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Practical Ship Hydrodynamics

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10 <strong>Practical</strong> <strong>Ship</strong> <strong>Hydrodynamics</strong><br />

y + dy<br />

u<br />

v + v y dy<br />

v<br />

y<br />

x x + dx<br />

u + u x dx<br />

Figure 1.1 Control volume to derive continuity equation in two dimensions<br />

The continuity equation in three dimensions can be derived correspondingly to:<br />

ux C vy C wz D 0<br />

w is the velocity component in z direction.<br />

The Navier–Stokes equations together with the continuity equation suffice<br />

to describe all real flow physics for ship flows. The Navier–Stokes equations<br />

describe conservation of momentum in the flow:<br />

⊲ut C uux C vuy C wuz⊳ D f1 px C ⊲uxx C uyy C uzz⊳<br />

⊲vt C uvx C vvy C wvz⊳ D f2 py C ⊲vxx C vyy C vzz⊳<br />

⊲wt C uwx C vwy C wwz⊳ D f3 pz C ⊲wxx C wyy C wzz⊳<br />

fi is an acceleration due to a volumetric force, p the pressure, the viscosity<br />

and t the time. Often the volumetric forces are neglected, but gravity can<br />

be included by setting f3 D g ⊲D9.81 m/s 2 ⊳ or the propeller action can<br />

be modelled by a distribution of volumetric forces f1. The l.h.s. of the<br />

Navier–Stokes equations without the time derivative describes convection,<br />

the time derivative describes the rate of change (‘source term’), the last term<br />

on the r.h.s. describes diffusion.<br />

The Navier–Stokes equations in the above form contain on the l.h.s. products<br />

of the velocities and their derivatives. This is a non-conservative formulation<br />

of the Navier–Stokes equations. A conservative formulation contains<br />

unknown functions (here velocities) only as first derivatives. Using the product<br />

rule for differentiation and the continuity equation, the non-conservative formulation<br />

can be transformed into a conservative formulation, e.g. for the first of<br />

the Navier–Stokes equations above:<br />

⊲u 2 ⊳x C ⊲uv⊳y C ⊲uw⊳z D 2uux C uyv C uvy C uzw C uwz<br />

D uux C vuy C wuz C u⊲ux C vy C wz⊳<br />

� �� �<br />

D0<br />

D uux C vuy C wuz<br />

Navier–Stokes equations and the continuity equation form a system of coupled,<br />

non-linear partial differential equations. An analytical solution of this system<br />

is impossible for ship flows. Even if the influence of the free surface (waves)<br />

is neglected, today’s computers are not powerful enough to allow a numerical

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