% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 3936 % Primary Name: ALBANYTOWN % Record Type: TAVG % Country: Australia % Latitude: -35.02000 +/- 0.00500 % Longitude: 117.88000 +/- 0.00500 % Elevation (m): 13.00 +/- 0.05 % # of Months: 62 % % IDs: gsod - 949999-00039 % wban - 39 % % Sources: Global Summary of the Day % % Site Hash: e67d4c74f309196cc1d3e17228f2d8c8 % Raw Data Hash: 99f3cb7b091439d859f87f4a7ef7d659 % Adj Data Hash: 95fbfea4a5bebe17cd2594d0f515197b % % 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 1959 1 NaN NaN NaN NaN NaN NaN 19.279 0.361 1959 2 NaN NaN NaN NaN NaN NaN 18.638 -0.253 1959 3 NaN NaN NaN NaN NaN NaN 19.422 1.284 1959 4 NaN NaN NaN NaN NaN NaN 16.117 0.461 1959 5 NaN NaN NaN NaN NaN NaN 14.520 0.837 1959 6 NaN NaN NaN NaN NaN NaN 13.144 1.113 1959 7 NaN NaN NaN NaN NaN NaN 11.997 0.880 1959 8 NaN NaN NaN NaN NaN NaN 12.350 1.186 1959 9 NaN NaN NaN NaN NaN NaN 11.788 -0.233 1959 10 NaN NaN NaN NaN NaN NaN 13.791 0.509 1959 11 NaN NaN NaN NaN NaN NaN 15.041 -0.445 1959 12 NaN NaN NaN NaN NaN NaN 15.310 -2.051 1960 1 18.081 -1.956 0 0 18.081 -1.956 17.297 -1.621 1960 2 18.887 -1.122 0 0 18.887 -1.122 18.394 -0.497 1960 3 17.190 -2.067 0 0 17.190 -2.067 16.653 -1.485 1960 4 15.285 -1.489 0 0 15.285 -1.489 13.577 -2.078 1960 5 13.846 -0.956 0 0 13.846 -0.956 12.091 -1.592 1960 6 12.407 -0.742 0 0 12.407 -0.742 11.149 -0.882 1960 7 11.081 -1.155 0 0 11.081 -1.155 9.891 -1.226 1960 8 11.833 -0.450 0 0 11.833 -0.450 10.228 -0.937 1960 9 13.569 0.429 0 0 13.569 0.429 11.601 -0.420 1960 10 15.465 1.064 0 0 15.465 1.064 13.857 0.575 1960 11 15.913 -0.692 0 0 15.913 -0.692 14.845 -0.642 1960 12 18.324 -0.155 0 0 18.324 -0.155 17.602 0.241 1961 1 20.547 0.510 0 0 20.547 0.510 20.513 1.595 1961 2 21.494 1.485 0 0 21.494 1.485 20.390 1.499 1961 3 20.240 0.983 0 0 20.240 0.983 19.766 1.628 1961 4 16.181 -0.593 0 0 16.181 -0.593 14.544 -1.112 1961 5 15.923 1.121 0 0 15.923 1.121 14.531 0.847 1961 6 13.361 0.211 0 0 13.361 0.211 12.282 0.251 1961 7 12.466 0.230 0 0 12.466 0.230 10.834 -0.283 1961 8 12.392 0.109 0 0 12.392 0.109 11.158 -0.006 1961 9 14.459 1.320 0 0 14.459 1.320 13.384 1.363 1961 10 14.927 0.526 0 0 14.927 0.526 13.886 0.604 1961 11 16.991 0.386 0 0 16.991 0.386 16.003 0.516 1961 12 18.140 -0.340 0 0 18.140 -0.340 17.602 0.241 1962 1 20.045 0.008 0 0 20.045 0.008 19.930 1.012 1962 2 19.649 -0.360 0 0 19.649 -0.360 19.070 0.180 1962 3 18.590 -0.667 0 0 18.590 -0.667 17.757 -0.380 1962 4 17.974 1.199 0 0 17.974 1.199 16.802 1.146 1962 5 15.430 0.628 0 0 15.430 0.628 14.602 0.918 1962 6 14.043 0.893 0 0 14.043 0.893 13.276 1.245 1962 7 12.423 0.187 0 0 12.423 0.187 11.007 -0.110 1962 8 13.289 1.005 0 0 13.289 1.005 12.047 0.883 1962 9 13.154 0.014 0 0 13.154 0.014 11.969 -0.052 1962 10 13.765 -0.635 0 0 13.765 -0.635 12.281 -1.001 1962 11 16.849 0.244 0 0 16.849 0.244 16.229 0.743 1962 12 18.686 0.207 0 0 18.686 0.207 18.229 0.868 1963 1 19.401 -0.635 0 0 19.401 -0.635 19.004 0.087 1963 2 19.671 -0.339 0 0 19.671 -0.339 18.691 -0.199 1963 3 19.785 0.528 0 0 19.785 0.528 19.007 0.869 1963 4 17.404 0.629 0 0 17.404 0.629 15.700 0.044 1963 5 15.457 0.655 0 0 15.457 0.655 14.145 0.461 1963 6 12.496 -0.653 0 0 12.496 -0.653 11.947 -0.084 1963 7 11.828 -0.408 0 0 11.828 -0.408 10.779 -0.338 1963 8 12.677 0.394 0 0 12.677 0.394 11.238 0.074 1963 9 14.043 0.903 0 0 14.043 0.903 12.646 0.626 1963 10 16.541 2.141 0 0 16.541 2.141 14.968 1.686 1963 11 17.352 0.747 0 0 17.352 0.747 16.223 0.736 1963 12 19.674 1.194 0 0 19.674 1.194 18.583 1.222 1964 1 19.627 -0.409 0 0 19.627 -0.409 18.974 0.056 1964 2 19.366 -0.643 0 0 19.366 -0.643 18.472 -0.418 1964 3 19.239 -0.018 0 0 19.239 -0.018 18.785 0.647 1964 4 16.443 -0.332 0 0 16.443 -0.332 14.500 -1.155 1964 5 15.288 0.486 0 0 15.288 0.486 13.195 -0.488 1964 6 14.180 1.030 0 0 14.180 1.030 13.236 1.205 1964 7 12.492 0.256 0 0 12.492 0.256 11.281 0.165 1964 8 12.418 0.135 0 0 12.418 0.135 10.832 -0.332 1964 9 12.464 -0.675 0 0 12.464 -0.675 11.180 -0.840 1964 10 13.565 -0.836 0 0 13.565 -0.836 11.242 -2.039 1964 11 16.523 -0.082 0 0 16.523 -0.082 14.915 -0.571 1964 12 17.106 -1.374 1 0 NaN NaN 15.951 -1.410 1965 1 NaN NaN NaN NaN NaN NaN 19.852 0.934 1965 2 NaN NaN NaN NaN NaN NaN 19.180 0.289 1965 3 18.865 -0.391 1 0 NaN NaN 18.415 0.277 1965 4 18.876 2.102 1 0 NaN NaN 16.787 1.131 1965 5 NaN NaN NaN NaN NaN NaN 13.204 -0.480 1965 6 NaN NaN NaN NaN NaN NaN 11.939 -0.092 1965 7 NaN NaN NaN NaN NaN NaN 10.905 -0.212 1965 8 NaN NaN NaN NaN NaN NaN 10.774 -0.390 1965 9 NaN NaN NaN NaN NaN NaN 12.150 0.129 1965 10 NaN NaN NaN NaN NaN NaN 14.475 1.193 1965 11 NaN NaN NaN NaN NaN NaN 14.905 -0.581 1965 12 NaN NaN NaN NaN NaN NaN 18.508 1.147 1966 1 NaN NaN NaN NaN NaN NaN 19.277 0.360 1966 2 NaN NaN NaN NaN NaN NaN 18.495 -0.395 1966 3 NaN NaN NaN NaN NaN NaN 18.808 0.671 1966 4 NaN NaN NaN NaN NaN NaN 15.023 -0.633