% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 15244 % Primary Name: MISAMARI INDIA % Record Type: TAVG % Country: India % Latitude: 26.80000 +/- 0.00050 % Longitude: 92.61600 +/- 0.00050 % Elevation (m): 98.00 +/- 0.05 % # of Months: 24 % % IDs: gsod - 749246-99999 % usaf - 749246 % % Sources: Global Summary of the Day % % Site Hash: fd9e5751d6b1994825687f77fdf67066 % Raw Data Hash: 272b5cb5ddc6aecad7743fd199fa6d76 % Adj Data Hash: 76bc4e3335f3bd484fe50be682bcbe6c % % 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 1942 11 NaN NaN NaN NaN NaN NaN 21.016 0.357 1942 12 NaN NaN NaN NaN NaN NaN 16.369 -0.467 1943 1 NaN NaN NaN NaN NaN NaN 16.419 0.736 1943 2 NaN NaN NaN NaN NaN NaN 17.085 -0.946 1943 3 NaN NaN NaN NaN NaN NaN 20.391 -1.099 1943 4 NaN NaN NaN NaN NaN NaN 22.120 -1.573 1943 5 NaN NaN NaN NaN NaN NaN 25.396 -0.087 1943 6 NaN NaN NaN NaN NaN NaN 27.490 0.386 1943 7 NaN NaN NaN NaN NaN NaN 27.881 0.307 1943 8 NaN NaN NaN NaN NaN NaN 27.064 -0.518 1943 9 NaN NaN NaN NaN NaN NaN 27.197 0.139 1943 10 NaN NaN NaN NaN NaN NaN 24.428 -0.178 1943 11 15.587 -5.501 1 0 NaN NaN 21.388 0.729 1943 12 17.518 0.253 0 0 17.518 0.253 17.030 0.194 1944 1 16.181 0.069 0 0 16.181 0.069 15.343 -0.341 1944 2 17.918 -0.543 1 0 NaN NaN 17.202 -0.829 1944 3 22.348 0.429 0 0 22.348 0.429 22.244 0.754 1944 4 23.604 -0.518 0 0 23.604 -0.518 23.130 -0.563 1944 5 25.713 -0.200 0 0 25.713 -0.200 25.294 -0.189 1944 6 27.350 -0.183 0 0 27.350 -0.183 26.996 -0.108 1944 7 28.457 0.454 0 0 28.457 0.454 27.718 0.144 1944 8 28.335 0.324 0 0 28.335 0.324 27.764 0.182 1944 9 26.354 -1.133 0 0 26.354 -1.133 26.287 -0.771 1944 10 24.970 -0.066 0 0 24.970 -0.066 24.842 0.236 1944 11 20.502 -0.586 0 0 20.502 -0.586 20.065 -0.594 1944 12 18.125 0.861 0 0 18.125 0.861 17.476 0.640 1945 1 16.043 -0.069 0 0 16.043 -0.069 15.558 -0.125 1945 2 16.385 -2.075 1 0 NaN NaN 16.309 -1.722 1945 3 22.290 0.371 0 0 22.290 0.371 22.112 0.622 1945 4 25.287 1.165 0 0 25.287 1.165 24.688 0.995 1945 5 25.308 -0.605 0 0 25.308 -0.605 24.780 -0.704 1945 6 27.606 0.072 0 0 27.606 0.072 27.329 0.225 1945 7 28.215 0.212 0 0 28.215 0.212 27.472 -0.102 1945 8 27.599 -0.412 0 0 27.599 -0.412 27.102 -0.480 1945 9 27.380 -0.107 0 0 27.380 -0.107 27.372 0.314 1945 10 26.014 0.978 1 0 NaN NaN 24.074 -0.532 1945 11 NaN NaN NaN NaN NaN NaN 20.351 -0.308 1945 12 NaN NaN NaN NaN NaN NaN 16.297 -0.539 1946 1 NaN NaN NaN NaN NaN NaN 16.429 0.746 1946 2 NaN NaN NaN NaN NaN NaN 19.478 1.447 1946 3 NaN NaN NaN NaN NaN NaN 21.624 0.134 1946 4 NaN NaN NaN NaN NaN NaN 22.994 -0.699 1946 5 NaN NaN NaN NaN NaN NaN 25.427 -0.057 1946 6 NaN NaN NaN NaN NaN NaN 27.149 0.044 1946 7 NaN NaN NaN NaN NaN NaN 27.192 -0.382 1946 8 NaN NaN NaN NaN NaN NaN 28.035 0.453 1946 9 NaN NaN NaN NaN NaN NaN 27.297 0.239 1946 10 NaN NaN NaN NaN NaN NaN 23.977 -0.630