3. Radiation and Diffraction Flashcards

1
Q

Rayleigh distribution is considered a good approximation for the probability density function of the maxima of the wave elevation if

A

If a gaussian distribution is a good approximation for the instantaneous wave elevation and the wave-spectrum is narrow banded

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2
Q

The probability associated with a certain sea condition is given by

A

It’s occurrence divided by the sum of all possible occurrences

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3
Q

Short-crested waves mean

A

The wave spectrum varies with the direction theta

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4
Q

Linear hydrodynamic loads are split into

A

Diffraction and radiation

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5
Q

Contributions to the diffraction problem

A

Excitation loads

  • Froude-Kriloff loads
  • Diffraction loads
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6
Q

Froude-Kriloff principle

A

The flow penetrates the body with a normal velocity like the body was not there. This causes hydrodynamic loads on the body called FK loads

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7
Q

Diffraction loads principle

A

To recover the body impermeability, the body presence causes a flow (and so waves)

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8
Q

The wave excitation loads are obtained by

A

Integrating the incident wave dynamic pressure and the diffraction dynamic pressure along the mean wetted hull surface

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9
Q

Radiation problem HP

A

The body is forced to oscillate in its six degrees of freedom

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10
Q

(Radiation) hydrodynamic loads identifies as

A

Added mass
Damping
Restoring terms

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11
Q

Added mass is in phase with ____

Damping is in phase with ____

A

Acceleration

Velocity

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12
Q

The vertical FK force component is given by

A

The incident wave vertical acceleration at the geometrical center of the 2D body multiplied by the mass of water displaced by the body

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13
Q

Strip theory for radiation problem

A

Justified for zero speed when the frequencies correspond to a wavelength in the order of the cross-sectional dimension in y,z plane.
—> 3D problems sum of 2D problems

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14
Q

Strip theory for diffraction problem

A

Considers wavelengths large compared to cross section in z,y plane by adding FK forces

—> 3D problem by sum of 2D + FK loads

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15
Q

Does the body move in the diffraction problem

A

The body does not move: incident-waves plus diffraction flow give zero normal velocity at the fixed-body surface

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16
Q

Consequence of long-wave approximation for excitation forces:

A

Waves generated by the wave-body interaction are small —> the damping contribution to the forces are small relative to the terms proportional to the acceleration and can be neglected

17
Q

What happens to B33 when omega goes to infinity or zero

A

It is zero as it is connected with the square power of the amplitude if the radiated waves

18
Q

A33 for a half circle in omega—> infinity

A

Equals the mass of the water displaced by the half circle

19
Q

can Ajj and Bjj be negative?

A

Wave radiation damping Bjj can not be negative.

Added mass Ajj can be negative for certain frequencies and body shapes. E.g., catamaran

20
Q

Added mass and damping coefficients depend on

A

Frequency
Body shape
Forward speed U