% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 12297 % Primary Name: BAOTOU % Record Type: TAVG % Country: China % Latitude: 40.56700 +/- 0.00050 % Longitude: 109.98300 +/- 0.00050 % Elevation (m): 940.00 +/- 0.05 % # of Months: 63 % % IDs: gsod - 534460-99999 % icao - ZBOW % usaf - 534460 % % Sources: Global Summary of the Day % % Site Hash: 1cfd784ea393d02ee5ac91bc4045b8f9 % Raw Data Hash: 59857d56ce588bd84e5fba9ae7470401 % Adj Data Hash: 1a0ca0b2b55b201d09cc6e9ee5ba1cfe % % 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 21.222 2.125 1955 9 NaN NaN NaN NaN NaN NaN 14.202 1.190 1955 10 NaN NaN NaN NaN NaN NaN 4.829 -0.757 1955 11 NaN NaN NaN NaN NaN NaN -4.030 -0.214 1955 12 NaN NaN NaN NaN NaN NaN -9.712 2.552 1956 1 NaN NaN NaN NaN NaN NaN -14.016 0.254 1956 2 NaN NaN NaN NaN NaN NaN -12.071 -1.734 1956 3 NaN NaN NaN NaN NaN NaN -1.726 0.123 1956 4 NaN NaN NaN NaN NaN NaN 6.632 0.243 1956 5 NaN NaN NaN NaN NaN NaN 12.811 -1.032 1956 6 NaN NaN NaN NaN NaN NaN 17.415 -1.495 1956 7 NaN NaN NaN NaN NaN NaN 19.580 -1.438 1956 8 18.371 -2.615 1 0 NaN NaN 18.443 -0.655 1956 9 16.019 1.118 0 0 16.019 1.118 13.674 0.662 1956 10 7.188 -0.287 0 0 7.188 -0.287 5.674 0.088 1956 11 -5.264 -3.337 0 0 -5.264 -3.337 -6.993 -3.177 1956 12 -12.500 -2.125 0 0 -12.500 -2.125 -15.106 -2.842 1957 1 -14.659 -2.279 0 0 -14.659 -2.279 -14.982 -0.712 1957 2 -12.204 -3.757 0 0 -12.204 -3.757 -14.871 -4.535 1957 3 0.333 0.294 0 0 0.333 0.294 -2.566 -0.716 1957 4 8.307 0.030 0 0 8.307 0.030 6.563 0.174 1957 5 13.322 -2.409 0 0 13.322 -2.409 11.723 -2.120 1957 6 19.690 -1.109 0 0 19.690 -1.109 17.859 -1.051 1957 7 21.878 -1.028 0 0 21.878 -1.028 20.068 -0.950 1957 8 20.495 -0.492 0 0 20.495 -0.492 19.328 0.231 1957 9 12.139 -2.762 0 0 12.139 -2.762 10.351 -2.661 1957 10 6.554 -0.921 0 0 6.554 -0.921 5.390 -0.196 1957 11 -0.522 1.405 0 0 -0.522 1.405 -1.711 2.104 1957 12 -9.090 1.286 0 0 -9.090 1.286 -10.963 1.301 1958 1 -13.147 -0.766 0 0 -13.147 -0.766 -14.962 -0.692 1958 2 -7.784 0.664 0 0 -7.784 0.664 -10.608 -0.271 1958 3 0.002 -0.037 0 0 0.002 -0.037 -1.786 0.064 1958 4 9.493 1.215 0 0 9.493 1.215 7.413 1.025 1958 5 16.292 0.561 0 0 16.292 0.561 14.185 0.343 1958 6 21.846 1.048 0 0 21.846 1.048 19.517 0.607 1958 7 23.201 0.294 0 0 23.201 0.294 21.519 0.501 1958 8 18.977 -2.010 0 0 18.977 -2.010 17.298 -1.799 1958 9 16.024 1.124 0 0 16.024 1.124 13.870 0.859 1958 10 6.812 -0.663 0 0 6.812 -0.663 5.139 -0.448 1958 11 -2.137 -0.210 0 0 -2.137 -0.210 -3.806 0.010 1958 12 -6.815 3.560 0 0 -6.815 3.560 -8.196 4.068 1959 1 -12.237 0.144 0 0 -12.237 0.144 -14.207 0.063 1959 2 -6.377 2.071 0 0 -6.377 2.071 -9.276 1.060 1959 3 1.421 1.382 0 0 1.421 1.382 -0.524 1.325 1959 4 8.863 0.586 0 0 8.863 0.586 6.731 0.342 1959 5 15.432 -0.299 0 0 15.432 -0.299 13.539 -0.304 1959 6 19.750 -1.049 0 0 19.750 -1.049 17.544 -1.366 1959 7 22.306 -0.600 0 0 22.306 -0.600 20.457 -0.561 1959 8 20.228 -0.759 0 0 20.228 -0.759 18.625 -0.472 1959 9 14.131 -0.769 0 0 14.131 -0.769 11.535 -1.476 1959 10 9.536 2.061 0 0 9.536 2.061 7.793 2.207 1959 11 -4.646 -2.719 0 0 -4.646 -2.719 -5.803 -1.988 1959 12 -10.525 -0.150 0 0 -10.525 -0.150 -12.297 -0.033 1960 1 -11.920 0.460 0 0 -11.920 0.460 -13.473 0.796 1960 2 -4.015 4.432 0 0 -4.015 4.432 -6.090 4.246 1960 3 1.952 1.913 0 0 1.952 1.913 0.415 2.265 1960 4 8.352 0.075 0 0 8.352 0.075 5.882 -0.506 1960 5 14.530 -1.201 0 0 14.530 -1.201 12.595 -1.247 1960 6 21.931 1.133 0 0 21.931 1.133 19.294 0.384 1960 7 23.869 0.963 0 0 23.869 0.963 21.957 0.939 1960 8 21.061 0.075 0 0 21.061 0.075 19.679 0.582 1960 9 15.981 1.081 0 0 15.981 1.081 13.832 0.820 1960 10 7.783 0.309 0 0 7.783 0.309 6.020 0.434 1960 11 -2.491 -0.564 0 0 -2.491 -0.564 -4.011 -0.195 1960 12 -12.864 -2.488 0 0 -12.864 -2.488 -14.633 -2.369 1961 1 -12.502 -0.121 0 0 -12.502 -0.121 -13.965 0.305 1961 2 -6.357 2.091 0 0 -6.357 2.091 -8.919 1.417 1961 3 2.317 2.278 0 0 2.317 2.278 0.052 1.901 1961 4 10.298 2.021 0 0 10.298 2.021 8.315 1.926 1961 5 16.159 0.428 0 0 16.159 0.428 13.837 -0.006 1961 6 21.774 0.976 0 0 21.774 0.976 19.875 0.965 1961 7 23.036 0.129 0 0 23.036 0.129 21.495 0.477 1961 8 20.305 -0.682 0 0 20.305 -0.682 19.022 -0.075 1961 9 14.222 -0.678 0 0 14.222 -0.678 12.238 -0.773 1961 10 8.208 0.733 0 0 8.208 0.733 6.306 0.720 1961 11 NaN NaN NaN NaN NaN NaN -1.398 2.418 1961 12 NaN NaN NaN NaN NaN NaN -12.751 -0.487 1962 1 NaN NaN NaN NaN NaN NaN -15.817 -1.548 1962 2 NaN NaN NaN NaN NaN NaN -9.806 0.530 1962 3 NaN NaN NaN NaN NaN NaN -3.572 -1.722 1962 4 NaN NaN NaN NaN NaN NaN 4.538 -1.850 1962 5 NaN NaN NaN NaN NaN NaN 13.129 -0.714 1962 6 NaN NaN NaN NaN NaN NaN 17.759 -1.150 1962 7 NaN NaN NaN NaN NaN NaN 19.838 -1.179 1962 8 NaN NaN NaN NaN NaN NaN 20.385 1.287 1962 9 NaN NaN NaN NaN NaN NaN 13.017 0.005 1962 10 NaN NaN NaN NaN NaN NaN 6.168 0.582