% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 12454 % Primary Name: TAO-AN /PAICHENTZE % Record Type: TAVG % Country: China % Latitude: 45.63300 +/- 0.00050 % Longitude: 122.85000 +/- 0.00050 % Elevation (m): 150.90 +/- 0.05 % # of Months: 63 % % IDs: gsod - 509360-99999 % usaf - 509360 % % Sources: Global Summary of the Day % % Site Hash: 776db16ff96ef55e377cbe69b080edcb % Raw Data Hash: e2facf93fe75e4f5ff95bff5d54a3254 % Adj Data Hash: 2177db9b386aef45f7ca74b29889069e % % 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 23.677 1.903 1955 9 NaN NaN NaN NaN NaN NaN 15.827 0.805 1955 10 NaN NaN NaN NaN NaN NaN 6.263 0.383 1955 11 NaN NaN NaN NaN NaN NaN -4.522 0.960 1955 12 NaN NaN NaN NaN NaN NaN -9.683 4.821 1956 1 NaN NaN NaN NaN NaN NaN -19.125 -2.000 1956 2 NaN NaN NaN NaN NaN NaN -16.202 -2.963 1956 3 NaN NaN NaN NaN NaN NaN -6.276 -2.326 1956 4 NaN NaN NaN NaN NaN NaN 4.789 -1.603 1956 5 NaN NaN NaN NaN NaN NaN 14.752 -0.217 1956 6 NaN NaN NaN NaN NaN NaN 20.060 -0.717 1956 7 NaN NaN NaN NaN NaN NaN 22.514 -1.099 1956 8 21.058 -0.613 1 0 NaN NaN 22.128 0.355 1956 9 14.798 -0.121 1 0 NaN NaN 15.139 0.118 1956 10 5.507 -0.271 1 0 NaN NaN 6.628 0.748 1956 11 -8.391 -2.806 0 0 -8.391 -2.806 -9.008 -3.526 1956 12 -17.780 -3.174 0 0 -17.780 -3.174 -18.388 -3.885 1957 1 -15.056 2.172 0 0 -15.056 2.172 -15.623 1.502 1957 2 -15.890 -2.548 1 0 NaN NaN -17.768 -4.528 1957 3 -7.964 -3.912 0 0 -7.964 -3.912 -9.111 -5.161 1957 4 6.946 0.656 0 0 6.946 0.656 6.861 0.469 1957 5 14.871 0.005 0 0 14.871 0.005 14.976 0.007 1957 6 20.724 0.049 0 0 20.724 0.049 20.823 0.046 1957 7 21.228 -2.283 0 0 21.228 -2.283 21.834 -1.778 1957 8 19.869 -1.802 0 0 19.869 -1.802 20.316 -1.458 1957 9 13.124 -1.795 0 0 13.124 -1.795 12.609 -2.412 1957 10 6.125 0.347 0 0 6.125 0.347 6.497 0.617 1957 11 -3.191 2.394 0 0 -3.191 2.394 -2.969 2.513 1957 12 -12.599 2.007 0 0 -12.599 2.007 -13.239 1.264 1958 1 -16.306 0.921 0 0 -16.306 0.921 -17.357 -0.232 1958 2 -12.198 1.143 0 0 -12.198 1.143 -13.604 -0.364 1958 3 -4.787 -0.735 0 0 -4.787 -0.735 -5.577 -1.628 1958 4 5.357 -0.932 0 0 5.357 -0.932 5.583 -0.809 1958 5 14.609 -0.257 0 0 14.609 -0.257 14.787 -0.181 1958 6 20.753 0.078 0 0 20.753 0.078 20.903 0.126 1958 7 24.208 0.698 0 0 24.208 0.698 24.580 0.967 1958 8 20.330 -1.341 0 0 20.330 -1.341 20.880 -0.893 1958 9 14.822 -0.097 0 0 14.822 -0.097 15.002 -0.020 1958 10 5.206 -0.572 0 0 5.206 -0.572 5.797 -0.084 1958 11 -3.933 1.651 0 0 -3.933 1.651 -3.322 2.160 1958 12 -11.116 3.489 0 0 -11.116 3.489 -10.628 3.875 1959 1 -16.498 0.729 0 0 -16.498 0.729 -16.132 0.993 1959 2 -9.296 4.046 0 0 -9.296 4.046 -9.413 3.826 1959 3 0.903 4.955 0 0 0.903 4.955 0.661 4.610 1959 4 6.493 0.203 0 0 6.493 0.203 7.321 0.929 1959 5 15.004 0.138 0 0 15.004 0.138 15.541 0.573 1959 6 19.819 -0.856 0 0 19.819 -0.856 20.013 -0.764 1959 7 22.376 -1.134 0 0 22.376 -1.134 22.876 -0.737 1959 8 21.799 0.128 0 0 21.799 0.128 22.457 0.684 1959 9 15.569 0.649 0 0 15.569 0.649 15.871 0.850 1959 10 6.955 1.177 0 0 6.955 1.177 7.470 1.590 1959 11 -7.378 -1.793 0 0 -7.378 -1.793 -6.901 -1.419 1959 12 -13.518 1.087 0 0 -13.518 1.087 -13.384 1.119 1960 1 -18.758 -1.530 0 0 -18.758 -1.530 -18.458 -1.332 1960 2 -8.657 4.684 0 0 -8.657 4.684 -9.022 4.218 1960 3 -3.943 0.109 0 0 -3.943 0.109 -4.227 -0.277 1960 4 5.876 -0.414 0 0 5.876 -0.414 5.874 -0.518 1960 5 13.002 -1.864 0 0 13.002 -1.864 13.022 -1.946 1960 6 19.361 -1.314 0 0 19.361 -1.314 19.583 -1.194 1960 7 23.683 0.172 0 0 23.683 0.172 23.805 0.193 1960 8 21.624 -0.047 0 0 21.624 -0.047 22.081 0.308 1960 9 15.274 0.355 0 0 15.274 0.355 15.428 0.407 1960 10 5.280 -0.499 0 0 5.280 -0.499 6.141 0.261 1960 11 -6.131 -0.547 0 0 -6.131 -0.547 -5.492 -0.010 1960 12 -17.237 -2.631 0 0 -17.237 -2.631 -16.157 -1.653 1961 1 -17.857 -0.629 0 0 -17.857 -0.629 -17.271 -0.146 1961 2 -11.268 2.074 0 0 -11.268 2.074 -12.150 1.089 1961 3 -2.461 1.591 0 0 -2.461 1.591 -2.587 1.363 1961 4 7.509 1.219 0 0 7.509 1.219 7.499 1.107 1961 5 14.025 -0.841 0 0 14.025 -0.841 14.032 -0.937 1961 6 22.126 1.451 0 0 22.126 1.451 21.781 1.004 1961 7 23.219 -0.292 0 0 23.219 -0.292 23.749 0.137 1961 8 21.319 -0.352 0 0 21.319 -0.352 21.925 0.152 1961 9 15.978 1.059 0 0 15.978 1.059 15.855 0.833 1961 10 5.376 -0.402 0 0 5.376 -0.402 6.033 0.152 1961 11 NaN NaN NaN NaN NaN NaN -2.941 2.542 1961 12 NaN NaN NaN NaN NaN NaN -13.587 0.916 1962 1 NaN NaN NaN NaN NaN NaN -13.919 3.206 1962 2 NaN NaN NaN NaN NaN NaN -10.821 2.419 1962 3 NaN NaN NaN NaN NaN NaN -5.282 -1.332 1962 4 NaN NaN NaN NaN NaN NaN 6.711 0.319 1962 5 NaN NaN NaN NaN NaN NaN 14.146 -0.822 1962 6 NaN NaN NaN NaN NaN NaN 20.675 -0.102 1962 7 NaN NaN NaN NaN NaN NaN 23.693 0.080 1962 8 NaN NaN NaN NaN NaN NaN 21.870 0.097 1962 9 NaN NaN NaN NaN NaN NaN 14.896 -0.125 1962 10 NaN NaN NaN NaN NaN NaN 5.452 -0.429