% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 11883 % Primary Name: MOU-HSIEN /MAOKSIEN % Record Type: TAVG % Country: China % Latitude: 31.71700 +/- 0.00050 % Longitude: 103.88300 +/- 0.00050 % Elevation (m): 1571.90 +/- 0.05 % # of Months: 63 % % IDs: gsod - 561830-99999 % usaf - 561830 % % Sources: Global Summary of the Day % % Site Hash: eceab71f8332068afeb511e81abf2265 % Raw Data Hash: 22ea139a899067ef2258bdf5281d85a0 % Adj Data Hash: 82663d134be2ae915b7768ad797ab9d5 % % 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 1955 8 NaN NaN NaN NaN NaN NaN 19.888 0.270 1955 9 NaN NaN NaN NaN NaN NaN 16.531 0.552 1955 10 NaN NaN NaN NaN NaN NaN 11.341 0.011 1955 11 NaN NaN NaN NaN NaN NaN 5.909 -0.417 1955 12 NaN NaN NaN NaN NaN NaN 2.496 0.917 1956 1 NaN NaN NaN NaN NaN NaN -1.080 -1.259 1956 2 NaN NaN NaN NaN NaN NaN 3.239 0.576 1956 3 NaN NaN NaN NaN NaN NaN 7.654 0.329 1956 4 NaN NaN NaN NaN NaN NaN 12.689 1.062 1956 5 NaN NaN NaN NaN NaN NaN 14.717 -0.543 1956 6 NaN NaN NaN NaN NaN NaN 18.018 0.236 1956 7 NaN NaN NaN NaN NaN NaN 19.193 -0.767 1956 8 18.510 -2.245 1 0 NaN NaN 18.564 -1.054 1956 9 16.952 -0.164 0 0 17.456 0.340 15.756 -0.223 1956 10 11.602 -0.865 0 0 12.106 -0.361 10.955 -0.375 1956 11 6.111 -1.353 1 0 NaN NaN 5.509 -0.817 1956 12 2.579 -0.137 1 0 NaN NaN 0.555 -1.024 1957 1 0.778 -0.539 1 0 NaN NaN 0.965 0.785 1957 2 -0.208 -4.007 1 0 NaN NaN 0.302 -2.360 1957 3 8.096 -0.367 0 0 8.600 0.137 7.353 0.028 1957 4 11.800 -0.965 0 0 12.304 -0.461 11.510 -0.117 1957 5 14.321 -2.077 0 0 14.825 -1.573 13.949 -1.311 1957 6 18.134 -0.785 1 0 NaN NaN 16.734 -1.048 1957 7 21.076 -0.021 0 0 21.580 0.483 19.789 -0.171 1957 8 20.754 -0.001 0 0 21.258 0.503 19.820 0.202 1957 9 15.320 -1.796 0 0 15.824 -1.292 14.766 -1.213 1957 10 10.661 -1.806 0 0 11.165 -1.302 9.921 -1.409 1957 11 8.385 0.921 0 0 8.889 1.425 7.566 1.239 1957 12 3.541 0.825 0 0 4.045 1.329 2.437 0.858 1958 1 -0.423 -1.740 0 0 0.081 -1.236 -0.262 -0.441 1958 2 2.819 -0.980 0 0 3.323 -0.476 2.135 -0.527 1958 3 9.517 1.054 0 0 10.020 1.558 9.455 2.130 1958 4 13.939 1.174 0 0 14.443 1.678 13.444 1.817 1958 5 15.046 -1.351 0 0 15.550 -0.847 14.755 -0.505 1958 6 18.698 -0.221 0 0 19.202 0.283 17.628 -0.154 1958 7 21.731 0.634 0 0 22.235 1.138 20.765 0.805 1958 8 19.283 -1.472 0 0 19.787 -0.968 18.691 -0.927 1958 9 16.887 -0.229 0 0 17.391 0.275 16.066 0.087 1958 10 10.909 -1.559 0 0 11.412 -1.055 10.642 -0.688 1958 11 7.074 -0.390 0 0 7.578 0.114 6.569 0.242 1958 12 3.487 0.771 0 0 3.991 1.274 2.217 0.638 1959 1 0.249 -1.068 0 0 0.753 -0.564 -0.172 -0.352 1959 2 2.103 -1.696 0 0 2.607 -1.193 1.960 -0.702 1959 3 7.376 -1.087 0 0 7.880 -0.583 7.304 -0.021 1959 4 13.424 0.659 0 0 13.928 1.163 12.788 1.161 1959 5 13.858 -2.539 0 0 14.362 -2.035 14.034 -1.226 1959 6 18.324 -0.595 0 0 18.828 -0.091 17.308 -0.475 1959 7 21.741 0.644 0 0 22.245 1.147 20.983 1.023 1959 8 21.194 0.438 0 0 21.697 0.942 20.731 1.113 1959 9 16.581 -0.535 0 0 17.085 -0.031 15.450 -0.529 1959 10 13.036 0.568 0 0 13.540 1.072 12.002 0.672 1959 11 7.306 -0.158 0 0 7.809 0.345 6.853 0.526 1959 12 2.113 -0.604 0 0 2.617 -0.100 1.540 -0.040 1960 1 3.014 1.698 0 4 2.213 0.896 0.346 0.167 1960 2 6.799 2.999 0 0 5.997 2.198 4.616 1.954 1960 3 10.726 2.263 0 0 9.924 1.461 9.210 1.884 1960 4 12.035 -0.730 0 0 11.234 -1.531 10.676 -0.952 1960 5 16.240 -0.157 0 0 15.439 -0.959 14.909 -0.351 1960 6 19.593 0.673 0 0 18.791 -0.128 17.425 -0.357 1960 7 21.722 0.625 0 0 20.921 -0.176 19.734 -0.225 1960 8 21.534 0.779 0 0 20.732 -0.023 19.331 -0.287 1960 9 18.946 1.830 0 0 18.145 1.029 16.387 0.408 1960 10 12.407 -0.061 0 0 11.605 -0.862 10.608 -0.722 1960 11 8.174 0.710 0 0 7.373 -0.091 6.370 0.044 1960 12 3.869 1.153 0 0 3.068 0.351 1.620 0.041 1961 1 1.980 0.664 0 0 1.179 -0.138 0.089 -0.091 1961 2 3.169 -0.631 0 0 2.367 -1.432 1.909 -0.753 1961 3 7.615 -0.848 0 0 6.813 -1.650 6.295 -1.030 1961 4 14.059 1.294 0 0 13.258 0.493 11.772 0.144 1961 5 17.253 0.856 0 0 16.452 0.054 15.165 -0.095 1961 6 20.602 1.683 0 0 19.800 0.881 18.260 0.478 1961 7 22.491 1.394 0 0 21.689 0.592 20.493 0.533 1961 8 22.163 1.408 0 0 21.362 0.606 20.514 0.896 1961 9 18.753 1.637 0 0 17.951 0.835 16.437 0.458 1961 10 13.831 1.364 0 0 13.030 0.563 12.055 0.725 1961 11 NaN NaN NaN NaN NaN NaN 6.529 0.203 1961 12 NaN NaN NaN NaN NaN NaN 1.020 -0.559 1962 1 NaN NaN NaN NaN NaN NaN -1.029 -1.209 1962 2 NaN NaN NaN NaN NaN NaN 4.211 1.549 1962 3 NaN NaN NaN NaN NaN NaN 6.963 -0.363 1962 4 NaN NaN NaN NaN NaN NaN 11.422 -0.205 1962 5 NaN NaN NaN NaN NaN NaN 14.593 -0.667 1962 6 NaN NaN NaN NaN NaN NaN 17.349 -0.433 1962 7 NaN NaN NaN NaN NaN NaN 20.373 0.413 1962 8 NaN NaN NaN NaN NaN NaN 18.851 -0.767 1962 9 NaN NaN NaN NaN NaN NaN 16.093 0.114 1962 10 NaN NaN NaN NaN NaN NaN 11.759 0.429