% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 5057 % Primary Name: IRON RANGE AUSTRALIA % Record Type: TAVG % Country: Australia % Latitude: -12.70000 +/- 0.05000 % Longitude: 143.30000 +/- 0.05000 % Elevation (m): 18.00 +/- 0.05 % # of Months: 25 % % IDs: gsod - 749438-99999 % usaf - 749438 % % Sources: Global Summary of the Day % % Site Hash: 90f338bc7a9f68b0738157ed89c66f4b % Raw Data Hash: ad0ba958a2fffe9247f5107a7327b43e % Adj Data Hash: 910ead0c6291d748060df65b0603b104 % % 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 1941 9 NaN NaN NaN NaN NaN NaN 24.170 -0.973 1941 10 NaN NaN NaN NaN NaN NaN 24.942 -1.389 1941 11 NaN NaN NaN NaN NaN NaN 27.105 -0.400 1941 12 NaN NaN NaN NaN NaN NaN 27.766 0.070 1942 1 NaN NaN NaN NaN NaN NaN 28.115 0.771 1942 2 NaN NaN NaN NaN NaN NaN 27.621 0.276 1942 3 NaN NaN NaN NaN NaN NaN 28.217 1.064 1942 4 NaN NaN NaN NaN NaN NaN 27.610 1.152 1942 5 NaN NaN NaN NaN NaN NaN 26.561 0.752 1942 6 NaN NaN NaN NaN NaN NaN 25.627 1.087 1942 7 NaN NaN NaN NaN NaN NaN 24.929 0.971 1942 8 NaN NaN NaN NaN NaN NaN 24.946 0.638 1942 9 25.837 1.471 1 0 NaN NaN 25.918 0.775 1942 10 25.656 0.102 0 0 25.656 0.102 26.487 0.157 1942 11 26.846 0.118 0 0 26.846 0.118 27.640 0.136 1942 12 26.611 -0.308 0 0 26.611 -0.308 27.397 -0.298 1943 1 26.600 0.032 0 0 26.600 0.032 27.050 -0.295 1943 2 26.368 -0.200 1 0 NaN NaN 27.115 -0.230 1943 3 25.418 -0.959 0 0 25.418 -0.959 26.365 -0.788 1943 4 25.665 -0.018 0 0 25.665 -0.018 26.312 -0.147 1943 5 24.557 -0.475 0 0 24.557 -0.475 25.488 -0.320 1943 6 22.689 -1.074 0 0 22.689 -1.074 23.583 -0.956 1943 7 23.280 0.098 0 0 23.280 0.098 24.237 0.279 1943 8 23.973 0.441 0 0 23.973 0.441 24.911 0.603 1943 9 24.978 0.611 0 0 24.978 0.611 25.923 0.780 1943 10 26.448 0.894 0 0 26.448 0.894 27.001 0.670 1943 11 27.167 0.438 0 0 27.167 0.438 27.606 0.101 1943 12 26.892 -0.027 0 0 26.892 -0.027 27.785 0.089 1944 1 27.260 0.692 0 0 27.260 0.692 27.649 0.305 1944 2 26.977 0.409 1 0 NaN NaN 27.140 -0.205 1944 3 25.869 -0.507 0 0 25.869 -0.507 26.586 -0.566 1944 4 25.396 -0.286 0 0 25.396 -0.286 25.941 -0.518 1944 5 23.961 -1.071 0 0 23.961 -1.071 25.008 -0.800 1944 6 23.333 -0.429 0 0 23.333 -0.429 24.183 -0.356 1944 7 22.846 -0.335 0 0 22.846 -0.335 23.720 -0.237 1944 8 22.869 -0.663 0 0 22.869 -0.663 23.904 -0.404 1944 9 24.157 -0.209 0 0 24.157 -0.209 24.775 -0.368 1944 10 NaN NaN NaN NaN NaN NaN 25.668 -0.662 1944 11 NaN NaN NaN NaN NaN NaN 27.096 -0.409 1944 12 NaN NaN NaN NaN NaN NaN 27.733 0.038 1945 1 NaN NaN NaN NaN NaN NaN 27.326 -0.018 1945 2 NaN NaN NaN NaN NaN NaN 27.466 0.121 1945 3 NaN NaN NaN NaN NaN NaN 27.037 -0.115 1945 4 NaN NaN NaN NaN NaN NaN 25.906 -0.552 1945 5 NaN NaN NaN NaN NaN NaN 24.711 -1.097 1945 6 NaN NaN NaN NaN NaN NaN 24.117 -0.422 1945 7 NaN NaN NaN NaN NaN NaN 23.501 -0.457 1945 8 NaN NaN NaN NaN NaN NaN 25.033 0.725 1945 9 NaN NaN NaN NaN NaN NaN 25.524 0.381