% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 15924 % Primary Name: SARONA % Record Type: TAVG % Country: Israel % Latitude: 32.10000 +/- 0.05000 % Longitude: 34.80000 +/- 0.05000 % Elevation (m): 20.00 +/- 0.05 % # of Months: 120 % % IDs: ghcnm - 62240176002 % hadcru - 401807 % % Sources: Global Historical Climatology Network - Monthly v2 % Hadley Centre Data Release % Global Historical Climatology Network - Monthly v3 % % Site Hash: 84a9b5eb66b85a993b873449552b5cb1 % Raw Data Hash: aa7392c1b9aa4605872224bada05ab65 % Adj Data Hash: 9b51c5b9e8e92ae32510652a3a1b28f6 % % 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 1879 1 NaN NaN NaN NaN NaN NaN 11.871 1.443 1879 2 NaN NaN NaN NaN NaN NaN 13.628 2.136 1879 3 NaN NaN NaN NaN NaN NaN 13.192 -0.459 1879 4 NaN NaN NaN NaN NaN NaN 18.908 2.078 1879 5 NaN NaN NaN NaN NaN NaN 20.808 0.060 1879 6 NaN NaN NaN NaN NaN NaN 25.132 0.928 1879 7 NaN NaN NaN NaN NaN NaN 26.871 0.867 1879 8 NaN NaN NaN NaN NaN NaN 25.816 -0.538 1879 9 NaN NaN NaN NaN NaN NaN 23.956 -0.599 1879 10 NaN NaN NaN NaN NaN NaN 20.129 -1.259 1879 11 NaN NaN NaN NaN NaN NaN 16.124 -0.629 1879 12 NaN NaN NaN NaN NaN NaN 11.803 -0.194 1880 1 10.400 -1.370 0 0 10.400 -1.370 6.915 -3.512 1880 2 13.200 0.366 0 0 13.200 0.366 10.186 -1.307 1880 3 13.700 -1.294 0 0 13.700 -1.294 11.353 -2.299 1880 4 17.500 -0.673 0 0 17.500 -0.673 15.831 -0.999 1880 5 20.500 -1.590 0 0 20.500 -1.590 20.005 -0.743 1880 6 23.200 -2.346 0 0 23.200 -2.346 24.206 0.003 1880 7 25.000 -2.346 0 0 25.000 -2.346 25.541 -0.462 1880 8 26.200 -1.497 0 0 26.200 -1.497 26.149 -0.205 1880 9 24.900 -0.998 0 0 24.900 -0.998 23.655 -0.900 1880 10 23.100 0.370 0 0 23.100 0.370 21.749 0.361 1880 11 20.400 2.305 0 0 20.400 2.305 17.572 0.819 1880 12 13.800 0.461 0 0 13.800 0.461 10.009 -1.988 1881 1 15.300 3.530 0 0 15.300 3.530 11.888 1.460 1881 2 13.500 0.666 0 0 13.500 0.666 10.915 -0.577 1881 3 14.500 -0.494 0 0 14.500 -0.494 12.898 -0.754 1881 4 19.600 1.427 0 0 19.600 1.427 17.440 0.609 1881 5 20.200 -1.890 0 0 20.200 -1.890 20.060 -0.688 1881 6 21.700 -3.846 0 0 21.700 -3.846 23.185 -1.019 1881 7 24.800 -2.546 0 0 24.800 -2.546 25.245 -0.759 1881 8 26.700 -0.997 0 0 26.700 -0.997 27.270 0.916 1881 9 25.700 -0.198 0 0 25.700 -0.198 24.651 0.095 1881 10 22.400 -0.330 0 0 22.400 -0.330 20.762 -0.626 1881 11 18.600 0.505 0 0 18.600 0.505 15.410 -1.343 1881 12 13.800 0.461 0 0 13.800 0.461 10.594 -1.403 1882 1 11.300 -0.470 0 0 11.300 -0.470 8.584 -1.844 1882 2 10.000 -2.834 0 0 10.000 -2.834 8.029 -3.463 1882 3 14.400 -0.594 0 0 14.400 -0.594 13.158 -0.494 1882 4 16.900 -1.273 0 0 16.900 -1.273 15.679 -1.152 1882 5 18.500 -3.590 0 0 18.500 -3.590 18.752 -1.996 1882 6 20.800 -4.746 1 0 NaN NaN 22.781 -1.423 1882 7 23.900 -3.446 0 0 23.900 -3.446 25.191 -0.812 1882 8 25.300 -2.397 0 0 25.300 -2.397 26.018 -0.336 1882 9 24.900 -0.998 0 0 24.900 -0.998 24.540 -0.015 1882 10 22.200 -0.530 0 0 22.200 -0.530 20.060 -1.328 1882 11 19.000 0.905 0 0 19.000 0.905 16.245 -0.508 1882 12 15.500 2.161 0 0 15.500 2.161 12.091 0.094 1883 1 13.700 1.930 0 0 13.700 1.930 9.840 -0.588 1883 2 12.300 -0.534 0 0 12.300 -0.534 10.065 -1.427 1883 3 15.500 0.506 0 0 15.500 0.506 13.552 -0.100 1883 4 16.400 -1.773 0 0 16.400 -1.773 15.481 -1.349 1883 5 18.800 -3.290 0 0 18.800 -3.290 19.437 -1.311 1883 6 23.000 -2.546 0 0 23.000 -2.546 24.177 -0.027 1883 7 24.300 -3.046 0 0 24.300 -3.046 25.543 -0.461 1883 8 26.000 -1.697 0 0 26.000 -1.697 26.261 -0.093 1883 9 23.500 -2.398 0 0 23.500 -2.398 24.201 -0.355 1883 10 22.700 -0.030 0 0 22.700 -0.030 21.399 0.011 1883 11 18.000 -0.095 0 0 18.000 -0.095 15.691 -1.062 1883 12 13.500 0.161 0 0 13.500 0.161 10.692 -1.305 1884 1 10.300 -1.470 0 0 10.300 -1.470 8.172 -2.256 1884 2 11.800 -1.034 0 0 11.800 -1.034 9.431 -2.061 1884 3 14.200 -0.794 0 0 14.200 -0.794 12.279 -1.373 1884 4 18.700 0.527 0 0 18.700 0.527 16.854 0.024 1884 5 19.500 -2.590 0 0 19.500 -2.590 19.410 -1.338 1884 6 23.400 -2.146 0 0 23.400 -2.146 23.906 -0.298 1884 7 24.100 -3.246 0 0 24.100 -3.246 24.635 -1.369 1884 8 25.300 -2.397 0 0 25.300 -2.397 25.517 -0.838 1884 9 23.300 -2.598 0 0 23.300 -2.598 22.177 -2.379 1884 10 21.800 -0.930 0 0 21.800 -0.930 20.364 -1.024 1884 11 17.100 -0.995 0 0 17.100 -0.995 15.040 -1.713 1884 12 15.400 2.061 0 0 15.400 2.061 12.419 0.422 1885 1 12.500 0.730 0 0 12.500 0.730 9.300 -1.127 1885 2 13.000 0.166 0 0 13.000 0.166 11.489 -0.003 1885 3 15.300 0.306 0 0 15.300 0.306 13.654 0.003 1885 4 17.400 -0.773 0 0 17.400 -0.773 15.658 -1.173 1885 5 22.100 0.010 0 0 22.100 0.010 21.809 1.061 1885 6 23.200 -2.346 0 0 23.200 -2.346 23.678 -0.525 1885 7 25.100 -2.246 0 0 25.100 -2.246 25.662 -0.342 1885 8 25.400 -2.297 0 0 25.400 -2.297 26.095 -0.259 1885 9 25.000 -0.898 0 0 25.000 -0.898 24.039 -0.517 1885 10 23.600 0.870 0 0 23.600 0.870 21.574 0.186 1885 11 18.500 0.405 0 0 18.500 0.405 16.437 -0.316 1885 12 16.200 2.861 0 0 16.200 2.861 11.895 -0.102 1886 1 13.900 2.130 0 0 13.900 2.130 10.773 0.346 1886 2 14.400 1.566 0 0 14.400 1.566 11.520 0.028 1886 3 14.600 -0.394 0 0 14.600 -0.394 12.048 -1.604 1886 4 16.900 -1.273 0 0 16.900 -1.273 15.176 -1.654 1886 5 19.000 -3.090 0 0 19.000 -3.090 19.030 -1.718 1886 6 23.800 -1.746 0 0 23.800 -1.746 24.391 0.187 1886 7 24.300 -3.046 0 0 24.300 -3.046 24.979 -1.024 1886 8 25.900 -1.797 0 0 25.900 -1.797 26.007 -0.347 1886 9 24.900 -0.998 0 0 24.900 -0.998 23.905 -0.651 1886 10 22.400 -0.330 0 0 22.400 -0.330 20.705 -0.683 1886 11 17.200 -0.895 0 0 17.200 -0.895 14.117 -2.636 1886 12 14.500 1.161 0 0 14.500 1.161 10.958 -1.039 1887 1 12.300 0.530 0 0 12.300 0.530 8.590 -1.838 1887 2 12.300 -0.534 0 0 12.300 -0.534 10.360 -1.132 1887 3 14.000 -0.994 0 0 14.000 -0.994 12.437 -1.215 1887 4 18.600 0.427 0 0 18.600 0.427 16.886 0.056 1887 5 20.200 -1.890 0 0 20.200 -1.890 19.736 -1.012 1887 6 23.000 -2.546 0 0 23.000 -2.546 23.946 -0.258 1887 7 24.400 -2.946 0 0 24.400 -2.946 25.717 -0.287 1887 8 26.000 -1.697 0 0 26.000 -1.697 26.576 0.222 1887 9 24.800 -1.098 0 0 24.800 -1.098 23.916 -0.640 1887 10 24.400 1.670 0 0 24.400 1.670 23.420 2.032 1887 11 19.700 1.605 0 0 19.700 1.605 17.109 0.356 1887 12 15.800 2.461 0 0 15.800 2.461 11.598 -0.399 1888 1 11.900 0.130 0 0 11.900 0.130 8.694 -1.734 1888 2 14.200 1.366 0 0 14.200 1.366 11.938 0.446 1888 3 18.500 3.506 0 0 18.500 3.506 15.168 1.516 1888 4 18.200 0.027 0 0 18.200 0.027 16.484 -0.347 1888 5 20.100 -1.990 0 0 20.100 -1.990 19.431 -1.317 1888 6 22.600 -2.946 0 0 22.600 -2.946 23.131 -1.073 1888 7 26.100 -1.246 0 0 26.100 -1.246 27.299 1.295 1888 8 26.300 -1.397 0 0 26.300 -1.397 26.511 0.156 1888 9 25.100 -0.798 0 0 25.100 -0.798 24.504 -0.051 1888 10 25.500 2.770 0 0 25.500 2.770 23.092 1.703 1888 11 16.200 -1.895 0 0 16.200 -1.895 13.697 -3.056 1888 12 13.400 0.061 0 0 13.400 0.061 9.958 -2.039 1889 1 13.600 1.830 0 0 13.600 1.830 9.697 -0.730 1889 2 14.200 1.366 0 0 14.200 1.366 12.161 0.668 1889 3 17.300 2.306 0 0 17.300 2.306 14.725 1.074 1889 4 17.100 -1.073 0 0 17.100 -1.073 16.212 -0.618 1889 5 22.000 -0.090 0 0 22.000 -0.090 20.656 -0.092 1889 6 23.400 -2.146 0 0 23.400 -2.146 24.043 -0.161 1889 7 26.000 -1.346 0 0 26.000 -1.346 26.654 0.651 1889 8 26.300 -1.397 0 0 26.300 -1.397 26.801 0.446 1889 9 25.700 -0.198 0 0 25.700 -0.198 24.271 -0.285 1889 10 23.800 1.070 0 0 23.800 1.070 22.316 0.928 1889 11 15.700 -2.395 0 0 15.700 -2.395 14.130 -2.623 1889 12 14.300 0.961 0 0 14.300 0.961 10.419 -1.578 1890 1 NaN NaN NaN NaN NaN NaN 7.309 -3.119 1890 2 NaN NaN NaN NaN NaN NaN 10.228 -1.264 1890 3 NaN NaN NaN NaN NaN NaN 13.862 0.210 1890 4 NaN NaN NaN NaN NaN NaN 16.676 -0.154 1890 5 NaN NaN NaN NaN NaN NaN 21.089 0.341 1890 6 NaN NaN NaN NaN NaN NaN 24.228 0.025 1890 7 NaN NaN NaN NaN NaN NaN 26.591 0.587 1890 8 NaN NaN NaN NaN NaN NaN 27.447 1.093 1890 9 NaN NaN NaN NaN NaN NaN 23.612 -0.944 1890 10 NaN NaN NaN NaN NaN NaN 21.107 -0.281 1890 11 NaN NaN NaN NaN NaN NaN 16.306 -0.447 1890 12 NaN NaN NaN NaN NaN NaN 11.179 -0.818