% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 22101 % Primary Name: GORA KHAVTANDZHA % Record Type: TAVG % Country: Russia % Latitude: 68.85000 +/- 0.00050 % Longitude: 127.36700 +/- 0.00050 % Elevation (m): 696.80 +/- 512.20 % # of Months: 51 % % IDs: gsod - 241520-99999 % usaf - 241520 % % Sources: Global Summary of the Day % % Site Hash: 4aa70126d89ca4f38cc517e0a3328889 % Raw Data Hash: a3bf27ab171d308a15c3bbe8e67a6c7a % Adj Data Hash: dcaa1c0f4a17af31498dd767e8c4e972 % % 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 -41.425 -1.423 1958 2 NaN NaN NaN NaN NaN NaN -37.392 -1.351 1958 3 NaN NaN NaN NaN NaN NaN -30.215 -4.946 1958 4 NaN NaN NaN NaN NaN NaN -15.421 -1.787 1958 5 NaN NaN NaN NaN NaN NaN -2.913 -2.215 1958 6 NaN NaN NaN NaN NaN NaN 8.521 -2.033 1958 7 NaN NaN NaN NaN NaN NaN 15.500 1.181 1958 8 NaN NaN NaN NaN NaN NaN 10.459 -0.128 1958 9 NaN NaN NaN NaN NaN NaN 3.611 1.499 1958 10 NaN NaN NaN NaN NaN NaN -14.673 -1.303 1958 11 NaN NaN NaN NaN NaN NaN -38.146 -6.050 1958 12 NaN NaN NaN NaN NaN NaN -38.859 -1.074 1959 1 -43.411 -4.613 1 0 NaN NaN -42.450 -2.448 1959 2 -27.736 7.101 1 0 NaN NaN -33.538 2.503 1959 3 -17.500 6.565 1 0 NaN NaN -17.462 7.807 1959 4 -15.973 -3.543 1 0 NaN NaN -14.463 -0.829 1959 5 NaN NaN NaN NaN NaN NaN -1.173 -0.475 1959 6 NaN NaN NaN NaN NaN NaN 13.688 3.134 1959 7 14.278 -1.245 1 0 NaN NaN 13.272 -1.047 1959 8 NaN NaN NaN NaN NaN NaN 10.668 0.081 1959 9 0.692 -2.624 1 0 NaN NaN 4.441 2.329 1959 10 -12.711 -0.544 1 0 NaN NaN -11.807 1.563 1959 11 -25.971 4.922 1 0 NaN NaN -27.172 4.924 1959 12 -38.111 -1.530 0 0 -38.111 -1.530 -38.589 -0.804 1960 1 -43.188 -4.390 1 0 NaN NaN -41.225 -1.224 1960 2 NaN NaN NaN NaN NaN NaN -39.462 -3.421 1960 3 NaN NaN NaN NaN NaN NaN -26.592 -1.323 1960 4 NaN NaN NaN NaN NaN NaN -13.149 0.485 1960 5 NaN NaN NaN NaN NaN NaN -0.359 0.339 1960 6 NaN NaN NaN NaN NaN NaN 13.330 2.776 1960 7 NaN NaN NaN NaN NaN NaN 14.766 0.448 1960 8 11.480 -0.310 1 0 NaN NaN 8.899 -1.688 1960 9 2.479 -0.837 1 0 NaN NaN 1.480 -0.632 1960 10 -15.461 -3.295 1 0 NaN NaN -14.473 -1.103 1960 11 -30.936 -0.043 1 0 NaN NaN -35.871 -3.775 1960 12 -40.504 -3.923 1 0 NaN NaN -37.654 0.130 1961 1 -45.009 -6.211 0 2 -45.009 -6.211 -45.331 -5.329 1961 2 -32.993 1.844 0 0 -32.993 1.844 -35.519 0.522 1961 3 -26.017 -1.952 0 0 -26.017 -1.952 -26.358 -1.090 1961 4 -14.841 -2.411 0 0 -14.841 -2.411 -15.542 -1.908 1961 5 -0.491 -0.997 0 0 -0.491 -0.997 -2.146 -1.448 1961 6 12.004 0.246 0 0 12.004 0.246 11.258 0.704 1961 7 13.671 -1.851 1 0 NaN NaN 14.199 -0.120 1961 8 9.547 -2.244 0 0 9.547 -2.244 7.928 -2.659 1961 9 6.427 3.111 0 0 6.427 3.111 4.838 2.726 1961 10 -12.835 -0.669 0 0 -12.835 -0.669 -12.582 0.788 1961 11 -30.478 0.414 0 0 -30.478 0.414 -32.980 -0.884 1961 12 -35.603 0.978 0 0 -35.603 0.978 -34.494 3.291 1962 1 -31.395 7.403 0 0 -31.395 7.403 -34.809 5.193 1962 2 -35.631 -0.793 1 0 NaN NaN -33.913 2.128 1962 3 -25.493 -1.428 0 0 -25.493 -1.428 -24.988 0.281 1962 4 -11.246 1.184 0 0 -11.246 1.184 -12.813 0.821 1962 5 0.722 0.216 0 0 0.722 0.216 -1.092 -0.394 1962 6 9.222 -2.536 0 0 9.222 -2.536 8.302 -2.252 1962 7 14.510 -1.013 0 0 14.510 -1.013 13.402 -0.916 1962 8 12.932 1.141 0 0 12.932 1.141 10.594 0.007 1962 9 0.707 -2.609 0 0 0.707 -2.609 0.765 -1.348 1962 10 -9.353 2.814 0 0 -9.353 2.814 -10.362 3.008 1962 11 -35.109 -4.216 0 0 -35.109 -4.216 -36.680 -4.584 1962 12 -37.286 -0.705 0 0 -37.286 -0.705 -38.119 -0.335 1963 1 -33.905 4.892 0 0 -33.905 4.892 -35.325 4.676 1963 2 -27.370 7.468 0 0 -27.370 7.468 -31.524 4.517 1963 3 -21.335 2.730 0 0 -21.335 2.730 -22.194 3.075 1963 4 -15.320 -2.890 0 0 -15.320 -2.890 -16.365 -2.731 1963 5 -5.151 -5.656 0 0 -5.151 -5.656 -6.149 -5.451 1963 6 8.617 -3.141 0 0 8.617 -3.141 8.287 -2.267 1963 7 14.135 -1.387 0 0 14.135 -1.387 13.886 -0.433 1963 8 12.254 0.463 0 0 12.254 0.463 10.234 -0.353 1963 9 2.234 -1.082 0 0 2.234 -1.082 1.926 -0.186 1963 10 -10.705 1.461 0 0 -10.705 1.461 -11.941 1.429 1963 11 -26.603 4.289 0 0 -26.603 4.289 -30.540 1.556 1963 12 -35.134 1.446 0 0 -35.134 1.446 -35.585 2.200 1964 1 NaN NaN NaN NaN NaN NaN -36.401 3.601 1964 2 NaN NaN NaN NaN NaN NaN -32.004 4.037 1964 3 NaN NaN NaN NaN NaN NaN -25.886 -0.618 1964 4 NaN NaN NaN NaN NaN NaN -14.881 -1.247 1964 5 NaN NaN NaN NaN NaN NaN -3.079 -2.381 1964 6 NaN NaN NaN NaN NaN NaN 11.953 1.399 1964 7 NaN NaN NaN NaN NaN NaN 14.796 0.477 1964 8 NaN NaN NaN NaN NaN NaN 8.979 -1.608 1964 9 NaN NaN NaN NaN NaN NaN 1.123 -0.989 1964 10 NaN NaN NaN NaN NaN NaN -14.322 -0.952 1964 11 NaN NaN NaN NaN NaN NaN -35.356 -3.259 1964 12 NaN NaN NaN NaN NaN NaN -38.303 -0.518