Fróðskaparrit - 01.01.2007, Qupperneq 132

Fróðskaparrit - 01.01.2007, Qupperneq 132
130 VALIDATION OF THE ECMWF ANALYSIS WAVE DATA FOR THE AREA AROUND THE FAROE ISLANDS Event number Start date End date 1 20/8-2000 20/9-2000 2 15/1-2002 15/2-2002 3 1/6-2002 1/7-2002 4 1/1-2003 1/2-2003 Table 2. Duration of the inspected events The data from WVD-4 are quality checked for all events by the data provider. On top of tliis check, different nianual in- spections of the raw data from the peak of the storms are performed, which resulted in rejection of a few measurements in the January 2003 storm. Data from the other locations are only quality checked by pa- rameter behaviour; that is outliers are re- moved if they are not supported by several measurements etc. The time tags connected to measured wave parameter values have been adjusted so they correspond to real-time, rather than completion times of the measured time se- ries (data-burst) which generate the wave spectra. Wave buoys can only accurately meas- ure waves up to some fixed cut-off fre- quency^. A, and the calculation procedures of the buoys do not add a diagnostic upper frequency tail above fhigh. For this reason integrated wave parameters, especially those based on higher order momentums of the spectrum (e.g. Tm02), are affected by this upper frequency limit of the buoy measuring system. At WVD-4 fhj =0.58 Hz (Heinesen, 2005), at K.7 fhig=0.25 Hz (Peter Fenna at Met Offíce UK, pers. com., 2006) and at the OPW buoys fh h is esti- mated to be in the region of 0.5 Hz (Heine- sen, 2001). In order to compensate for the effect of fh h on the measured wave parameters, the wave parameters from WVD-4 are recal- culated from the measured spectrum padded with an f5 high frequency tail. As the spectra are not available for the OPW buoys or the K7 buoy, it is not possible compensate for the influence of the cut-off frequency on the measured wave parame- ters from these sites. In relation to the wave measurements from K7 it ought to be mentioned that the wave height and wave period (labelled Hm0 and Tm02 here), are in fact calculated di- rectly from the time series as root-mean- square wave height and zero-crossing wave period T_, and not from the measured wave spectra as at the other buoys used here. According to the operator, the differ- ence between using the root-mean-square value instead of the wave spectra to com- pute the wave height has been found to be insignificant (Peter Fenna at Met Offíce UK, pers. com., 2006). The two wave peri- ods Tm02 and T_ should in average be di- rectly comparable as they both correspond to the period of the mean wavelength, or alternatively if the wave field is assumed to be a random Gaussian process, then these two periods have been shown to be equal (Rice, 1944; 1945). Wind measurements are available for comparison from the meteorological sta- tion F8 and the K7 buoy. Numerical inves- tigations of stable circumstances suggest that the measured wind speed at the F8 sta- tion is on average comparable to the off- shore 10-meter wind (Heinesen, 2002). Nevertheless direct comparison of wind-
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