Stability modifications of the Frøya wind spectrum

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Abstract

A general-stability wind spectrum for the marine boundary layer being an extension of the Frøya wind spectrum (Andersen and Løvseth, 2006) is proposed in order to quantify spectral stability modifications for marine operations and wind turbines.

The analysis of the Frøya data was based on results from the literature: Stability modifications are given by the ratio of a geometrical length scale ZSC increasing linearly with height to a crude representation of the Monin–Obukhov length L. It was a problem that the Frøya data were not available in digital form.

Based on a slightly conservative approach restricted to periods below 6 min, the major spectral stability modification was found to be a linear scaling, whereas frequency shifting was less evident. A smooth representation of the linear scaling factor versus the above ratio was found correspond to monotonic decrease for stable conditions and unlimited monotonic increase for unstable conditions. The modification vanishes as the wind speed increases.

In view of the large scatter in the results for near-neutral stability and the need for better resolution for wind speed and static stability, it is necessary to re-analyse the Frøya database (in digital form) or to analyse some other relevant data set.

Introduction

A wind spectrum for the maritime boundary layer (MBL) during severe weather conditions with relevance for floating marine structures was the most important result from the Frøya project (Andersen and Løvseth, 2006). The Frøya spectrum is mainly a description of the fluctuations of the horizontal wind speed during neutral conditions and in the height range 10–100 m above sea level and has been incorporated in the guidelines NORSOK (1999), API RP2A, and ISO/DIS 19901. For wind speed (10 m, 1 h) stronger than gale (15 m/s), the MBL becomes gradually better mixed and therefore neutrally stratified. The main focus when establishing this description was low frequency wind fluctuations (periods around 20 s–5 min) during near-neutral conditions for measured reference wind speed in the range 10–26 m/s. This reflects the need to obtain a spectral description for floating structures with natural periods in the range around 0.5–2 min during severe weather 35–40 m/s.

The low frequency range is generally associated with significant uncertainty. This is so both because most investigations (Andersen, 1991) have focused on higher frequencies reflecting the needs for most land based structures, but also because very few studies have been made over the ocean (Wills et al., 1986; Shiotani, 1975; Ochi and Shin, 1988). Also, the low frequency range is known to be very sensitive to the effects of MBL stability (Plate, 1982). Thus, very accurate temperature profile measurements are required to ensure that near-neutral data only are included in the analysis and that the spectrum can adequately be extrapolated to severe conditions. Insufficient temperature profile data were a severe shortcoming of some earlier studies (Wills et al., 1986; Shiotani, 1975; Ochi and Shin, 1988).

In the present study, the focus is still on the height and frequency ranges indicated above. However, it is now the operational wind speed range (<15–20 m/s) which is emphasized. This range is important for marine operations and wind turbines and is sensitive to stability effects. This means that a generalization of the Frøya wind spectrum quantifying these effects is needed to provide an adequate spectral description in this range. In view of the engineering practice to use wind spectra based on neutral conditions (NORSOK, 1999; API RP2A; and ISO/DIS 19901), the present generalization will provide a measure of the contribution to the uncertainty of such spectra due to stability effects. It is desirable that this generalization is made within findings from the literature, particularly with attention given to deviations from the neutral Frøya spectrum in terms of simple parameterizations.

As for the Frøya wind spectrum, the data used presently are those from the Frøya project. The main reason for this is the excellent quality of this 15 year old data set both with respect to wind speed and stability. Also, the data set had not been fully and consistently analysed with respect to the effects of stability. However, due to numerous computer system revisions over the years the data are no longer easily available on digital form. Thus, for the present study they had to be extracted from a report (Andersen and Løvseth, 1992) where they were available on graphs with insufficient resolution. The quality of the data presently used, the analysis and the results of the present study are likely to suffer from this.

Section snippets

The Frøya spectrum

The Frøya spectrum S(f) for neutral stability conditions is given byS(f)=320·(Ur/10)2·(z/10)0.45·(1+f˜n)-5/3·n,n=0.468f˜=172·(z/10)2/3·(Ur/10)-0.75·fThis description is assumed valid for reference wind speed Ur (10 m, 1 h) in the range 10–40 m/s, for heights z above sea level in the range 10–100 m and frequencies f (Hz) in the range corresponding to periods 1 s–40 min.

The spectral fit was made to the frequency range corresponding to periods 10 min and shorter as spectral estimates associated with the

The Frøya project and stability

In addition to the Frøya spectrum (Eq. (1a), (1b)), an early version of a spectrum for general stability was developed during the Frøya project (Andersen and Løvseth, 1992). This spectrum will not be discussed in any detail here but some features will be mentioned. First, the description is complicated and indicates an unreasonable and not justified behaviour outside the measured range of the stability parameter. The general increase of the spectral density S(f) with decreasing stability

The modified Frøya spectrum

In the literature, modifications due to stability from a basic neutral description are normally made in terms of the ratio between some geometrical length scale ZSC and the Monin–Obukhov length L (Andersen, 1991). The reported geometrical length scale varies from a fixed one to the height coordinate z and compromises between the two. This is presently taken as a framework for the analysis.

The Frøya spectrum like the Kaimal and Harris spectra (Andersen and Løvseth, 2006) exhibits a monotonic

Conclusion

The Frøya spectrum is valid for both moderate and strong wind speed conditions for neutral stability conditions. For moderate wind speeds, non-neutral stability may significantly modify the MBL wind structure and wind spectrum. This is the main subject of this paper.

As for the Frøya wind spectrum, the data used presently are those from the Frøya project. The main reason for this is the excellent quality of this data set both with respect to wind speed and stability. Also, they had not been

References (12)

  • Andersen, O.J., 1991. The maritime turbulent wind field. A literature review,...
  • Andersen, O.J., Løvseth, J., 1992. The maritime turbulent wind field. Measurements and models. Phase 2–Extension...
  • O.J. Andersen et al.

    The Frøya database and maritime boundary layer wind description

    Mar. Struct.

    (2006)
  • API RP2A-WSD: Planning, Designing, and Constructing Fixed Offshore Plattforms—Working Stress...
  • Draft International Standards, ISO/DIS 19901-1. ISO/TC 67/SC7. Petroleum and natural gas industries—Specific...
  • O. Moraes et al.

    The velocity spectra in the stable surface layer

    Boundary-Layer Meteorol.

    (1987)
There are more references available in the full text version of this article.

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