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5003 Lectures - Faculty of Engineering and Applied Science

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E<strong>5003</strong> - Ship Structures I 208<br />

© C.G. Daley<br />

Consider a channel section. A channel is a common<br />

structural pr<strong>of</strong>ile, but one that is asymmetric on<br />

one axis. The center <strong>of</strong> area (centroid) <strong>and</strong> the<br />

‘shear center’ are not at the same location.<br />

What is the centroid? For one thing, it is a<br />

property <strong>of</strong> the cross sectional area. But what does<br />

it mean for the channel section? If we were to<br />

want to use the section as a column <strong>and</strong> apply an<br />

axial force that would only compress (<strong>and</strong> not<br />

bend) the column, we would apply the force at the<br />

centroid ‘g’. This is because a uniform stress in<br />

the cross section would have a ‘center <strong>of</strong> force’ at<br />

‘g’.<br />

To find ‘g’ we use the st<strong>and</strong>ard formulations;

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