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Preface The expedition ARK XIX/3 with the German icebreaking RV ...

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Sound velocity:<br />

As <strong>the</strong> cores all contained gas, <strong>the</strong> signal amplitude was generally very low and often<br />

zero. Interpretation of <strong>the</strong>se data <strong>with</strong> respect to travelling times (and thus, sound<br />

velocities) is critical. However, travelling times for all cores were estimated to be<br />

between 1000 and 1300 m/s for <strong>the</strong> longer cores. <strong>The</strong> Short cores (< 2m) and <strong>the</strong><br />

‘cold core’ showed <strong>the</strong> same low velocities at depth but at <strong>the</strong> very top, where good<br />

acoustic coupling was present, sound velocities reached 1700 m/s.<br />

Fig. B3.2-1: Triangles indicate <strong>the</strong> positions where gravity cores were taken.<br />

Susceptibility:<br />

Susceptibility (10 -6 SI) was quite homogeneous ranging between 100 and 200 in most<br />

of <strong>the</strong> cores at all depths. <strong>The</strong> ‘cold core’ has two layers of enhanced susceptibility of<br />

about 300 at approx. 0.7 and 4.4m depth. <strong>The</strong> core PS64/371 shows enhanced<br />

susceptibilities in <strong>the</strong> upper 30 cm reaching values of 440.<br />

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