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UNCERTAINTY IN PEAKEDNESS FACTOR ESTIMATION BY JONSWAP SPECTRAL FITTING FROM MEASUREMENTS

机译:测量中的Jonswap Spectral拟合升降因子估计的不确定性

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In offshore engineering, JONSWAP shapes are commonly used to fit wave spectra and characterise the peakedness of the sea state. The latter is defined as γ, the so-called peak enhancement factor, which is as large as the peak is acute, with values generally ranging from ~1 to 7 (1 and 3.3 being usually adopted for fully-developed and average wind seas respectively). The determination of γ values permit to simulate realistic sea conditions later on, in particular for determining extreme loads on floating structures in severe sea states. The consistency of the fitting with respect to the actual sea state is subject to - at least - two key, connected aspects, which are: the frequency resolution (i.e., the spacing between two consecutive spectrum estimates) and the sampling error (i.e., the statistical variability of estimates due to both the finiteness of the wave record and the spectral averaging). Based on realistic sea state spectral simulations, this work addresses the sensitivity of the JONSWAP fitting to these aspects and shows that it systematically results in a bias in the peakedness estimate - the bias being aggravated when the sampling error is large for a given signal length (from 10min to 1h). It is shown, in particular, that the error committed with respect to the true γ value is generally higher than 5% for most types of peaks and may often exceed 30%. The aim of this work is to emphasize this issue for practical offshore and oceanographic applications for it may, in turn, potentially introduce a bias in the dynamic response of floating structures in numerical simulations and tank tests.
机译:在海上工程中,Jonswap形状通常用于装配波谱并表征海水的尖峰。后者被定义为γ,所谓的峰值增强因子,其与峰值一样大,其值通常为〜1至7(1和3.3分别用于完全发达和平均风水) )。 γ值的确定允许在稍后模拟现实海洋条件,特别是确定严重海区浮动结构的极端载荷。对实际海水状态的拟合的一致性是至少 - 两个关键,连接的方面,即:频率分辨率(即,两个连续频谱估计之间的间隔)和采样误差(即,由于波记录的有限度和光谱平均而估计的统计变化。基于现实的海区谱仿真,这项工作解决了Jonswap适合这些方面的灵敏度,并表明它系统地导致峰值估计的偏差 - 当采样误差对于给定信号长度大时加重偏差(从10min到1h)。特别地示出了关于真实γ值的错误通常高于5%,对于大多数类型的峰值,并且通常可能超过30%。这项工作的目的是强调这个问题对于实际的海上和海洋申请,又可能在数值模拟和罐试验中引入浮动结构的动态响应偏差。

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