% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 4509 % Primary Name: TABBIMOBILE STATE FOREST % Record Type: TAVG % Country: Australia % Latitude: -29.20000 +/- 0.00005 % Longitude: 153.26670 +/- 0.00005 % Elevation (m): 18.30 +/- 0.50 % # of Months: 23 % % IDs: ghcnd - ASN00058052 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: 28b7e793273c6257db3e0b92ee61366b % Raw Data Hash: ca06cfea20443177fb5efd4c22b265dd % Adj Data Hash: ad3b4d229dba7ceb4ccfc35aaa94e556 % % 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 1964 1 NaN NaN NaN NaN NaN NaN 23.305 0.451 1964 2 NaN NaN NaN NaN NaN NaN 22.686 -0.342 1964 3 NaN NaN NaN NaN NaN NaN 22.529 0.240 1964 4 NaN NaN NaN NaN NaN NaN 20.193 0.198 1964 5 NaN NaN NaN NaN NaN NaN 16.983 0.048 1964 6 NaN NaN NaN NaN NaN NaN 14.744 -0.216 1964 7 NaN NaN NaN NaN NaN NaN 14.064 0.296 1964 8 NaN NaN NaN NaN NaN NaN 14.493 -0.236 1964 9 NaN NaN NaN NaN NaN NaN 17.246 0.570 1964 10 NaN NaN NaN NaN NaN NaN 17.687 -1.036 1964 11 NaN NaN NaN NaN NaN NaN 20.095 -0.587 1964 12 NaN NaN NaN NaN NaN NaN 21.603 -0.493 1965 1 27.227 0.389 0 0 27.227 0.389 21.962 -0.892 1965 2 27.164 0.152 0 0 27.164 0.152 22.651 -0.377 1965 3 26.810 0.537 1 0 NaN NaN 22.513 0.224 1965 4 24.338 0.359 1 0 NaN NaN 20.187 0.192 1965 5 20.198 -0.720 0 0 20.198 -0.720 16.846 -0.088 1965 6 18.235 -0.710 1 0 NaN NaN 15.239 0.278 1965 7 16.190 -1.562 0 0 16.190 -1.562 13.206 -0.562 1965 8 18.623 -0.091 0 0 18.623 -0.091 15.184 0.455 1965 9 22.380 1.719 1 0 NaN NaN 18.207 1.530 1965 10 24.424 1.717 1 0 NaN NaN 19.585 0.862 1965 11 25.990 1.323 1 0 NaN NaN 20.944 0.262 1965 12 27.308 1.228 0 0 27.308 1.228 22.029 -0.068 1966 1 27.032 0.194 0 0 27.032 0.194 21.925 -0.928 1966 2 28.686 1.674 1 0 NaN NaN 23.566 0.538 1966 3 26.044 -0.229 1 0 NaN NaN 22.121 -0.168 1966 4 24.003 0.024 1 0 NaN NaN 20.553 0.558 1966 5 19.390 -1.529 0 0 19.390 -1.529 16.176 -0.759 1966 6 17.697 -1.248 0 0 17.697 -1.248 14.719 -0.241 1966 7 16.018 -1.734 0 0 16.018 -1.734 13.116 -0.652 1966 8 17.971 -0.742 0 0 17.971 -0.742 14.591 -0.138 1966 9 20.003 -0.658 0 0 20.003 -0.658 16.226 -0.451 1966 10 22.332 -0.375 0 0 22.332 -0.375 17.713 -1.011 1966 11 NaN NaN NaN NaN NaN NaN 20.152 -0.530 1966 12 26.655 0.575 0 0 26.655 0.575 21.686 -0.410 1967 1 NaN NaN NaN NaN NaN NaN 22.420 -0.434 1967 2 NaN NaN NaN NaN NaN NaN 22.685 -0.343 1967 3 NaN NaN NaN NaN NaN NaN 21.006 -1.283 1967 4 NaN NaN NaN NaN NaN NaN 19.691 -0.304 1967 5 NaN NaN NaN NaN NaN NaN 16.794 -0.140 1967 6 NaN NaN NaN NaN NaN NaN 17.441 2.480 1967 7 NaN NaN NaN NaN NaN NaN 13.666 -0.102 1967 8 NaN NaN NaN NaN NaN NaN 13.892 -0.837 1967 9 NaN NaN NaN NaN NaN NaN 16.362 -0.315 1967 10 NaN NaN NaN NaN NaN NaN 19.933 1.209 1967 11 NaN NaN NaN NaN NaN NaN 20.532 -0.150 1967 12 NaN NaN NaN NaN NaN NaN 20.898 -1.198