% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 3425 % Primary Name: LIAPOOTAH POWER STATION % Record Type: TAVG % Country: Australia % Latitude: -42.38080 +/- 0.00005 % Longitude: 146.50830 +/- 0.00005 % Elevation (m): 238.00 +/- 0.50 % # of Months: 46 % % IDs: ghcnd - ASN00095027 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: 1dd65d7feec0a622b9a1b4feadb09241 % Raw Data Hash: c906b38b88e59d5d4e81084fe6d6fd83 % Adj Data Hash: ebb849bbf55a26e487e0550006b221b1 % % 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 1988 7 NaN NaN NaN NaN NaN NaN 6.358 1.561 1988 8 NaN NaN NaN NaN NaN NaN 6.424 0.911 1988 9 NaN NaN NaN NaN NaN NaN 8.825 1.579 1988 10 NaN NaN NaN NaN NaN NaN 8.798 -0.227 1988 11 NaN NaN NaN NaN NaN NaN 11.770 1.001 1988 12 NaN NaN NaN NaN NaN NaN 13.926 1.417 1989 1 NaN NaN NaN NaN NaN NaN 15.333 1.070 1989 2 NaN NaN NaN NaN NaN NaN 15.772 1.467 1989 3 NaN NaN NaN NaN NaN NaN 13.899 1.284 1989 4 NaN NaN NaN NaN NaN NaN 11.580 1.896 1989 5 NaN NaN NaN NaN NaN NaN 7.769 0.497 1989 6 NaN NaN NaN NaN NaN NaN 4.585 -0.885 1989 7 4.707 -0.700 1 0 NaN NaN 4.878 0.082 1989 8 5.911 -0.213 0 0 5.911 -0.213 5.458 -0.055 1989 9 8.880 1.023 0 0 8.880 1.023 8.112 0.866 1989 10 9.965 0.328 0 0 9.965 0.328 9.084 0.058 1989 11 13.922 2.542 1 0 NaN NaN 12.120 1.351 1989 12 14.953 1.833 0 0 14.953 1.833 13.442 0.933 1990 1 15.287 0.413 0 0 15.287 0.413 14.484 0.220 1990 2 NaN NaN NaN NaN NaN NaN 14.712 0.407 1990 3 14.269 1.044 0 0 14.269 1.044 13.782 1.167 1990 4 11.519 1.225 0 0 11.519 1.225 10.950 1.267 1990 5 8.276 0.393 0 0 8.276 0.393 7.863 0.591 1990 6 5.829 -0.252 1 0 NaN NaN 6.197 0.727 1990 7 4.919 -0.488 0 0 4.919 -0.488 5.159 0.363 1990 8 5.037 -1.087 0 0 5.037 -1.087 4.677 -0.837 1990 9 8.212 0.355 0 0 8.212 0.355 7.675 0.429 1990 10 11.005 1.368 0 0 11.005 1.368 9.835 0.810 1990 11 13.083 1.703 0 0 13.083 1.703 11.659 0.890 1990 12 13.897 0.776 0 0 13.897 0.776 12.507 -0.002 1991 1 15.658 0.784 0 0 15.658 0.784 14.745 0.482 1991 2 NaN NaN NaN NaN NaN NaN 12.966 -1.339 1991 3 12.221 -1.004 0 0 12.221 -1.004 11.571 -1.044 1991 4 10.215 -0.079 1 0 NaN NaN 9.296 -0.388 1991 5 7.850 -0.032 0 0 7.850 -0.032 7.651 0.379 1991 6 7.042 0.961 0 0 7.042 0.961 6.996 1.526 1991 7 5.554 0.147 0 0 5.554 0.147 5.503 0.706 1991 8 5.542 -0.582 0 0 5.542 -0.582 5.140 -0.374 1991 9 7.848 -0.008 0 0 7.848 -0.008 7.208 -0.038 1991 10 10.834 1.198 0 0 10.834 1.198 9.659 0.634 1991 11 11.137 -0.243 0 0 11.137 -0.243 10.251 -0.519 1991 12 14.388 1.268 0 0 14.388 1.268 12.738 0.229 1992 1 13.381 -1.494 0 0 13.381 -1.494 12.571 -1.692 1992 2 14.864 -0.052 0 0 14.864 -0.052 13.957 -0.348 1992 3 NaN NaN NaN NaN NaN NaN 13.372 0.757 1992 4 NaN NaN NaN NaN NaN NaN 10.299 0.616 1992 5 7.693 -0.189 0 0 7.693 -0.189 7.713 0.442 1992 6 3.920 -2.161 0 0 3.920 -2.161 4.321 -1.148 1992 7 5.287 -0.120 0 0 5.287 -0.120 5.182 0.386 1992 8 5.553 -0.571 0 0 5.553 -0.571 5.069 -0.445 1992 9 6.583 -1.273 0 0 6.583 -1.273 6.060 -1.186 1992 10 10.824 1.188 0 0 10.824 1.188 9.810 0.785 1992 11 12.112 0.732 0 0 12.112 0.732 10.949 0.180 1992 12 15.123 2.002 0 0 15.123 2.002 13.613 1.103 1993 1 15.289 0.414 0 0 15.289 0.414 15.012 0.748 1993 2 16.297 1.381 1 0 NaN NaN 15.102 0.797 1993 3 13.292 0.066 0 0 13.292 0.066 12.746 0.131 1993 4 11.438 1.144 0 0 11.438 1.144 10.986 1.302 1993 5 8.082 0.200 0 0 8.082 0.200 7.964 0.693 1993 6 5.792 -0.289 0 0 5.792 -0.289 5.504 0.035 1993 7 5.918 0.511 0 0 5.918 0.511 6.163 1.367 1993 8 7.273 1.148 0 0 7.273 1.148 6.900 1.386 1993 9 NaN NaN NaN NaN NaN NaN 7.965 0.719 1993 10 NaN NaN NaN NaN NaN NaN 9.197 0.171 1993 11 NaN NaN NaN NaN NaN NaN 10.308 -0.461 1993 12 NaN NaN NaN NaN NaN NaN 12.411 -0.099 1994 1 NaN NaN NaN NaN NaN NaN 12.964 -1.300 1994 2 NaN NaN NaN NaN NaN NaN 15.041 0.736 1994 3 NaN NaN NaN NaN NaN NaN 12.476 -0.139 1994 4 NaN NaN NaN NaN NaN NaN 10.554 0.871 1994 5 NaN NaN NaN NaN NaN NaN 7.387 0.115 1994 6 NaN NaN NaN NaN NaN NaN 5.382 -0.088 1994 7 NaN NaN NaN NaN NaN NaN 5.657 0.861 1994 8 NaN NaN NaN NaN NaN NaN 5.167 -0.346