% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 21411 % Primary Name: PRUSK TYRKANDA % Record Type: TAVG % Country: Russia % Latitude: 57.80000 +/- 0.00050 % Longitude: 127.88300 +/- 0.00050 % Elevation (m): 875.60 +/- 277.99 % # of Months: 45 % % IDs: gsod - 311120-99999 % usaf - 311120 % % Sources: Global Summary of the Day % % Site Hash: f49934efa267b182ed6b5132e307c004 % Raw Data Hash: 6081282d189b7fdbddeea187195fae95 % Adj Data Hash: 98a8a453112182fc2b1effc341a1da40 % % 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 1958 1 NaN NaN NaN NaN NaN NaN -37.312 -1.797 1958 2 NaN NaN NaN NaN NaN NaN -30.838 0.521 1958 3 NaN NaN NaN NaN NaN NaN -23.824 -2.762 1958 4 NaN NaN NaN NaN NaN NaN -9.614 -0.595 1958 5 NaN NaN NaN NaN NaN NaN 1.997 0.062 1958 6 NaN NaN NaN NaN NaN NaN 7.817 -2.382 1958 7 NaN NaN NaN NaN NaN NaN 13.097 -0.546 1958 8 NaN NaN NaN NaN NaN NaN 11.108 0.116 1958 9 NaN NaN NaN NaN NaN NaN 3.503 0.595 1958 10 NaN NaN NaN NaN NaN NaN -8.339 1.352 1958 11 NaN NaN NaN NaN NaN NaN -22.916 2.311 1958 12 NaN NaN NaN NaN NaN NaN -33.231 0.658 1959 1 -34.776 -1.423 1 0 NaN NaN -37.583 -2.068 1959 2 -21.261 7.936 1 0 NaN NaN -27.718 3.641 1959 3 NaN NaN NaN NaN NaN NaN -15.859 5.202 1959 4 NaN NaN NaN NaN NaN NaN -7.768 1.251 1959 5 NaN NaN NaN NaN NaN NaN 1.720 -0.215 1959 6 NaN NaN NaN NaN NaN NaN 11.600 1.401 1959 7 12.938 -2.866 1 0 NaN NaN 11.806 -1.836 1959 8 11.721 -1.433 1 0 NaN NaN 14.100 3.108 1959 9 5.532 0.463 1 0 NaN NaN 6.218 3.311 1959 10 -9.261 -1.731 1 0 NaN NaN -7.344 2.347 1959 11 -20.364 2.701 1 0 NaN NaN -24.728 0.499 1959 12 -28.523 3.204 1 0 NaN NaN -31.798 2.090 1960 1 -34.477 -1.123 1 0 NaN NaN -38.839 -3.324 1960 2 NaN NaN NaN NaN NaN NaN -31.339 0.019 1960 3 NaN NaN NaN NaN NaN NaN -24.505 -3.443 1960 4 NaN NaN NaN NaN NaN NaN -10.793 -1.774 1960 5 NaN NaN NaN NaN NaN NaN 0.455 -1.480 1960 6 NaN NaN NaN NaN NaN NaN 10.436 0.237 1960 7 NaN NaN NaN NaN NaN NaN 14.654 1.011 1960 8 6.111 -7.043 1 0 NaN NaN 11.573 0.581 1960 9 NaN NaN NaN NaN NaN NaN 2.207 -0.701 1960 10 NaN NaN NaN NaN NaN NaN -10.587 -0.896 1960 11 NaN NaN NaN NaN NaN NaN -25.732 -0.506 1960 12 -38.001 -6.274 1 0 NaN NaN -34.139 -0.250 1961 1 -32.960 0.393 1 0 NaN NaN -39.229 -3.714 1961 2 -24.338 4.859 1 0 NaN NaN -29.645 1.713 1961 3 -17.932 0.968 1 0 NaN NaN -20.607 0.455 1961 4 -9.119 -2.261 0 0 -9.119 -2.261 -9.528 -0.509 1961 5 1.115 -2.982 0 0 1.115 -2.982 0.776 -1.160 1961 6 9.680 -2.681 0 0 9.680 -2.681 8.578 -1.621 1961 7 13.504 -2.300 0 0 13.504 -2.300 12.800 -0.842 1961 8 12.506 -0.648 0 0 12.506 -0.648 11.894 0.902 1961 9 4.895 -0.175 0 0 4.895 -0.175 3.943 1.035 1961 10 -9.728 -2.198 1 0 NaN NaN -9.103 0.589 1961 11 -18.984 4.081 0 0 -18.984 4.081 -22.831 2.395 1961 12 -26.784 4.943 0 0 -26.784 4.943 -31.182 2.706 1962 1 -22.776 10.577 0 0 -22.776 10.577 -30.187 5.328 1962 2 -23.408 5.789 0 0 -23.408 5.789 -29.047 2.312 1962 3 -21.775 -2.875 1 0 NaN NaN -22.207 -1.145 1962 4 -7.728 -0.871 1 0 NaN NaN -7.866 1.153 1962 5 1.955 -2.142 0 0 1.955 -2.142 1.858 -0.077 1962 6 10.031 -2.329 0 0 10.031 -2.329 9.647 -0.552 1962 7 16.359 0.555 0 0 16.359 0.555 15.199 1.557 1962 8 12.196 -0.958 0 0 12.196 -0.958 10.741 -0.251 1962 9 2.636 -2.434 0 0 2.636 -2.434 2.852 -0.055 1962 10 -8.593 -1.063 0 0 -8.593 -1.063 -8.702 0.989 1962 11 -24.063 -0.999 0 0 -24.063 -0.999 -26.936 -1.710 1962 12 -27.359 4.368 0 0 -27.359 4.368 -33.069 0.820 1963 1 -28.032 5.321 0 0 -28.032 5.321 -30.399 5.116 1963 2 -22.417 6.780 0 0 -22.417 6.780 -28.593 2.766 1963 3 -15.142 3.759 0 0 -15.142 3.759 -18.218 2.843 1963 4 -10.789 -3.932 0 0 -10.789 -3.932 -10.892 -1.873 1963 5 -2.090 -6.187 1 0 NaN NaN -0.316 -2.252 1963 6 14.055 1.695 1 0 NaN NaN 9.703 -0.496 1963 7 16.022 0.218 0 0 16.022 0.218 15.014 1.372 1963 8 9.357 -3.797 1 0 NaN NaN 12.024 1.032 1963 9 NaN NaN NaN NaN NaN NaN 3.607 0.700 1963 10 NaN NaN NaN NaN NaN NaN -7.509 2.182 1963 11 -18.197 4.868 1 0 NaN NaN -24.654 0.572 1963 12 -18.246 13.481 1 0 NaN NaN -32.625 1.264 1964 1 NaN NaN NaN NaN NaN NaN -30.305 5.210 1964 2 NaN NaN NaN NaN NaN NaN -30.793 0.566 1964 3 NaN NaN NaN NaN NaN NaN -20.024 1.037 1964 4 NaN NaN NaN NaN NaN NaN -11.567 -2.548 1964 5 NaN NaN NaN NaN NaN NaN 1.108 -0.827 1964 6 NaN NaN NaN NaN NaN NaN 8.964 -1.235 1964 7 NaN NaN NaN NaN NaN NaN 12.462 -1.180 1964 8 NaN NaN NaN NaN NaN NaN 10.480 -0.512 1964 9 NaN NaN NaN NaN NaN NaN 1.042 -1.866 1964 10 NaN NaN NaN NaN NaN NaN -9.436 0.255 1964 11 NaN NaN NaN NaN NaN NaN -25.835 -0.608 1964 12 NaN NaN NaN NaN NaN NaN -35.903 -2.014