% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 12063 % Primary Name: LANCHOW CHINA % Record Type: TAVG % Country: China % Latitude: 36.00000 +/- 0.00500 % Longitude: 103.75000 +/- 0.00500 % Elevation (m): 1543.00 +/- 0.05 % # of Months: 14 % % IDs: gsod - 749344-99999 % icao - RLHW % usaf - 749344 % % Sources: Global Summary of the Day % % Site Hash: af5b3b0c55ba5d13a2219f2f649b5b90 % Raw Data Hash: 39a427256832ab79aa2f626c76f446b1 % Adj Data Hash: 015aa2ec3c7073f7f5a8be66d955cfc4 % % 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 11 NaN NaN NaN NaN NaN NaN -1.183 -0.035 1944 12 NaN NaN NaN NaN NaN NaN -10.992 -3.377 1945 1 NaN NaN NaN NaN NaN NaN -11.380 -2.130 1945 2 NaN NaN NaN NaN NaN NaN -9.493 -4.312 1945 3 NaN NaN NaN NaN NaN NaN 1.865 -0.064 1945 4 NaN NaN NaN NaN NaN NaN 9.934 1.875 1945 5 NaN NaN NaN NaN NaN NaN 14.030 1.185 1945 6 NaN NaN NaN NaN NaN NaN 17.977 1.587 1945 7 NaN NaN NaN NaN NaN NaN 18.806 0.335 1945 8 NaN NaN NaN NaN NaN NaN 18.487 1.085 1945 9 NaN NaN NaN NaN NaN NaN 13.571 1.056 1945 10 NaN NaN NaN NaN NaN NaN 7.033 0.730 1945 11 4.747 2.179 1 0 NaN NaN 1.573 2.721 1945 12 -3.948 -0.049 0 0 -3.948 -0.049 -7.261 0.354 1946 1 -3.536 1.997 0 0 -3.536 1.997 -7.104 2.145 1946 2 1.194 2.659 1 0 NaN NaN -2.439 2.742 1946 3 4.498 -1.147 0 0 4.498 -1.147 0.888 -1.040 1946 4 14.670 2.895 0 0 14.670 2.895 10.863 2.804 1946 5 16.724 0.164 0 0 16.724 0.164 12.836 -0.008 1946 6 21.224 1.118 0 0 21.224 1.118 16.632 0.242 1946 7 22.648 0.460 0 0 22.648 0.460 18.704 0.233 1946 8 21.971 0.853 0 0 21.971 0.853 18.325 0.923 1946 9 16.911 0.680 0 0 16.911 0.680 12.952 0.437 1946 10 11.065 1.045 0 0 11.065 1.045 7.718 1.415 1946 11 2.780 0.212 1 0 NaN NaN -0.258 0.890 1946 12 -4.609 -0.711 0 0 -4.609 -0.711 -7.814 -0.199 1947 1 NaN NaN NaN NaN NaN NaN -8.467 0.783 1947 2 NaN NaN NaN NaN NaN NaN -5.235 -0.055 1947 3 NaN NaN NaN NaN NaN NaN 2.840 0.911 1947 4 NaN NaN NaN NaN NaN NaN 9.257 1.199 1947 5 NaN NaN NaN NaN NaN NaN 14.648 1.804 1947 6 NaN NaN NaN NaN NaN NaN 16.576 0.186 1947 7 NaN NaN NaN NaN NaN NaN 19.229 0.758 1947 8 NaN NaN NaN NaN NaN NaN 17.484 0.082 1947 9 NaN NaN NaN NaN NaN NaN 12.465 -0.050 1947 10 NaN NaN NaN NaN NaN NaN 5.843 -0.460 1947 11 NaN NaN NaN NaN NaN NaN 0.782 1.930 1947 12 NaN NaN NaN NaN NaN NaN -7.455 0.160