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Review of Cabling Techniques and Environmental Effects Applicable

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Sheringham Shoal Offshore Wind Farm<br />

Physical change<br />

A broadly similar approach was adopted by HR Wallingford, for the assessment<br />

<strong>of</strong> ploughing operations for the Sheringham Shoal Offshore Wind Farm.<br />

However, within the study a more sophisticated approach was adopted for the<br />

dispersion <strong>of</strong> fine sediment using the dispersion model SEDPLUME-RW. The<br />

model used the hydrodynamic output from a TELEMAC-2D flow model <strong>and</strong> the<br />

assumption <strong>of</strong> a logarithmic velocity pr<strong>of</strong>ile through the water column to track<br />

the 3-dimensional movement <strong>of</strong> fine sediment particles (mobile surface layer<br />

comprising s<strong>and</strong>y gravel with less than 4% fines). The results indicated that<br />

dispersion <strong>of</strong> sediment was rapid with concentrations dropping to less than<br />

1mg/l above background within a single flood or ebb excursion. It was noted that<br />

dispersion occurred at a slower rate on a neap tide than a spring tide because<br />

<strong>of</strong> the lower rate <strong>of</strong> turbulent diffusion with footprints 4km <strong>and</strong> 9km either side<br />

<strong>of</strong> the cable route. The scenarios included ploughing through chalk, ploughing<br />

through a silt/clay/s<strong>and</strong> mix <strong>and</strong> trenching through chalk.<br />

For ploughing chalk during a neap tide, the dispersion footprint extends for<br />

around 9km in each direction, with concentrations dropping to levels <strong>of</strong> less than<br />

1mg/l (above background) within a single flood or ebb excursion. For the spring<br />

tide simulation the higher turbulence causes the chalk concentrations to drop<br />

below 1mg/l (above background) within 4km <strong>of</strong> the cable route.<br />

The results for fines arising from other bed types with high percentages <strong>of</strong> fines,<br />

the neap tide footprint extends less than 2km, while the spring tide footprint is<br />

very small. As before the neap tide footprint is larger due to the lower rate <strong>of</strong><br />

turbulent diffusion. The extent <strong>of</strong> the footprint on both tides is less than that <strong>of</strong><br />

chalk due to the lower amount <strong>of</strong> material available per metre length <strong>of</strong> cable<br />

<strong>and</strong> the settling <strong>of</strong> silt during periods <strong>of</strong> slacker flows (chalk is assumed to have<br />

zero settling). This result is applicable to much <strong>of</strong> the inter-turbine cabling within<br />

the wind farm site where there are no exposures <strong>of</strong> chalk.<br />

The volume <strong>of</strong> material released by trenching through chalk is much higher,<br />

<strong>and</strong> therefore the extent <strong>and</strong> persistence <strong>of</strong> concentrations above 1mg/l is much<br />

greater. The predicted plume extends more than 10km in either direction at a<br />

level <strong>of</strong> up to 20mg/l (above background) on a neap tide. The model predicts<br />

a gradual drift <strong>of</strong> the plume towards the shore over the six tides, but that the<br />

plume has dispersed to less than 1mg/l concentration before the end <strong>of</strong> the<br />

model run.<br />

The footprint <strong>of</strong> silt deposition was found to extend over a wide area, but at<br />

an undetectable rate. Even under slack water conditions, the maximum rate<br />

<strong>of</strong> deposition over the six tide simulation was less than 0.5mm in the areas <strong>of</strong><br />

greatest deposition, <strong>and</strong> in most <strong>of</strong> the footprint area the rate was far less. This<br />

result is anticipated as the deposited fines will be re-suspended on each tide,<br />

with no measurable material left in place.<br />

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