Book contents
- Frontmatter
- Contents
- Preface
- List of symbols
- 1 INTRODUCTION
- 2 RESISTANCE AND PROPULSION
- 3 WAVES
- 4 WAVE RESISTANCE AND WASH
- 5 SURFACE EFFECT SHIPS
- 6 HYDROFOIL VESSELS AND FOIL THEORY
- 7 SEMI-DISPLACEMENT VESSELS
- 8 SLAMMING, WHIPPING, AND SPRINGING
- 9 PLANING VESSELS
- 10 MANEUVERING
- APPENDIX: Units of Measurement and Physical Constants
- References
- Index
4 - WAVE RESISTANCE AND WASH
Published online by Cambridge University Press: 15 September 2009
- Frontmatter
- Contents
- Preface
- List of symbols
- 1 INTRODUCTION
- 2 RESISTANCE AND PROPULSION
- 3 WAVES
- 4 WAVE RESISTANCE AND WASH
- 5 SURFACE EFFECT SHIPS
- 6 HYDROFOIL VESSELS AND FOIL THEORY
- 7 SEMI-DISPLACEMENT VESSELS
- 8 SLAMMING, WHIPPING, AND SPRINGING
- 9 PLANING VESSELS
- 10 MANEUVERING
- APPENDIX: Units of Measurement and Physical Constants
- References
- Index
Summary
Introduction
In this chapter, we concentrate on wave resistance and ship-generated waves (wash) of high-speed vessels in calm water conditions. The focus is on semi-displacement vessels and air cushion–supported vehicles. Wave resistance of hydrofoils is discussed in section 6.8.
Wave resistance
Figure 4.1 shows the numerically calculated relative importance of resistance components of a 70 m–long catamaran in deep water. The main particulars are presented in Table 4.1. The ship speed U is 40 knots in calm water. The effect of head sea waves with different significant wave heights H⅓ is also shown. The added resistance due to the incident waves and wind are accounted for by selecting a representative wind velocity and mean wave period for each H⅓. Corresponding data for a 70 m–long surface effect ship (SES) are shown in Figure 4.2, with the main particulars given in Table 4.2. The ship power is kept constant in the calculations, which means increasing speed loss with increasing H⅓. Voluntary speed reduction, for instance, as a result of excessive vertical accelerations, is not accounted for. The speed loss is most pronounced for the SES, as shown in Figure 4.2. The SES speed has dropped from 50 knots in calm water to about 35 knots in H⅓ = 5 m. The speed loss for the catamaran is not shown. However, because viscous frictional resistance is mainly proportional to UH2, the curve for frictional resistance as a function of H⅓ shows that the speed loss is not large.
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- Hydrodynamics of High-Speed Marine Vehicles , pp. 99 - 140Publisher: Cambridge University PressPrint publication year: 2006
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