% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 11826 % Primary Name: LIANGSHAN CHINA AAB % Record Type: TAVG % Country: China % Latitude: 30.58300 +/- 0.00050 % Longitude: 107.83300 +/- 0.00050 % Elevation (m): 501.00 +/- 0.05 % # of Months: 14 % % IDs: gsod - 749340-99999 % icao - RLGN % usaf - 749340 % % Sources: Global Summary of the Day % % Site Hash: 09f664c68da8b642c63066620196f69b % Raw Data Hash: 1f4976b3304e576af6323b20c39b6af1 % Adj Data Hash: f358b14a291ef5746fe2440853244d33 % % 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 1944 2 NaN NaN NaN NaN NaN NaN 7.715 0.366 1944 3 NaN NaN NaN NaN NaN NaN 13.448 1.409 1944 4 NaN NaN NaN NaN NaN NaN 16.476 -0.506 1944 5 NaN NaN NaN NaN NaN NaN 20.706 -0.142 1944 6 NaN NaN NaN NaN NaN NaN 23.648 -0.824 1944 7 NaN NaN NaN NaN NaN NaN 28.269 0.969 1944 8 NaN NaN NaN NaN NaN NaN 27.544 0.274 1944 9 NaN NaN NaN NaN NaN NaN 22.305 -0.144 1944 10 NaN NaN NaN NaN NaN NaN 15.902 -1.132 1944 11 NaN NaN NaN NaN NaN NaN 12.357 0.509 1944 12 NaN NaN NaN NaN NaN NaN 3.750 -3.361 1945 1 NaN NaN NaN NaN NaN NaN 4.532 -0.743 1945 2 14.212 6.889 1 0 NaN NaN 4.770 -2.579 1945 3 11.143 -0.869 0 0 11.143 -0.869 11.286 -0.753 1945 4 17.006 0.049 0 0 17.006 0.049 17.432 0.450 1945 5 21.688 0.866 0 0 21.688 0.866 22.035 1.187 1945 6 25.693 1.246 0 0 25.693 1.246 25.581 1.109 1945 7 26.968 -0.306 0 0 26.968 -0.306 27.196 -0.104 1945 8 26.873 -0.371 0 0 26.873 -0.371 27.420 0.150 1945 9 23.461 1.038 0 0 23.461 1.038 23.242 0.793 1945 10 16.830 -0.177 0 0 16.830 -0.177 17.251 0.218 1945 11 15.256 3.434 1 0 NaN NaN 14.304 2.455 1945 12 NaN NaN NaN NaN NaN NaN 7.543 0.432 1946 1 8.677 3.428 0 0 8.677 3.428 7.499 2.224 1946 2 10.616 3.293 1 0 NaN NaN 10.427 3.078 1946 3 11.349 -0.663 0 0 11.349 -0.663 11.065 -0.973 1946 4 19.985 3.029 0 0 19.985 3.029 19.952 2.969 1946 5 NaN NaN NaN NaN NaN NaN 21.215 0.367 1946 6 NaN NaN NaN NaN NaN NaN 24.366 -0.106 1946 7 NaN NaN NaN NaN NaN NaN 27.185 -0.115 1946 8 NaN NaN NaN NaN NaN NaN 28.166 0.897 1946 9 NaN NaN NaN NaN NaN NaN 23.076 0.626 1946 10 NaN NaN NaN NaN NaN NaN 18.041 1.008 1946 11 NaN NaN NaN NaN NaN NaN 12.491 0.643 1946 12 NaN NaN NaN NaN NaN NaN 6.339 -0.771 1947 1 NaN NaN NaN NaN NaN NaN 6.192 0.917 1947 2 NaN NaN NaN NaN NaN NaN 7.350 0.001 1947 3 NaN NaN NaN NaN NaN NaN 13.679 1.641 1947 4 NaN NaN NaN NaN NaN NaN 17.939 0.957