% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 11827 % Primary Name: HANKOW CHINA % Record Type: TAVG % Country: China % Latitude: 30.58300 +/- 0.00050 % Longitude: 114.25000 +/- 0.00050 % Elevation (m): 37.00 +/- 0.05 % # of Months: 30 % % IDs: gsod - 749348-99999 % usaf - 749348 % % Sources: Global Summary of the Day % % Site Hash: 83dbc895f3d7a154a04a19a5bedcb8ba % Raw Data Hash: 26e3429e2e8ae660903204d3856bdcdf % Adj Data Hash: 970974517af7fa6655ab8ff346883de6 % % 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 9 NaN NaN NaN NaN NaN NaN 24.849 0.666 1944 10 NaN NaN NaN NaN NaN NaN 17.252 -0.942 1944 11 NaN NaN NaN NaN NaN NaN 13.503 1.368 1944 12 NaN NaN NaN NaN NaN NaN 2.448 -3.904 1945 1 NaN NaN NaN NaN NaN NaN 2.514 -1.447 1945 2 NaN NaN NaN NaN NaN NaN 2.827 -2.992 1945 3 NaN NaN NaN NaN NaN NaN 10.507 -0.189 1945 4 NaN NaN NaN NaN NaN NaN 17.474 0.784 1945 5 NaN NaN NaN NaN NaN NaN 21.598 -0.161 1945 6 NaN NaN NaN NaN NaN NaN 26.881 0.902 1945 7 NaN NaN NaN NaN NaN NaN 29.281 -0.022 1945 8 NaN NaN NaN NaN NaN NaN 28.930 0.084 1945 9 15.532 -8.276 1 0 NaN NaN 25.384 1.201 1945 10 17.812 -0.007 0 0 17.812 -0.007 17.729 -0.465 1945 11 15.076 3.315 0 0 15.076 3.315 15.814 3.679 1945 12 6.944 0.967 0 0 6.944 0.967 7.025 0.673 1946 1 5.600 2.014 0 0 5.600 2.014 6.264 2.302 1946 2 8.520 3.076 0 0 8.520 3.076 9.267 3.448 1946 3 8.729 -1.592 0 0 8.729 -1.592 9.133 -1.563 1946 4 18.352 2.036 0 0 18.352 2.036 19.103 2.413 1946 5 21.366 -0.018 0 0 21.366 -0.018 21.536 -0.223 1946 6 26.828 1.224 0 0 26.828 1.224 26.733 0.754 1946 7 28.561 -0.367 0 0 28.561 -0.367 28.792 -0.511 1946 8 28.824 0.353 0 0 28.824 0.353 29.475 0.628 1946 9 25.072 1.264 0 0 25.072 1.264 25.693 1.510 1946 10 18.661 0.842 0 0 18.661 0.842 18.977 0.783 1946 11 13.094 1.334 0 0 13.094 1.334 13.948 1.813 1946 12 4.489 -1.488 0 0 4.489 -1.488 4.634 -1.718 1947 1 3.713 0.127 0 0 3.713 0.127 4.580 0.618 1947 2 -14.792 -20.236 1 0 NaN NaN 5.187 -0.632 1947 3 11.647 1.326 0 0 11.647 1.326 11.686 0.990 1947 4 17.631 1.316 0 0 17.631 1.316 17.698 1.008 1947 5 22.022 0.637 0 0 22.022 0.637 22.083 0.324 1947 6 25.609 0.005 0 0 25.609 0.005 25.311 -0.668 1947 7 29.324 0.396 0 0 29.324 0.396 29.844 0.541 1947 8 29.271 0.799 0 0 29.271 0.799 29.826 0.979 1947 9 24.609 0.801 0 0 24.609 0.801 24.908 0.724 1947 10 16.765 -1.054 0 0 16.765 -1.054 16.911 -1.283 1947 11 11.680 -0.081 0 0 11.680 -0.081 12.877 0.742 1947 12 4.206 -1.771 0 0 4.206 -1.771 4.857 -1.495 1948 1 4.262 0.675 0 0 4.262 0.675 4.763 0.802 1948 2 7.647 2.203 0 0 7.647 2.203 7.347 1.528 1948 3 NaN NaN NaN NaN NaN NaN 10.143 -0.553 1948 4 NaN NaN NaN NaN NaN NaN 18.319 1.628 1948 5 NaN NaN NaN NaN NaN NaN 20.452 -1.307 1948 6 NaN NaN NaN NaN NaN NaN 25.949 -0.030 1948 7 NaN NaN NaN NaN NaN NaN 28.800 -0.503 1948 8 NaN NaN NaN NaN NaN NaN 29.526 0.680 1948 9 NaN NaN NaN NaN NaN NaN 24.627 0.443 1948 10 NaN NaN NaN NaN NaN NaN 18.245 0.051 1948 11 NaN NaN NaN NaN NaN NaN 11.119 -1.016 1948 12 NaN NaN NaN NaN NaN NaN 7.523 1.171 1949 1 NaN NaN NaN NaN NaN NaN 4.952 0.991 1949 2 NaN NaN NaN NaN NaN NaN 7.452 1.633