% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 12470 % Primary Name: CHIA-MU-SSU /CHIAMUEZE % Record Type: TAVG % Country: China % Latitude: 46.81700 +/- 0.00050 % Longitude: 130.33300 +/- 0.00050 % Elevation (m): 80.20 +/- 0.05 % # of Months: 63 % % IDs: gsod - 508730-99999 % usaf - 508730 % % Sources: Global Summary of the Day % % Site Hash: 419cf2ab33ff59585ecc8d1a0795f9d5 % Raw Data Hash: 96881d866c50a8359573d9b3807c2250 % Adj Data Hash: 05e527bd27d7c5504f9d298aca232881 % % 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 21.266 1.262 1955 9 NaN NaN NaN NaN NaN NaN 13.522 -0.031 1955 10 NaN NaN NaN NaN NaN NaN 4.927 0.410 1955 11 NaN NaN NaN NaN NaN NaN -6.652 0.945 1955 12 NaN NaN NaN NaN NaN NaN -13.059 4.647 1956 1 NaN NaN NaN NaN NaN NaN -22.019 -1.385 1956 2 NaN NaN NaN NaN NaN NaN -19.456 -2.898 1956 3 NaN NaN NaN NaN NaN NaN -9.086 -2.295 1956 4 NaN NaN NaN NaN NaN NaN 2.876 -1.288 1956 5 NaN NaN NaN NaN NaN NaN 12.406 0.028 1956 6 NaN NaN NaN NaN NaN NaN 17.593 -0.548 1956 7 NaN NaN NaN NaN NaN NaN 19.764 -1.740 1956 8 19.049 -1.577 1 0 NaN NaN 19.820 -0.185 1956 9 14.934 0.760 1 0 NaN NaN 13.974 0.420 1956 10 5.807 0.669 1 0 NaN NaN 5.742 1.225 1956 11 -9.352 -2.376 0 0 -9.352 -2.376 -9.717 -2.120 1956 12 -19.152 -2.067 0 0 -19.152 -2.067 -20.313 -2.607 1957 1 -17.321 2.692 0 0 -17.321 2.692 -17.933 2.700 1957 2 -17.871 -1.933 0 0 -17.871 -1.933 -18.314 -1.755 1957 3 -9.546 -3.375 0 0 -9.546 -3.375 -10.453 -3.661 1957 4 4.731 -0.053 0 0 4.731 -0.053 4.283 0.119 1957 5 13.357 0.359 0 0 13.357 0.359 12.983 0.606 1957 6 16.946 -1.814 0 0 16.946 -1.814 16.810 -1.331 1957 7 21.034 -1.091 0 0 21.034 -1.091 21.014 -0.490 1957 8 19.000 -1.625 0 0 19.000 -1.625 18.770 -1.235 1957 9 12.083 -2.091 0 0 12.083 -2.091 11.742 -1.812 1957 10 5.319 0.181 0 0 5.319 0.181 5.168 0.651 1957 11 -4.433 2.543 0 0 -4.433 2.543 -4.782 2.815 1957 12 -17.065 0.020 0 0 -17.065 0.020 -16.750 0.955 1958 1 -21.991 -1.978 0 0 -21.991 -1.978 -21.629 -0.996 1958 2 -17.067 -1.129 0 0 -17.067 -1.129 -16.694 -0.136 1958 3 -9.541 -3.370 0 0 -9.541 -3.370 -10.164 -3.373 1958 4 3.904 -0.881 0 0 3.904 -0.881 3.103 -1.061 1958 5 12.220 -0.778 0 0 12.220 -0.778 11.658 -0.719 1958 6 19.319 0.558 0 0 19.319 0.558 18.095 -0.046 1958 7 22.722 0.597 0 0 22.722 0.597 22.518 1.013 1958 8 19.181 -1.444 0 0 19.181 -1.444 19.096 -0.908 1958 9 14.415 0.241 0 0 14.415 0.241 13.655 0.102 1958 10 4.647 -0.491 0 0 4.647 -0.491 4.842 0.325 1958 11 -4.026 2.950 0 0 -4.026 2.950 -5.515 2.082 1958 12 -14.590 2.495 0 0 -14.590 2.495 -14.474 3.231 1959 1 -20.647 -0.634 0 0 -20.647 -0.634 -21.142 -0.508 1959 2 -10.085 5.853 0 0 -10.085 5.853 -12.081 4.478 1959 3 -0.158 6.013 0 0 -0.158 6.013 -1.098 5.693 1959 4 5.293 0.508 0 0 5.293 0.508 4.886 0.722 1959 5 13.814 0.816 0 0 13.814 0.816 12.925 0.547 1959 6 18.015 -0.746 0 0 18.015 -0.746 17.534 -0.606 1959 7 19.793 -2.332 0 0 19.793 -2.332 19.481 -2.023 1959 8 21.351 0.726 0 0 21.351 0.726 21.382 1.378 1959 9 15.402 1.228 0 0 15.402 1.228 15.132 1.578 1959 10 6.749 1.612 0 0 6.749 1.612 6.748 2.231 1959 11 -6.707 0.269 0 0 -6.707 0.269 -7.638 -0.042 1959 12 -15.792 1.293 0 0 -15.792 1.293 -17.009 0.696 1960 1 -22.027 -2.014 0 0 -22.027 -2.014 -22.263 -1.629 1960 2 -12.276 3.662 1 0 NaN NaN -14.200 2.359 1960 3 -5.378 0.793 0 0 -5.378 0.793 -7.441 -0.649 1960 4 3.841 -0.944 0 0 3.841 -0.944 3.087 -1.076 1960 5 10.670 -2.328 0 0 10.670 -2.328 10.261 -2.117 1960 6 17.344 -1.416 0 0 17.344 -1.416 16.290 -1.850 1960 7 21.656 -0.469 0 0 21.656 -0.469 21.547 0.043 1960 8 20.812 0.187 0 0 20.812 0.187 20.433 0.428 1960 9 14.783 0.609 0 0 14.783 0.609 13.611 0.058 1960 10 4.059 -1.078 0 0 4.059 -1.078 4.061 -0.456 1960 11 -6.707 0.269 0 0 -6.707 0.269 -7.458 0.138 1960 12 -17.536 -0.451 0 0 -17.536 -0.451 -19.540 -1.834 1961 1 -20.391 -0.378 0 0 -20.391 -0.378 -21.413 -0.779 1961 2 -15.645 0.293 0 0 -15.645 0.293 -16.491 0.067 1961 3 -4.389 1.782 0 0 -4.389 1.782 -6.146 0.645 1961 4 5.798 1.014 0 0 5.798 1.014 4.894 0.730 1961 5 12.692 -0.306 0 0 12.692 -0.306 11.710 -0.667 1961 6 20.844 2.084 0 0 20.844 2.084 18.839 0.699 1961 7 23.203 1.078 0 0 23.203 1.078 21.977 0.473 1961 8 20.659 0.034 0 0 20.659 0.034 20.209 0.205 1961 9 15.678 1.504 0 0 15.678 1.504 14.888 1.334 1961 10 4.645 -0.492 0 0 4.645 -0.492 4.780 0.263 1961 11 NaN NaN NaN NaN NaN NaN -5.450 2.147 1961 12 NaN NaN NaN NaN NaN NaN -14.638 3.068 1962 1 NaN NaN NaN NaN NaN NaN -17.989 2.644 1962 2 NaN NaN NaN NaN NaN NaN -15.353 1.206 1962 3 NaN NaN NaN NaN NaN NaN -8.116 -1.324 1962 4 NaN NaN NaN NaN NaN NaN 5.363 1.199 1962 5 NaN NaN NaN NaN NaN NaN 12.623 0.245 1962 6 NaN NaN NaN NaN NaN NaN 17.642 -0.498 1962 7 NaN NaN NaN NaN NaN NaN 21.032 -0.472 1962 8 NaN NaN NaN NaN NaN NaN 19.498 -0.507 1962 9 NaN NaN NaN NaN NaN NaN 13.485 -0.068 1962 10 NaN NaN NaN NaN NaN NaN 4.530 0.013