% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 11854 % Primary Name: KWANGHAN CHINA AAB % Record Type: TAVG % Country: China % Latitude: 31.11600 +/- 0.00050 % Longitude: 104.00000 +/- 0.00050 % Elevation (m): 500.00 +/- 0.05 % # of Months: 8 % % IDs: gsod - 749338-99999 % usaf - 749338 % % Sources: Global Summary of the Day % % Site Hash: 4a5816c1d2170831dd0d6794c6d0c272 % Raw Data Hash: dbdb74ec3ff28ddd754bce4c7301350d % Adj Data Hash: 5ce316b63c087f1124fa3d1344cd422a % % 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 1 NaN NaN NaN NaN NaN NaN 0.178 -0.002 1944 2 NaN NaN NaN NaN NaN NaN 3.034 0.371 1944 3 NaN NaN NaN NaN NaN NaN 8.483 1.157 1944 4 NaN NaN NaN NaN NaN NaN 11.487 -0.141 1944 5 NaN NaN NaN NaN NaN NaN 15.264 0.004 1944 6 NaN NaN NaN NaN NaN NaN 17.260 -0.522 1944 7 NaN NaN NaN NaN NaN NaN 20.523 0.563 1944 8 NaN NaN NaN NaN NaN NaN 19.997 0.379 1944 9 NaN NaN NaN NaN NaN NaN 15.925 -0.054 1944 10 NaN NaN NaN NaN NaN NaN 10.913 -0.417 1944 11 NaN NaN NaN NaN NaN NaN 6.815 0.488 1944 12 NaN NaN NaN NaN NaN NaN -1.208 -2.787 1945 1 4.843 -1.580 1 0 NaN NaN 0.098 -0.081 1945 2 5.695 -3.211 1 0 NaN NaN 0.094 -2.568 1945 3 12.789 -0.781 0 0 12.789 -0.781 7.556 0.230 1945 4 18.506 0.634 0 0 18.506 0.634 12.321 0.693 1945 5 23.391 1.887 0 0 23.391 1.887 16.348 1.088 1945 6 25.939 1.913 0 0 25.939 1.913 18.896 1.114 1945 7 26.871 0.668 0 0 26.871 0.668 20.336 0.377 1945 8 24.907 -0.955 0 0 24.907 -0.955 19.482 -0.136 1945 9 NaN NaN NaN NaN NaN NaN 17.027 1.048 1945 10 NaN NaN NaN NaN NaN NaN 11.509 0.179 1945 11 NaN NaN NaN NaN NaN NaN 8.779 2.452 1945 12 NaN NaN NaN NaN NaN NaN 1.811 0.231 1946 1 NaN NaN NaN NaN NaN NaN 2.336 2.157 1946 2 NaN NaN NaN NaN NaN NaN 5.766 3.104 1946 3 NaN NaN NaN NaN NaN NaN 7.038 -0.288 1946 4 NaN NaN NaN NaN NaN NaN 14.678 3.050 1946 5 NaN NaN NaN NaN NaN NaN 16.041 0.781 1946 6 NaN NaN NaN NaN NaN NaN 18.305 0.523 1946 7 NaN NaN NaN NaN NaN NaN 20.509 0.549 1946 8 NaN NaN NaN NaN NaN NaN 20.801 1.183