% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 25692 % Primary Name: KIPAPA FIELD HAWAII % Record Type: TAVG % Country: United States % State: HI % Latitude: 21.48300 +/- 0.00050 % Longitude: -158.03300 +/- 0.00050 % Elevation (m): 256.00 +/- 0.05 % # of Months: 40 % % IDs: gsod - 911170-99999 % icao - PHHI % usaf - 911170 % % Sources: Global Summary of the Day % % Site Hash: bc10e036fb7e720b490205e9978db268 % Raw Data Hash: cd44a04a1608d9229088f7ce6e126ca3 % Adj Data Hash: 2122d420fa236d15f345137de6bea7a0 % % 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 1941 6 NaN NaN NaN NaN NaN NaN 24.840 0.359 1941 7 NaN NaN NaN NaN NaN NaN 25.221 0.203 1941 8 NaN NaN NaN NaN NaN NaN 25.942 0.512 1941 9 NaN NaN NaN NaN NaN NaN 26.111 0.667 1941 10 NaN NaN NaN NaN NaN NaN 24.858 0.128 1941 11 NaN NaN NaN NaN NaN NaN 23.928 0.165 1941 12 NaN NaN NaN NaN NaN NaN 22.205 -0.131 1942 1 NaN NaN NaN NaN NaN NaN 21.428 -0.183 1942 2 NaN NaN NaN NaN NaN NaN 21.813 0.330 1942 3 NaN NaN NaN NaN NaN NaN 20.606 -1.256 1942 4 NaN NaN NaN NaN NaN NaN 21.524 -0.853 1942 5 NaN NaN NaN NaN NaN NaN 23.590 0.083 1942 6 24.472 1.403 1 0 NaN NaN 24.462 -0.019 1942 7 24.323 0.716 0 0 24.323 0.716 24.986 -0.032 1942 8 24.539 0.521 0 0 24.539 0.521 25.689 0.259 1942 9 24.057 0.025 0 0 24.057 0.025 25.667 0.223 1942 10 23.376 0.058 0 0 23.376 0.058 25.027 0.297 1942 11 22.731 0.380 0 0 22.731 0.380 24.652 0.889 1942 12 21.606 0.682 0 0 21.606 0.682 23.451 1.116 1943 1 20.434 0.234 0 0 20.434 0.234 22.136 0.525 1943 2 19.883 -0.187 0 0 19.883 -0.187 21.519 0.037 1943 3 20.882 0.431 0 0 20.882 0.431 21.309 -0.553 1943 4 21.580 0.614 0 0 21.580 0.614 22.880 0.502 1943 5 22.478 0.384 0 0 22.478 0.384 23.918 0.411 1943 6 23.676 0.607 0 0 23.676 0.607 24.832 0.351 1943 7 24.305 0.698 0 0 24.305 0.698 25.091 0.073 1943 8 24.194 0.175 0 0 24.194 0.175 25.448 0.019 1943 9 24.102 0.070 0 0 24.102 0.070 25.468 0.024 1943 10 23.851 0.533 0 0 23.851 0.533 25.025 0.295 1943 11 22.035 -0.316 0 0 22.035 -0.316 24.035 0.273 1943 12 21.192 0.268 0 0 21.192 0.268 22.779 0.443 1944 1 20.661 0.462 0 0 20.661 0.462 22.244 0.633 1944 2 20.239 0.168 1 0 NaN NaN 21.470 -0.012 1944 3 20.654 0.203 0 0 20.654 0.203 22.013 0.151 1944 4 21.691 0.725 0 0 21.691 0.725 22.989 0.611 1944 5 22.099 0.004 0 0 22.099 0.004 23.373 -0.133 1944 6 22.765 -0.304 0 0 22.765 -0.304 24.087 -0.393 1944 7 23.686 0.080 0 0 23.686 0.080 24.634 -0.385 1944 8 25.966 1.948 0 0 25.966 1.948 25.019 -0.411 1944 9 23.978 -0.054 0 0 23.978 -0.054 24.917 -0.527 1944 10 22.767 -0.552 0 0 22.767 -0.552 24.215 -0.515 1944 11 21.650 -0.701 0 0 21.650 -0.701 23.754 -0.008 1944 12 19.970 -0.954 0 0 19.970 -0.954 22.082 -0.253 1945 1 19.737 -0.463 0 0 19.737 -0.463 21.772 0.161 1945 2 20.345 0.275 0 0 20.345 0.275 22.437 0.955 1945 3 20.905 0.454 0 0 20.905 0.454 22.724 0.862 1945 4 20.820 -0.145 0 0 20.820 -0.145 22.490 0.113 1945 5 22.470 0.375 0 0 22.470 0.375 24.079 0.572 1945 6 23.554 0.485 0 0 23.554 0.485 25.068 0.587 1945 7 23.651 0.044 0 0 23.651 0.044 25.239 0.221 1945 8 23.654 -0.364 0 0 23.654 -0.364 25.447 0.017 1945 9 23.473 -0.559 1 0 NaN NaN 25.159 -0.285 1945 10 NaN NaN NaN NaN NaN NaN 24.881 0.151 1945 11 NaN NaN NaN NaN NaN NaN 24.261 0.498 1945 12 NaN NaN NaN NaN NaN NaN 22.424 0.089 1946 1 NaN NaN NaN NaN NaN NaN 22.205 0.594 1946 2 NaN NaN NaN NaN NaN NaN 22.209 0.727 1946 3 NaN NaN NaN NaN NaN NaN 22.565 0.703 1946 4 NaN NaN NaN NaN NaN NaN 22.306 -0.071 1946 5 NaN NaN NaN NaN NaN NaN 23.348 -0.159 1946 6 NaN NaN NaN NaN NaN NaN 24.674 0.193 1946 7 NaN NaN NaN NaN NaN NaN 24.853 -0.165 1946 8 NaN NaN NaN NaN NaN NaN 25.671 0.242 1946 9 NaN NaN NaN NaN NaN NaN 25.599 0.156