% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 25653 % Primary Name: TANTALUS MAUKA % Record Type: TAVG % Country: United States % State: HI % Latitude: 21.33330 +/- 0.00005 % Longitude: -157.83330 +/- 0.00005 % Elevation (m): 488.00 +/- 0.05 % # of Months: 61 % % IDs: coop - 518736 % ghcnd - USC00518736 % ncdc - 20023534 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % US Cooperative Summary of the Month % Multi-network Metadata System % % Site Hash: 4d9f8ea6c7c7de23a807d67523cd3dd8 % Raw Data Hash: 585b00cfb9595849a7d66b925432ba8c % Adj Data Hash: 68c63ed38164edb69233c30d41122188 % % 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 1956 8 NaN NaN NaN NaN NaN NaN 25.045 -0.385 1956 9 NaN NaN NaN NaN NaN NaN 25.108 -0.336 1956 10 NaN NaN NaN NaN NaN NaN 24.558 -0.173 1956 11 NaN NaN NaN NaN NaN NaN 23.798 0.035 1956 12 NaN NaN NaN NaN NaN NaN 22.384 0.048 1957 1 NaN NaN NaN NaN NaN NaN 21.717 0.106 1957 2 NaN NaN NaN NaN NaN NaN 20.532 -0.950 1957 3 NaN NaN NaN NaN NaN NaN 20.963 -0.899 1957 4 NaN NaN NaN NaN NaN NaN 21.738 -0.640 1957 5 NaN NaN NaN NaN NaN NaN 23.119 -0.388 1957 6 NaN NaN NaN NaN NaN NaN 24.468 -0.013 1957 7 NaN NaN NaN NaN NaN NaN 24.880 -0.138 1957 8 20.494 -1.163 1 0 NaN NaN 25.180 -0.250 1957 9 22.278 0.606 0 0 22.278 0.606 25.334 -0.110 1957 10 22.556 1.597 0 0 22.556 1.597 25.106 0.376 1957 11 21.222 1.231 0 0 21.222 1.231 24.489 0.727 1957 12 19.056 0.492 0 0 19.056 0.492 22.456 0.121 1958 1 19.278 1.438 0 0 19.278 1.438 21.207 -0.404 1958 2 19.778 2.068 0 0 19.778 2.068 21.245 -0.237 1958 3 18.278 0.187 0 0 18.278 0.187 20.721 -1.141 1958 4 18.722 0.117 0 0 18.722 0.117 21.811 -0.566 1958 5 18.833 -0.901 0 0 18.833 -0.901 22.781 -0.726 1958 6 20.333 -0.376 0 0 20.333 -0.376 24.282 -0.199 1958 7 20.500 -0.746 0 0 20.500 -0.746 24.484 -0.535 1958 8 21.611 -0.047 0 0 21.611 -0.047 25.258 -0.172 1958 9 21.667 -0.005 0 0 21.667 -0.005 25.504 0.060 1958 10 21.056 0.097 0 0 21.056 0.097 24.491 -0.240 1958 11 20.611 0.620 0 0 20.611 0.620 23.411 -0.351 1958 12 18.944 0.381 0 0 18.944 0.381 21.677 -0.659 1959 1 19.444 1.605 0 0 19.444 1.605 21.727 0.116 1959 2 17.278 -0.432 0 0 17.278 -0.432 20.979 -0.503 1959 3 18.833 0.743 0 0 18.833 0.743 22.764 0.902 1959 4 18.444 -0.161 0 0 18.444 -0.161 22.150 -0.227 1959 5 19.056 -0.679 0 0 19.056 -0.679 23.345 -0.162 1959 6 20.222 -0.487 0 0 20.222 -0.487 24.786 0.305 1959 7 20.889 -0.357 0 0 20.889 -0.357 25.144 0.125 1959 8 20.833 -0.825 0 0 20.833 -0.825 25.430 0.000 1959 9 21.056 -0.616 0 0 21.056 -0.616 25.741 0.297 1959 10 21.056 0.097 0 0 21.056 0.097 24.977 0.247 1959 11 19.778 -0.213 0 0 19.778 -0.213 23.951 0.189 1959 12 18.056 -0.508 0 0 18.056 -0.508 22.393 0.057 1960 1 18.056 0.216 0 0 18.056 0.216 21.544 -0.067 1960 2 17.722 0.012 0 0 17.722 0.012 21.311 -0.171 1960 3 18.111 0.020 0 0 18.111 0.020 21.606 -0.256 1960 4 18.111 -0.494 0 0 18.111 -0.494 22.217 -0.160 1960 5 19.222 -0.513 0 0 19.222 -0.513 23.795 0.288 1960 6 20.222 -0.487 0 0 20.222 -0.487 24.675 0.195 1960 7 20.389 -0.857 0 0 20.389 -0.857 24.964 -0.054 1960 8 20.556 -1.102 0 0 20.556 -1.102 25.548 0.119 1960 9 20.778 -0.894 0 0 20.778 -0.894 25.394 -0.050 1960 10 21.111 0.153 0 0 21.111 0.153 24.859 0.129 1960 11 19.500 -0.491 0 0 19.500 -0.491 23.798 0.036 1960 12 19.056 0.492 0 0 19.056 0.492 22.269 -0.067 1961 1 18.611 0.772 0 0 18.611 0.772 21.622 0.011 1961 2 18.444 0.734 0 0 18.444 0.734 22.229 0.747 1961 3 19.333 1.243 0 0 19.333 1.243 22.788 0.926 1961 4 19.111 0.506 0 0 19.111 0.506 22.784 0.406 1961 5 19.611 -0.124 0 0 19.611 -0.124 24.072 0.566 1961 6 19.889 -0.820 0 0 19.889 -0.820 24.441 -0.040 1961 7 20.167 -1.080 0 0 20.167 -1.080 24.731 -0.287 1961 8 20.500 -1.158 0 0 20.500 -1.158 25.374 -0.056 1961 9 21.000 -0.672 0 0 21.000 -0.672 25.377 -0.067 1961 10 20.667 -0.292 0 0 20.667 -0.292 24.770 0.040 1961 11 19.111 -0.880 0 0 19.111 -0.880 23.498 -0.265 1961 12 18.462 -0.102 1 0 NaN NaN 22.491 0.155 1962 1 18.840 1.001 1 0 NaN NaN 22.265 0.653 1962 2 17.286 -0.424 1 0 NaN NaN 21.056 -0.426 1962 3 17.314 -0.776 1 0 NaN NaN 21.506 -0.357 1962 4 19.117 0.511 1 0 NaN NaN 22.862 0.485 1962 5 19.023 -0.712 1 0 NaN NaN 23.569 0.062 1962 6 19.887 -0.821 1 0 NaN NaN 24.297 -0.184 1962 7 19.307 -1.939 1 0 NaN NaN 24.533 -0.485 1962 8 20.231 -1.427 1 0 NaN NaN 24.988 -0.442 1962 9 NaN NaN NaN NaN NaN NaN 25.050 -0.394 1962 10 NaN NaN NaN NaN NaN NaN 24.184 -0.546 1962 11 NaN NaN NaN NaN NaN NaN 24.111 0.348 1962 12 NaN NaN NaN NaN NaN NaN 21.956 -0.379 1963 1 NaN NaN NaN NaN NaN NaN 21.642 0.030 1963 2 NaN NaN NaN NaN NaN NaN 21.883 0.401 1963 3 NaN NaN NaN NaN NaN NaN 22.304 0.442 1963 4 NaN NaN NaN NaN NaN NaN 22.873 0.496 1963 5 NaN NaN NaN NaN NaN NaN 23.166 -0.341 1963 6 NaN NaN NaN NaN NaN NaN 24.217 -0.263 1963 7 NaN NaN NaN NaN NaN NaN 24.758 -0.260 1963 8 NaN NaN NaN NaN NaN NaN 25.463 0.033