% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 25628 % Primary Name: LUNALILO HOME 724.2 % Record Type: TAVG % Country: United States % State: HI % Latitude: 21.28330 +/- 0.00005 % Longitude: -157.70000 +/- 0.00005 % Elevation (m): 11.90 +/- 0.05 % # of Months: 66 % % Alternate Names: LUNALILO HOME % % IDs: coop - 515675 % ghcnd - USC00515675 % ncdc - 20023497 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % US Cooperative Summary of the Month % Multi-network Metadata System % % Site Hash: 85675874090fe8819e7938bed9671401 % Raw Data Hash: ef96ccf0ff3681f3773fee9b32f5c2cd % Adj Data Hash: 2d0f136693ed43c970d0e0b57b2c022e % % 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 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 NaN NaN NaN NaN NaN NaN 25.180 -0.250 1957 9 NaN NaN NaN NaN NaN NaN 25.334 -0.110 1957 10 23.667 -2.298 0 0 23.667 -2.298 25.106 0.376 1957 11 25.056 0.058 0 0 25.056 0.058 24.489 0.727 1957 12 23.667 0.096 0 0 23.667 0.096 22.456 0.121 1958 1 22.333 -0.513 0 0 22.333 -0.513 21.207 -0.404 1958 2 22.611 -0.106 0 0 22.611 -0.106 21.245 -0.237 1958 3 21.833 -1.264 0 0 21.833 -1.264 20.721 -1.141 1958 4 23.056 -0.556 0 0 23.056 -0.556 21.811 -0.566 1958 5 24.000 -0.741 0 0 24.000 -0.741 22.781 -0.726 1958 6 25.556 -0.160 0 0 25.556 -0.160 24.282 -0.199 1958 7 26.056 -0.197 0 0 26.056 -0.197 24.484 -0.535 1958 8 26.333 -0.331 0 0 26.333 -0.331 25.258 -0.172 1958 9 26.944 0.266 0 0 26.944 0.266 25.504 0.060 1958 10 26.056 0.090 0 0 26.056 0.090 24.491 -0.240 1958 11 24.278 -0.720 0 0 24.278 -0.720 23.411 -0.351 1958 12 23.111 -0.459 0 0 23.111 -0.459 21.677 -0.659 1959 1 22.667 -0.179 0 0 22.667 -0.179 21.727 0.116 1959 2 22.000 -0.717 0 0 22.000 -0.717 20.979 -0.503 1959 3 23.833 0.736 0 0 23.833 0.736 22.764 0.902 1959 4 23.278 -0.334 0 0 23.278 -0.334 22.150 -0.227 1959 5 24.667 -0.075 0 0 24.667 -0.075 23.345 -0.162 1959 6 26.167 0.451 0 0 26.167 0.451 24.786 0.305 1959 7 26.556 0.303 0 0 26.556 0.303 25.144 0.125 1959 8 26.389 -0.276 0 0 26.389 -0.276 25.430 0.000 1959 9 26.833 0.155 0 0 26.833 0.155 25.741 0.297 1959 10 26.333 0.368 0 0 26.333 0.368 24.977 0.247 1959 11 24.833 -0.164 0 0 24.833 -0.164 23.951 0.189 1959 12 23.500 -0.070 0 0 23.500 -0.070 22.393 0.057 1960 1 22.500 -0.346 0 0 22.500 -0.346 21.544 -0.067 1960 2 22.556 -0.161 0 0 22.556 -0.161 21.311 -0.171 1960 3 22.278 -0.820 0 0 22.278 -0.820 21.606 -0.256 1960 4 23.667 0.055 0 0 23.667 0.055 22.217 -0.160 1960 5 25.111 0.370 0 0 25.111 0.370 23.795 0.288 1960 6 26.000 0.284 0 0 26.000 0.284 24.675 0.195 1960 7 26.667 0.414 0 0 26.667 0.414 24.964 -0.054 1960 8 26.722 0.058 0 0 26.722 0.058 25.548 0.119 1960 9 27.000 0.321 0 0 27.000 0.321 25.394 -0.050 1960 10 26.278 0.313 0 0 26.278 0.313 24.859 0.129 1960 11 25.000 0.002 0 0 25.000 0.002 23.798 0.036 1960 12 23.444 -0.126 0 0 23.444 -0.126 22.269 -0.067 1961 1 22.556 -0.291 0 0 22.556 -0.291 21.622 0.011 1961 2 23.111 0.394 0 0 23.111 0.394 22.229 0.747 1961 3 24.000 0.903 0 0 24.000 0.903 22.788 0.926 1961 4 24.056 0.444 0 0 24.056 0.444 22.784 0.406 1961 5 25.611 0.870 0 0 25.611 0.870 24.072 0.566 1961 6 26.222 0.507 0 0 26.222 0.507 24.441 -0.040 1961 7 26.556 0.303 0 0 26.556 0.303 24.731 -0.287 1961 8 26.944 0.280 0 0 26.944 0.280 25.374 -0.056 1961 9 27.000 0.321 0 0 27.000 0.321 25.377 -0.067 1961 10 26.278 0.313 0 0 26.278 0.313 24.770 0.040 1961 11 24.444 -0.553 0 0 24.444 -0.553 23.498 -0.265 1961 12 23.722 0.152 0 0 23.722 0.152 22.491 0.155 1962 1 23.669 0.823 1 0 NaN NaN 22.265 0.653 1962 2 21.944 -0.772 0 0 21.944 -0.772 21.056 -0.426 1962 3 22.722 -0.375 0 0 22.722 -0.375 21.506 -0.357 1962 4 24.222 0.610 0 0 24.222 0.610 22.862 0.485 1962 5 24.944 0.203 0 0 24.944 0.203 23.569 0.062 1962 6 26.056 0.340 0 0 26.056 0.340 24.297 -0.184 1962 7 26.278 0.025 0 0 26.278 0.025 24.533 -0.485 1962 8 26.278 -0.387 0 0 26.278 -0.387 24.988 -0.442 1962 9 26.778 0.099 0 0 26.778 0.099 25.050 -0.394 1962 10 25.778 -0.187 0 0 25.778 -0.187 24.184 -0.546 1962 11 25.833 0.836 0 0 25.833 0.836 24.111 0.348 1962 12 22.908 -0.662 0 0 22.908 -0.662 21.956 -0.379 1963 1 22.389 -0.457 0 0 22.389 -0.457 21.642 0.030 1963 2 22.833 0.116 0 0 22.833 0.116 21.883 0.401 1963 3 NaN NaN NaN NaN NaN NaN 22.304 0.442 1963 4 24.944 1.332 0 0 24.944 1.332 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 1963 9 NaN NaN NaN NaN NaN NaN 25.577 0.133 1963 10 NaN NaN NaN NaN NaN NaN 25.066 0.335 1963 11 NaN NaN NaN NaN NaN NaN 24.270 0.508 1963 12 NaN NaN NaN NaN NaN NaN 22.703 0.368 1964 1 NaN NaN NaN NaN NaN NaN 22.682 1.071 1964 2 NaN NaN NaN NaN NaN NaN 22.101 0.619 1964 3 NaN NaN NaN NaN NaN NaN 22.191 0.328 1964 4 NaN NaN NaN NaN NaN NaN 22.553 0.176