#### [TOC]Chapters:[1][2][3] [4][5] [6][7] [8][9] [10][11] [12][13] [14][15] [Appdx A][Appdx B] [Appdx C]

## Chapter 3

DEFINITION OF QUANTITIES EVALUATED BY WAMIT

Cartesian coordinates are used to define the body geometry, forces, and other hydrodynamic quantities evaluated by WAMIT. These are output in nondimensional forms, in terms of the appropriate combinations of the water density ρ, the acceleration of gravity g, the incident-wave amplitude A, frequency ω, and the length scale L defined by the input parameter ULEN in the GDF file. The notation and definitions of physical quantities here correspond with those in Reference [3], except that in the latter reference the y axis is vertical.

The body geometry, motions and forces are defined in relation to the body coordinates (x,y,z), which can be different for each body if multiple bodies are analyzed. The z-axis must be vertical, and positive upwards. If planes of symmetry are defined for the body, the origin must be on these planes of symmetry. The global coordinates (X,Y,Z) are defined with Z = 0 in the plane of the undisturbed free surface, and the Z-axis positive upwards. The body coordinates for each body are related to the global coordinates by the array XBODY defined in Section 4.2.

The incident-wave system is defined relative to the global coordinate system, and the phases of the exciting forces, motions, pressure and fluid velocity are defined relative to the incident-wave elevation at X = Y = 0. These outputs are defined in the general form

| (3.1) |

where W = |U + iV | is the modulus and δ is the phase. With reference to equations (15.2) and (15.4), the incident-wave elevation at X = Y = 0 is equal to

| (3.2) |

If δ > 0 the output leads the phase of the incident wave, and if δ < 0 the output lags the incident wave.

For field data (pressure, velocity, and free-surface elevation) and mean drift forces the definitions given below in Sections 3.5-3.8 apply to the complete solution for the combined radiation and diffraction problems. The components of the field data can be evaluated separately for either the radiation or diffraction problems using the configuration parameters INUMOPT5 and INUMOPT6, as explained in Sections 4.7 and 5.2.

For the sake of simplicity, the definitions which follow in this Section assume that the origin of the body coordinate system is located on the free surface. Special definitions apply to some quantities if vertical walls are defined, as explained in Section 12.4.

### 3.1 HYDROSTATIC DATA

All hydrostatic data can be expressed in the form of surface integrals over the mean body wetted
surface S_{b}, by virtue of Gauss’ divergence theorem.

Volume:

All three forms of the volume are evaluated in WAMIT, as independent checks of the panel
coordinates, and printed in the summary header of the output file where they are denoted by
(VOLX, VOLY, VOLZ) respectively. The median volume of the three volumes is used for the
internal computations. If it is less than 10^{-30}, a warning is displayed and the coordinates of the
center of buoyancy are set equal to zero. For bottom-mounted structures, where panels are not
defined on the bottom, VOLZ differs from the correct submerged volume by the product of the
bottom area and depth.

Coordinates of center of buoyancy:

Matrix of hydrostatic and gravitational restoring coefficients:

C(3, 3) = ρg ∫
∫
_{Sb}n_{3}dS | (3, 3) = C(3, 3)∕ρgL^{2} |

C(3, 4) = ρg ∫
∫
_{Sb}yn_{3}dS | (3, 4) = C(3, 4)∕ρgL^{3} |

C(3, 5) = -ρg ∫
∫
_{Sb}xn_{3}dS | (3, 5) = C(3, 5)∕ρgL^{3} |

C(4, 4) = ρg ∫
∫
_{Sb}y^{2}n_{
3}dS + ρg∀z_{b} - mgz_{g} | (4, 4) = C(4, 4)∕ρgL^{4} |

C(4, 5) = -ρg ∫
∫
_{Sb}xyn_{3}dS | (4, 5) = C(4, 5)∕ρgL^{4} |

C(4, 6) = -ρg∀x_{b} + mgx_{g} | (4, 6) = C(4, 6)∕ρgL^{4} |

C(5, 5) = ρg ∫
∫
_{Sb}x^{2}n_{
3}dS + ρg∀z_{b} - mgz_{g} | (5, 5) = C(5, 5)∕ρgL^{4} |

C(5, 6) = -ρg∀y_{b} + mgy_{g} | (5, 6) = C(5, 6)∕ρgL^{4} |

where C(i,j) = C(j,i) for all i,j, except for C(4, 6) and C(5, 6). For all other values of the indices i,j, C(i,j) = 0. In particular, C(6, 4) = C(6, 5) = 0.

In C(4,4), C(4,6), C(5,5) and C(5,6), m denotes the body mass. When Alternative form 1 is used for the FRC file (Section 4.3) the body mass is computed from the relation m = ρ∀. When Alternative form 2 is used for the FRC file (Section 4.4) the body mass is defined by EXMASS(3,3).

### 3.2 ADDED-MASS AND DAMPING COEFFICIENTS

Here

### 3.3 EXCITING FORCES

a) Exciting forces from the Haskind relations

b) Exciting forces from direct integration of hydrodynamic pressure

where m = 2 for i = 1, 2, 3 and m = 3 for i = 4, 5, 6.

The separate Froude-Krylov and scattering components of the exciting forces can be
evaluated, using the options IOPTN(2)=2 and IOPTN(3)=2 as described in Section 4.3. The
Froude-Krylov component is defined as the contribution from the incident-wave potential φ_{0} and
the scattering component is the remainder. Using the Haskind relations, these two components
correspond respectively to the contributions from the first and second terms in parenthesis in the
equation above. Using direct integration they correspond to the components of the total
diffraction potential φ_{D} in equation 15.8.

### 3.4 BODY MOTIONS IN WAVES

Two alternative procedures are followed to evaluate the body motions in waves, corresponding respectively to the Alternative 1 (Section 4.3) and Alternative 2 (Section 4.4) FRC control files.

In Alternative 1, which is restricted to a body in free stable flotation without external constraints, the following relations hold

where m is the body mass and (x_{g},y_{g},z_{g}) are the coordinates of the center of gravity.

The inertia matrix is defined as follows.

| (3.3) |

WAMIT equates the body mass to the mass of the displaced water in free flotation. The
moments of inertia I_{ij} are defined in terms of the corresponding radii of gyration r_{ij}, defined by
the relation

The array XPRDCT(I,J) input to WAMIT contains the radii of gyration input with the same units of length as the length scale ULEN defined in the panel data file.

In the Alternative 2 format of the FRC file the matrices M_{ij} + M_{ij}^{E}, B_{
ij}^{E} and C_{
ij}^{E} are input
by the user to include the possibility of external force/moment constraints acting on the
body.

The complex amplitudes of the body’s motions ξ_{j} are obtained from the solution of the 6×6
linear system, obtained by applying Newton’s law

where the matrices M_{ij}^{E}, B_{
ij}^{E} and C_{
ij}^{E} are included only in the Alternative 2 case. Note that in
the Alternative 2 case the user must specify the body inertia matrix M_{ij} and include it in the
total inertia matrix M_{ij} + M_{ij}^{E} specified in the FRC file.

The non-dimensional definitions of the body motions are

where n = 0 for i = 1, 2, 3 and n = 1 for i = 4, 5, 6. The rotational motions (ξ_{4},ξ_{5},ξ_{6}) are
measured in radians.

### 3.5 HYDRODYNAMIC PRESSURE

The complex unsteady hydrodynamic pressure on the body boundary or in the fluid domain is related to the velocity potential by the linearized Bernoulli equation

The total velocity potential is defined by

where the radiation and diffraction velocity potentials are defined in Section 15.1. The nondimensional velocity potential and hydrodynamic pressure are defined as follows:

where K = ω^{2}∕g and

with n = 0 for j = 1, 2, 3 and n = 1 for j = 4, 5, 6.

The body pressure can be evaluated separately for the diffraction or radiation problems by assigning the configuration parameters INUMOPT5=1 and/or INUMOPT6=1, as explained in Section 4.7. When the radiation components are output separately, the nondimensional pressure due to jth mode is defined by

Special definitions are required in the limits of zero and infinite wave periods, as explained in Section 3.9.

### 3.6 FREE-SURFACE ELEVATION

The free surface elevation is obtained from the dynamic free-surface condition

and in nondimensional form

where is defined as in Section 3.5. (The nondimensional hydrodynamic pressure and wave elevation are equal to the nondimensional velocity potential at the respective positions.)

These parameters can be evaluated separately for the diffraction or radiation problems by assigning the configuration parameter INUMOPT6=1, as explained in Section 4.7. When the radiation components are output separately, the nondimensional free-surface elevation due to jth mode is defined by

The evaluation of the pressure or free-surface elevation requires special caution close to the body surface. Within a distance on the order of the dimensions of the adjacent panel(s), field-point quantities cannot be computed reliably. More specific limits can be ascertained by performing a sequence of computations and studying the continuity of the result. Approaching the body along a line normal to the centroid of a panel will minimize this problem. See Reference [12] regarding the computation of run-up at the intersection of the body and free surface. The parameter TOLFPTWL can be used to check for field points on the free surface which are close to, or inside, body waterlines (see Section 4.3).

### 3.7 VELOCITY VECTOR ON THE BODY AND IN THE FLUID DOMAIN

The nondimensional velocities evaluated by WAMIT are defined in vector form by

where

These parameters can be evaluated separately for the diffraction or radiation problems by assigning the configuration parameters INUMOPT5=1 and/or INUMOPT6=1, as explained in Section 4.7.

The evaluation of the velocity requires special caution close to the body surface, in the same manner as the pressure and free-surface elevation.

When the radiation components are output separately, the nondimensional velocity due to jth mode is defined by

_{j}∇φ

_{j}is the dimensional fluid velocity, and v

_{j}= iωξ

_{j}denotes the velocity of the body for j = 1, 2, 3 and the angular velocity for j = 4, 5, 6. n = 0 for j = 1, 2, 3 and n = 1 for j = 4, 5, 6.

Special definitions are required in the limits of zero and infinite wave periods, as explained in Section 3.9.

### 3.8 MEAN DRIFT FORCE AND MOMENT

The definition of the nondimensional mean drift force and moment in unidirectional waves is

where k = 1 for the forces (i = 1, 2, 3), and k = 2 for the moments (i = 4, 5, 6).

For bi-directional waves of the same period, with complex amplitudes (A_{1}, A_{2}) and
corresponding angles of incidence (β_{1}, β_{2}), the nondimensional outputs _{i}(β_{1},β_{2}) are the
coefficients such that the total dimensional mean drift force or moment exerted on the body is
given by the equation

_{i}

^{*}(β

_{ 2},β

_{1}) =

_{i}(β

_{1},β

_{2}), where the asterisk (*) denotes the complex conjugate.

In Option 7 the drift force and moment are evaluated based on the momentum flux across a control surface as described in Chapter 11, using equations (15.57-60).

In Option 8, the evaluation of the horizontal drift force and vertical moment is based on the
momentum conservation principle in its general form (see References [4] and [26]), without the
assumption of energy conservation. This permits the analysis of cases where the body motions
are affected by non-conservative effects, such as external damping. The azimuthal integration
required to evaluate the momentum flux is performed by an adaptive quadrature formula.
The integration is performed iteratively, with convergence specified by the criterion of
absolute or relative errors in each drift force less than TOL=10^{-4}. The maximum
number of iterations is controlled by the parameter MAXMIT. A warning message
is displayed in the event that this convergence criterion is not satisfied. See Section
5.8 for further information regarding the interpretation and control of this warning
message.

Often the warning message is issued because the length scale parameter ULEN is much
smaller than the relevant length scale of the body. Since the drift force increases in proportion to
length, and the moment in proportion to (length)^{2}, relatively small differences between large
values may not be significant. In this case the warning message can be avoided by increasing
ULEN to a value more representative of the length.

This force or moment can be either converged for most practical purposes or too small to be important in practice. It is recommended to check the practical importance of this quantity. Further check on the convergence of the result can be made by increasing MAXMIT gradually. Since the computational time increases exponentially, it is not recommended to use significantly large MAXMIT than the default value.

In Option 9, the evaluation of the drift force and moment is based on integration of the pressure over the body surface, using the relations in [10] and [17], as summarized in Section 15.7.

In Options 7 and 9, the mean drift force and moment evaluated from pressure integration and from momentum flux on a control surface are defined with respect to the body coordinate system. Conversely, the mean drift force and moment evaluated from momentum conservation in Option 8 are defined with respect to the global coordinate system.

### 3.9 ZERO AND INFINITE WAVE PERIODS

It is possible to evaluate the added mass (Option 1), and also the pressure and fluid velocity (Options 5 and 6) in the limiting cases of zero and infinite period (or equivalently, infinite and zero frequency), by inputting PER=0.0 and PER<0.0 in the POT file (see Section 4.2). This extension is particularly important in the context of evaluating the corresponding time-domain impulse response functions, as explained in Chapter 13.

The definition of the added-mass coefficients is the same as shown in Section 3.2. All other force coefficients are zero in these limits, with the exception of the heave exciting force and horizontal exciting moments, which tend to nonzero hydrostatic limits at zero frequency.

Special definitions are applied to the radiation pressure and velocity in the case of zero
frequency (infinite wave period), which is identified in the output files by a negative value of the
parameter PER, and also in the case of infinite frequency (zero wave period), which is identified
by PER=0. In general, for nonzero finite values of the frequency, the nondimensional outputs for
the radiation pressure and velocity are as defined in Sections 3.5 and 3.7. Thus the output
pressure for each radiation mode is KL_{j} and the output velocity for each mode is KL_{j}.
However for the two limiting cases, where KL = 0 or KL = ∞, the factor KL is
omitted from the outputs for Options 5 and 6. The following table summarizes these
definitions:

frequency | period | pressure | velocity | |

PER<0 | ω = 0 | ∞ | _{j} | _{j} |

0 <PER< ∞ | 0 < ω < ∞ | (2π∕ω) | KL_{j} | KL_{j} |

PER=0 | ω = ∞ | 0 | _{
j} | _{j} |