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Final report for WP4.3: Enhancement of design methods ... - Upwind

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damaging if the frequency <strong>of</strong> the excitation coincides with a natural frequency <strong>of</strong> the structure. In order to<br />

avoid the range <strong>of</strong> conditions at which resonance can occur, it is important to predict the frequencies at<br />

which large amplitudes <strong>of</strong> oscillation may be expected.<br />

Section D.4 addresses the issue <strong>of</strong> vortex induced vibrations, giving a methodology <strong>for</strong> calculating the<br />

critical velocities at which resonances will occur <strong>for</strong> a given structure. However this theory is only valid <strong>for</strong><br />

steady currents and cannot be used <strong>for</strong> waves unless the period is very long, i.e. if the KC number is high.<br />

In the light <strong>of</strong> this it is recommended that this whole section should be revised in any future revisions <strong>of</strong> the<br />

standard.<br />

Annex D: Calculation <strong>of</strong> hydrodynamic loads: Appurtenances<br />

For relatively small appurtenances it is sufficient to account <strong>for</strong> the additional hydrodynamic <strong>for</strong>ces in the<br />

dimensions and/or <strong>for</strong>ce coefficients assumed <strong>for</strong> the modelled elements. Section D.5 describes a method<br />

<strong>for</strong> calculating equivalent hydrodynamic coefficients Cdeq and Cmeq taking into account appurtenances and<br />

marine growth on a monopile support structure. The appurtenances are approximated by vertical circular<br />

cylinders, characterized by an equivalent diameter di. Using this method the equivalent hydrodynamic coefficients<br />

are calculated by:<br />

C<br />

⎪⎧<br />

'<br />

D<br />

= ⎨ C<br />

⎪⎩<br />

D<br />

⎡d<br />

N '<br />

deq ds<br />

φ<br />

and<br />

C<br />

meq<br />

i<br />

( R,<br />

e)<br />

⋅WAFd(<br />

K ) + ∑ ⎢ ⋅Cdsi(<br />

Ri<br />

, e)<br />

⋅WAFdi(<br />

Ki<br />

) ⋅ IFdi<br />

( i , Ki<br />

) ⎥⎬<br />

i=<br />

1 D<br />

⎪⎭<br />

⎢⎣<br />

' 2<br />

⎡ 2<br />

( ) N ⎛ '<br />

D<br />

⎞<br />

( ) ⎢⎜<br />

di<br />

C K , C + ⎟ ⋅ 1+ ( C ( K , C ) −1)<br />

⋅ IF ( φ , K )<br />

⎧<br />

⎪<br />

= ⎨<br />

⎪ D<br />

⎩<br />

2<br />

m<br />

ds<br />

∑<br />

⎢⎜<br />

⎟ i=<br />

1<br />

⎣⎝<br />

D ⎠<br />

( ) ⎥<br />

mi i dsi<br />

mi i i ⎬<br />

⎥⎪⎭<br />

In the above equations IFdi and IFmi are interference factors expressing the variation in hydrodynamic coefficient<br />

<strong>for</strong> the appurtenance due to the presence <strong>of</strong> the monopile. In order to calculate these factors the<br />

<strong>design</strong>er is referred to the reference documents [25] and [26].<br />

An improvement to the method currently stated in the standard has been proposed [27], using Cd and Cm<br />

values from [28] and ignoring the wake amplification factor WAFd. The method <strong>for</strong> calculating IFdi and IFmi<br />

is also expressed in more detail in the proposed method, including separate calculations <strong>for</strong> blocking and<br />

shielding regimes <strong>for</strong> both factors. It is recommended that the maintenance team consider this proposed<br />

method in future revisions <strong>of</strong> the standard.<br />

It has also been proposed that in future revisions <strong>of</strong> the standard indicative values should be given <strong>for</strong><br />

secondary loads and loads on secondary structures. In some instances these may be higher than loads on<br />

primary structures, so it is important they are well defined. It is recommended that this proposal be discussed<br />

by the Maintenance Team.<br />

Annex E: Ice loading<br />

Annex E <strong>of</strong> the standard provides guidance with regard to ice load calculations The standard states that<br />

the following ice loads should be assessed:<br />

• horizontal load due to temperature fluctuation in a fast ice cover (thermal ice pressure);<br />

• horizontal load from a fast ice cover subject to water level fluctuations and in terms <strong>of</strong> arch effect;<br />

• horizontal load from moving ice floes;<br />

• pressure from hummocked ice and ice ridges due to both subduction and ridging processes;<br />

• vertical <strong>for</strong>ce from fast ice covers subject to water level fluctuations.<br />

38<br />

⎤⎪⎫<br />

⎥⎦<br />

⎤⎫<br />

⎪<br />

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