd9744aef403ce82298eb7ed2b70fd4 % % 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 1989 3 NaN NaN NaN NaN NaN NaN 9.222 1.930 1989 4 NaN NaN NaN NaN NaN NaN 15.261 2.139 1989 5 NaN NaN NaN NaN NaN NaN 18.949 0.596 1989 6 NaN NaN NaN NaN NaN NaN 21.130 -2.698 1989 7 NaN NaN NaN NaN NaN NaN 25.170 -1.195 1989 8 NaN NaN NaN NaN NaN NaN 24.481 -0.861 1989 9 NaN NaN NaN NaN NaN NaN 19.105 -1.797 1989 10 NaN NaN NaN NaN NaN NaN 15.704 1.093 1989 11 NaN NaN NaN NaN NaN NaN 8.363 1.389 1989 12 NaN NaN NaN NaN NaN NaN -0.389 -3.095 1990 1 NaN NaN NaN NaN NaN NaN 3.004 2.076 1990 2 NaN NaN NaN NaN NaN NaN 4.144 0.588 1990 3 6.722 1.095 0 0 6.722 1.095 7.402 0.110 1990 4 12.222 0.765 0 0 12.222 0.765 13.530 0.409 1990 5 15.944 -0.743 0 0 15.944 -0.743 17.027 -1.326 1990 6 25.389 3.226 0 0 25.389 3.226 26.874 3.046 1990 7 24.000 -0.700 0 0 24.000 -0.700 25.547 -0.818 1990 8 22.889 -0.788 0 0 22.889 -0.788 25.192 -0.149 1990 9 21.000 1.763 0 0 21.000 1.763 22.541 1.639 1990 10 12.722 -0.224 0 0 12.722 -0.224 14.545 -0.066 1990 11 7.833 2.525 0 0 7.833 2.525 9.446 2.473 1990 12 -1.722 -2.764 0 0 -1.722 -2.764 0.341 -2.366 1991 1 -1.833 -1.097 0 0 -1.833 -1.097 -0.614 -1.542 1991 2 5.722 3.832 0 0 5.722 3.832 7.529 3.974 1991 3 7.889 2.261 0 0 7.889 2.261 8.984 1.691 1991 4 12.778 1.321 0 0 12.778 1.321 14.440 1.319 1991 5 17.889 1.201 0 0 17.889 1.201 19.757 1.404 1991 6 21.667 -0.497 0 0 21.667 -0.497 24.161 0.333 1991 7 23.000 -1.700 0 0 23.000 -1.700 25.712 -0.652 1991 8 NaN NaN NaN NaN NaN NaN 24.940 -0.401 1991 9 NaN NaN NaN NaN NaN NaN 19.873 -1.028 1991 10 NaN NaN NaN NaN NaN NaN 15.227 0.616 1991 11 NaN NaN NaN NaN NaN NaN 4.222 -2.752 1991 12 NaN NaN NaN NaN NaN NaN 3.670 0.964 1992 1 NaN NaN NaN NaN NaN NaN 3.146 2.218 1992 2 NaN NaN NaN NaN NaN NaN 6.711 3.156 1992 3 NaN NaN NaN NaN NaN NaN 9.690 2.398 1992 4 NaN NaN NaN NaN NaN NaN 14.543 1.422 1992 5 NaN NaN NaN NaN NaN NaN 17.560 -0.792 1992 6 NaN NaN NaN NaN NaN NaN 21.518 -2.311 1992 7 NaN NaN NaN NaN NaN NaN 25.365 -1.000