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5003 Lectures - Faculty of Engineering and Applied Science

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E<strong>5003</strong> - Ship Structures I 113<br />

© C.G. Daley<br />

k =<br />

44<br />

AE<br />

L<br />

,<br />

− AE<br />

k 14 = , k 24 = k 34 = k 54 = k 64 = 0<br />

L<br />

This has given us 12 terms, 1/3 <strong>of</strong> all the terms we need. Next we will find the<br />

terms for the #2 <strong>and</strong> #5 direction.<br />

Shear Terms<br />

The shear terms are found from the set <strong>of</strong> forces is required to create a unit<br />

displacement at d.o.f. #2 (<strong>and</strong> only #2);<br />

For shear <strong>of</strong> this type, the deflection is;<br />

3<br />

F 2L<br />

F 2 12 EI<br />

δ 2 = = 1 ⇒ = k 22 = 3<br />

12 EI δ<br />

L<br />

Note: to derive this easily, think <strong>of</strong> the beam as two cantilevers, each L/2<br />

long, with a point load at the end, equal to F2.<br />

The force at d.o.f. #5 is equal <strong>and</strong> opposite to the force at #2;<br />

F<br />

5<br />

= −F<br />

2<br />

2<br />

2<br />

F 5 ⇒ = k<br />

δ<br />

52<br />

− 12 EI<br />

= 3<br />

L<br />

Following from the double cantilever notion, the end moments (M3, M6) are ;

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