% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 4569 % Primary Name: GILRUTH PLAINS % Record Type: TAVG % Country: Australia % Latitude: -28.10000 +/- 0.00005 % Longitude: 145.98330 +/- 0.00005 % Elevation (m): 191.70 +/- 0.50 % # of Months: 48 % % IDs: ghcnd - ASN00044036 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: eb78e023450506e3eed52639e230decf % Raw Data Hash: 442382065af77e48a56fafc93b8ea6c1 % Adj Data Hash: 3223447b0aaab37c48800e04927c4767 % % 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 1962 1 NaN NaN NaN NaN NaN NaN 26.497 -1.984 1962 2 NaN NaN NaN NaN NaN NaN 28.055 0.214 1962 3 NaN NaN NaN NaN NaN NaN 24.297 -1.113 1962 4 NaN NaN NaN NaN NaN NaN 19.787 -1.161 1962 5 NaN NaN NaN NaN NaN NaN 14.107 -1.670 1962 6 NaN NaN NaN NaN NaN NaN 14.258 1.332 1962 7 NaN NaN NaN NaN NaN NaN 13.247 1.402 1962 8 NaN NaN NaN NaN NaN NaN 12.912 -0.812 1962 9 NaN NaN NaN NaN NaN NaN 17.407 -0.162 1962 10 NaN NaN NaN NaN NaN NaN 21.723 -0.014 1962 11 NaN NaN NaN NaN NaN NaN 26.409 1.305 1962 12 NaN NaN NaN NaN NaN NaN 25.833 -1.768 1963 1 26.014 -2.133 0 0 26.014 -2.133 25.602 -2.880 1963 2 28.669 1.164 1 0 NaN NaN 28.188 0.347 1963 3 25.594 0.520 0 0 25.594 0.520 25.899 0.490 1963 4 NaN NaN NaN NaN NaN NaN 20.622 -0.326 1963 5 16.983 1.541 1 0 NaN NaN 16.866 1.088 1963 6 11.875 -0.716 0 0 11.875 -0.716 12.522 -0.404 1963 7 10.434 -1.076 0 0 10.434 -1.076 11.167 -0.678 1963 8 14.111 0.723 1 0 NaN NaN 14.343 0.620 1963 9 17.138 -0.096 0 0 17.138 -0.096 17.454 -0.116 1963 10 21.061 -0.341 0 0 21.061 -0.341 21.282 -0.455 1963 11 24.059 -0.709 0 0 24.059 -0.709 23.925 -1.179 1963 12 28.194 0.928 0 0 28.194 0.928 27.696 0.095 1964 1 28.005 -0.142 0 0 28.005 -0.142 28.307 -0.175 1964 2 26.070 -1.435 1 0 NaN NaN 26.473 -1.367 1964 3 25.892 0.818 0 0 25.892 0.818 26.245 0.835 1964 4 20.850 0.237 0 0 20.850 0.237 21.328 0.380 1964 5 14.908 -0.534 0 0 14.908 -0.534 15.464 -0.313 1964 6 11.821 -0.769 0 0 11.821 -0.769 12.960 0.034 1964 7 12.215 0.705 0 0 12.215 0.705 12.700 0.855 1964 8 12.578 -0.810 0 0 12.578 -0.810 13.224 -0.500 1964 9 19.163 1.929 0 0 19.163 1.929 19.006 1.436 1964 10 19.372 -2.030 0 0 19.372 -2.030 19.545 -2.192 1964 11 23.852 -0.917 0 0 23.852 -0.917 24.016 -1.088 1964 12 26.186 -1.079 0 0 26.186 -1.079 26.302 -1.298 1965 1 29.023 0.877 0 0 29.023 0.877 28.580 0.098 1965 2 NaN NaN NaN NaN NaN NaN 29.355 1.515 1965 3 25.548 0.474 0 0 25.548 0.474 26.116 0.706 1965 4 19.520 -1.093 0 0 19.520 -1.093 20.513 -0.436 1965 5 15.446 0.004 0 0 15.446 0.004 16.116 0.339 1965 6 12.630 0.039 0 0 12.630 0.039 13.350 0.424 1965 7 9.573 -1.937 0 0 9.573 -1.937 10.635 -1.210 1965 8 14.206 0.817 0 0 14.206 0.817 14.767 1.044 1965 9 20.175 2.941 0 0 20.175 2.941 20.433 2.864 1965 10 23.339 1.937 0 0 23.339 1.937 23.654 1.917 1965 11 26.030 1.261 0 0 26.030 1.261 26.057 0.953 1965 12 27.952 0.686 0 0 27.952 0.686 27.814 0.214 1966 1 27.636 -0.511 0 0 27.636 -0.511 27.633 -0.849 1966 2 27.593 0.088 0 0 27.593 0.088 27.880 0.040 1966 3 25.324 0.250 0 0 25.324 0.250 25.586 0.176 1966 4 21.646 1.034 0 0 21.646 1.034 22.090 1.142 1966 5 13.765 -1.677 0 0 13.765 -1.677 14.374 -1.404 1966 6 12.331 -0.260 0 0 12.331 -0.260 13.325 0.399 1966 7 10.116 -1.393 0 0 10.116 -1.393 11.016 -0.829 1966 8 NaN NaN NaN NaN NaN NaN 13.227 -0.497 1966 9 16.650 -0.584 0 0 16.650 -0.584 17.009 -0.560 1966 10 NaN NaN NaN NaN NaN NaN 20.660 -1.077 1966 11 24.408 -0.360 0 0 24.408 -0.360 24.508 -0.596 1966 12 27.581 0.316 1 0 NaN NaN 27.315 -0.285 1967 1 30.807 2.661 0 0 30.807 2.661 30.186 1.704 1967 2 29.712 2.207 1 0 NaN NaN 29.365 1.525 1967 3 23.318 -1.756 0 0 23.318 -1.756 23.715 -1.694 1967 4 21.073 0.460 1 0 NaN NaN 21.559 0.611 1967 5 NaN NaN NaN NaN NaN NaN 16.275 0.498 1967 6 NaN NaN NaN NaN NaN NaN 14.854 1.928 1967 7 NaN NaN NaN NaN NaN NaN 11.324 -0.521 1967 8 NaN NaN NaN NaN NaN NaN 12.604 -1.120 1967 9 NaN NaN NaN NaN NaN NaN 17.124 -0.445 1967 10 NaN NaN NaN NaN NaN NaN 24.538 2.801 1967 11 NaN NaN NaN NaN NaN NaN 25.644 0.540 1967 12 NaN NaN NaN NaN NaN NaN 26.252 -1.349 1968 1 NaN NaN NaN NaN NaN NaN 28.218 -0.264 1968 2 NaN NaN NaN NaN NaN NaN 28.422 0.581 1968 3 NaN NaN NaN NaN NaN NaN 26.827 1.417 1968 4 NaN NaN NaN NaN NaN NaN 23.256 2.308