% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 26122 % Primary Name: KISSIMMEE FLORIDA AAF % Record Type: TAVG % Country: United States % State: FL % Latitude: 28.28300 +/- 0.00050 % Longitude: -81.41600 +/- 0.00050 % Elevation (m): 25.00 +/- 0.05 % # of Months: 18 % % IDs: gsod - 749047-99999 % icao - ISM % usaf - 749047 % % Sources: Global Summary of the Day % % Site Hash: 4ef7b5f07f1764702d1da77f026c0d54 % Raw Data Hash: b0f25cdbedefa58880dbabf91ab17943 % Adj Data Hash: 05bee8c2a1df20f7cc9ed9fb2bf2dfdc % % 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 1943 3 NaN NaN NaN NaN NaN NaN 19.614 0.003 1943 4 NaN NaN NaN NaN NaN NaN 21.457 -0.739 1943 5 NaN NaN NaN NaN NaN NaN 25.532 0.545 1943 6 NaN NaN NaN NaN NaN NaN 27.363 0.421 1943 7 NaN NaN NaN NaN NaN NaN 27.383 -0.448 1943 8 NaN NaN NaN NaN NaN NaN 27.805 -0.095 1943 9 NaN NaN NaN NaN NaN NaN 26.965 -0.091 1943 10 NaN NaN NaN NaN NaN NaN 21.867 -1.834 1943 11 NaN NaN NaN NaN NaN NaN 19.020 -0.870 1943 12 NaN NaN NaN NaN NaN NaN 16.532 -0.157 1944 1 NaN NaN NaN NaN NaN NaN 15.119 -0.859 1944 2 NaN NaN NaN NaN NaN NaN 19.126 2.481 1944 3 20.351 1.680 0 0 20.351 1.680 21.412 1.800 1944 4 22.096 0.841 0 0 22.096 0.841 23.138 0.943 1944 5 23.427 -0.620 0 0 23.427 -0.620 24.332 -0.654 1944 6 26.607 0.606 0 0 26.607 0.606 27.667 0.725 1944 7 26.455 -0.436 0 0 26.455 -0.436 27.392 -0.439 1944 8 26.595 -0.364 0 0 26.595 -0.364 27.634 -0.266 1944 9 26.594 0.478 0 0 26.594 0.478 27.893 0.836 1944 10 21.715 -1.046 0 0 21.715 -1.046 22.633 -1.068 1944 11 17.935 -1.015 0 0 17.935 -1.015 18.879 -1.011 1944 12 13.855 -1.895 0 0 13.855 -1.895 14.965 -1.725 1945 1 14.896 -0.142 0 0 14.896 -0.142 15.766 -0.212 1945 2 18.672 2.967 1 0 NaN NaN 18.365 1.720 1945 3 21.747 3.076 0 0 21.747 3.076 22.384 2.772 1945 4 23.533 2.278 0 0 23.533 2.278 24.321 2.125 1945 5 23.631 -0.416 0 0 23.631 -0.416 24.398 -0.589 1945 6 26.698 0.697 0 0 26.698 0.697 27.360 0.418 1945 7 26.319 -0.572 0 0 26.319 -0.572 27.324 -0.507 1945 8 27.400 0.441 1 0 NaN NaN 27.755 -0.144 1945 9 NaN NaN NaN NaN NaN NaN 27.322 0.265 1945 10 NaN NaN NaN NaN NaN NaN 24.154 0.453 1945 11 NaN NaN NaN NaN NaN NaN 19.173 -0.717 1945 12 NaN NaN NaN NaN NaN NaN 15.770 -0.920 1946 1 NaN NaN NaN NaN NaN NaN 16.979 1.001 1946 2 NaN NaN NaN NaN NaN NaN 17.145 0.500 1946 3 NaN NaN NaN NaN NaN NaN 20.540 0.928 1946 4 NaN NaN NaN NaN NaN NaN 22.600 0.404 1946 5 NaN NaN NaN NaN NaN NaN 25.477 0.490 1946 6 NaN NaN NaN NaN NaN NaN 26.614 -0.328 1946 7 NaN NaN NaN NaN NaN NaN 27.583 -0.248 1946 8 NaN NaN NaN NaN NaN NaN 27.709 -0.191