% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 11533 % Primary Name: LULIANG CHINA AAF % Record Type: TAVG % Country: China % Latitude: 25.00000 +/- 0.00050 % Longitude: 103.58300 +/- 0.00050 % Elevation (m): 1849.00 +/- 0.05 % # of Months: 18 % % IDs: gsod - 749323-99999 % usaf - 749323 % % Sources: Global Summary of the Day % % Site Hash: c641ee5b55aa0efe103e48c53068e4ba % Raw Data Hash: f82efd130e6b28f1387443fd6d647652 % Adj Data Hash: 74e912b9d50ad377dd23968eaebde08d % % 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 1943 6 NaN NaN NaN NaN NaN NaN 19.493 0.136 1943 7 NaN NaN NaN NaN NaN NaN 19.747 -0.036 1943 8 NaN NaN NaN NaN NaN NaN 18.625 -0.579 1943 9 NaN NaN NaN NaN NaN NaN 17.246 -0.481 1943 10 NaN NaN NaN NaN NaN NaN 15.338 0.579 1943 11 NaN NaN NaN NaN NaN NaN 11.558 0.319 1943 12 NaN NaN NaN NaN NaN NaN 8.471 0.210 1944 1 NaN NaN NaN NaN NaN NaN 8.849 1.081 1944 2 NaN NaN NaN NaN NaN NaN 10.127 0.328 1944 3 NaN NaN NaN NaN NaN NaN 14.103 0.587 1944 4 NaN NaN NaN NaN NaN NaN 16.588 -0.013 1944 5 NaN NaN NaN NaN NaN NaN 17.224 -1.758 1944 6 17.593 -2.514 1 0 NaN NaN 18.532 -0.826 1944 7 19.921 -0.611 0 0 19.921 -0.611 19.375 -0.407 1944 8 19.609 -0.345 0 0 19.609 -0.345 18.778 -0.426 1944 9 18.265 -0.213 0 0 18.265 -0.213 17.648 -0.080 1944 10 16.878 1.370 0 0 16.878 1.370 16.286 1.528 1944 11 13.087 1.099 0 0 13.087 1.099 12.549 1.311 1944 12 6.862 -2.149 0 0 6.862 -2.149 7.246 -1.015 1945 1 10.357 1.839 0 0 10.357 1.839 9.301 1.533 1945 2 7.587 -2.962 1 0 NaN NaN 7.334 -2.465 1945 3 13.450 -0.816 0 0 13.450 -0.816 13.615 0.098 1945 4 18.419 1.068 0 0 18.419 1.068 17.399 0.798 1945 5 17.228 -2.504 0 0 17.228 -2.504 16.566 -2.416 1945 6 20.470 0.364 0 0 20.470 0.364 19.033 -0.324 1945 7 20.672 0.140 0 0 20.672 0.140 19.478 -0.304 1945 8 19.858 -0.096 0 0 19.858 -0.096 18.661 -0.543 1945 9 19.554 1.076 0 0 19.554 1.076 18.396 0.668 1945 10 14.091 -1.417 0 0 14.091 -1.417 13.144 -1.615 1945 11 12.957 0.969 1 0 NaN NaN 12.730 1.492 1945 12 NaN NaN NaN NaN NaN NaN 8.423 0.162 1946 1 NaN NaN NaN NaN NaN NaN 10.068 2.301 1946 2 NaN NaN NaN NaN NaN NaN 11.806 2.007 1946 3 NaN NaN NaN NaN NaN NaN 15.013 1.496 1946 4 NaN NaN NaN NaN NaN NaN 17.857 1.256 1946 5 NaN NaN NaN NaN NaN NaN 19.932 0.950 1946 6 NaN NaN NaN NaN NaN NaN 20.753 1.396 1946 7 NaN NaN NaN NaN NaN NaN 20.604 0.821 1946 8 NaN NaN NaN NaN NaN NaN 20.684 1.479 1946 9 NaN NaN NaN NaN NaN NaN 19.496 1.768 1946 10 NaN NaN NaN NaN NaN NaN 14.892 0.133 1946 11 NaN NaN NaN NaN NaN NaN 13.007 1.768