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Fluid Dynamics and Ship Motion

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Continuum Mechanics using Mathematica®

Abstract

This chapter is a brief introduction to the very difficult problem of ship motion. The difficulties of this problem are due to the many factors determining the behavior of a ship during the navigation: the form of the ship, the sea waves, the wind action, etc. After introducing the roll, pitch, and yaw angles, many fundamental kinematic relations are determined. Then, the dynamical equations are proposed starting from dynamics of rigid bodies. A section is dedicated to the analysis of the forces acting on the ship. Since the nonlinear problem posed by these equations is very difficult to solve, small motions are considered which lead to linear differential equations. All the forces and momenta, describing the actions of weight, buoyant force, the interaction between ship and sea, are taken into account. In order to evaluate all the terms appearing in the motion equations, it is necessary to consider the effects produced by waves propagating on the free surface of the sea. To the analysis of the wave propagation on the free surface are dedicated the last sections of the chapter.

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Notes

  1. 1.

    The reader interested in the topics presented in this chapter may consult specialistic books, for instance [2, 14, 21, 24, 25, 41, 42, 44, 4649, 59, 70, 71].

  2. 2.

    The notations adopted in this chapter are the same used in [55] and [41].

  3. 3.

    It is evident that this hypothesis can be accepted for a big ship since, if the goods are well packed in the hold, any position change of passengers does not modify the mass distribution. This in not true for a small barge in which, any position change of a passenger should modify the mass distribution.

  4. 4.

    All the definitions and notations used in this chapter are the same used in [55], Chapters 12, 15, 16.

  5. 5.

    It is evident that, composing these three rotations, we obtain a Cartesian frame fixed in the body. It is possible to prove that, given any transformation \(G\xi \eta \zeta \rightarrow Gx^{{\prime}}y^{{\prime}}z^{{\prime}}\) by an orthogonal matrix, it is possible to determine \(\varphi\), θ, and ψ.

  6. 6.

    All the results and definitions of rigid body dynamics can be found in [55], Chapter 15.

  7. 7.

    See, for instance [55], Chapter 15.

  8. 8.

    It can be proved that \(\overline{\mathbf{K}}\) does not depend on the choice of the pole.

  9. 9.

    See, [71], pg. 5.

  10. 10.

    It can be proved that this circumstance is verified if the amplitude K 1 in (13.78) is such that K 1λ.

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Romano, A., Marasco, A. (2014). Fluid Dynamics and Ship Motion. In: Continuum Mechanics using Mathematica®. Modeling and Simulation in Science, Engineering and Technology. Birkhäuser, New York, NY. https://doi.org/10.1007/978-1-4939-1604-7_13

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