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I, (I 11 g /' a 11 g (' S " (> C k wa v (' sIr 0111 a {a r g (' (' .r fJ { 0 s i (111 IIIl d (' r 11'£1 I (' r: (' .r fJ (' r i fI/ (' 11 I all d d a I a<br />

with sufficient buoyancy to hold the charge taut at Sm from the sea bed.<br />

(Fig 2.4). The purpose of detonation 5 m above the sea-bed is to instigate<br />

against energy loss in simple rock fracturing, probable with detonation on<br />

the sea-bed. Detonation 5 m above the sea-bed, a distance less than the<br />

bubble radius, ought to achieve slap-down of the pressure pulse<br />

impulsively on the sea-bed without extensive rock fracturing. This is<br />

seismically more efficient.<br />

The shot point for practical purposes at sea was defined as the shackle<br />

ring shown in Fig 2.4. The mooring arrangement consisted of two Class 5<br />

buoys wired together with each buoy anchored to the sea-bed so that the<br />

whole system was held under tension. The mid-point of the wire connecting<br />

the two buoys consisted of a shackle ring which lay below sea level. The<br />

shackle ring was connected to a free floating orange marker buoy so that<br />

it could easily be retrieved when required, for example, to locate the<br />

precise shot point when the charge was to be lowered.<br />

The detonation cable was to be reeled out from a drum with small<br />

sponge-like floats<br />

through the shackle<br />

distances for the<br />

attached every few metres (see photographs), and fed<br />

ring down to the charge. Anticipated stand-off<br />

Goosander at shot-time were 1500' and 750' for the<br />

larger and smaller charge size respectively.<br />

2.5 PREDICTED SIGNAL AMPLITUDES AND EXPLOSION SOURCE PARAMETERS<br />

It was expected that the equipment deployed on the sea-bed at different<br />

distances from the explosions would need to span a wide range of signal<br />

amplitudes. It was necessary to forecast the approximate amplitude of<br />

direct pressure waves and seismic ground motions at each proposed site so<br />

that instrumental gains could be set accordingly.<br />

2,:;.' Press/I/"(' wav(':<br />

Standard expressions given by Cole (1948) for the direct shock or pressure<br />

wave P(t) MPa from an underwater explosion, detonated at time t = 0, are<br />

of the form:<br />

P(t)<br />

12<br />

(2.1)

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