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UNCERTAINTY IN PEAKEDNESS FACTOR ESTIMATION BY JONSWAP SPECTRAL FITTING FROM MEASUREMENTS

机译:通过Jonswap谱拟合从测量中估计骨粉系数的不确定性

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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 l0min 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形状通常用于拟合波谱并表征海态的峰值。后者定义为γ,即所谓的峰值增强因子,它与峰值的锐度一样大,其值通常在〜1到7之间(对于完全发达和平均的风浪,通常分别采用1和3.3) )。 γ值的确定可以稍后模拟实际的海况,尤其是用于确定严重海况下的浮动结构上的极限载荷。拟合相对于实际海况的一致性至少受两个关键的,相互联系的方面的影响,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,由于波记录的有限性和频谱平均的影响,估算值的统计差异)。基于现实的海况频谱模拟,这项工作解决了JONSWAP拟合在这些方面的敏感性问题,并表明它系统地导致峰值估计中存在偏差-对于给定的信号长度,当采样误差较大时,该偏差会加剧(从10分钟到1小时)。尤其表明,对于大多数类型的峰,相对于真实γ值所犯的误差通常高于5%,并且通常可能超过30%。这项工作的目的是在实际的海上和海洋应用中强调此问题,因为它可能反过来可能在数值模拟和储罐测试中对浮动结构的动力响应产生偏差。

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