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5003 Lectures - Faculty of Engineering and Applied Science

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E<strong>5003</strong> - Ship Structures I 151<br />

© C.G. Daley<br />

For the 3 bar frame at left, we can define the<br />

define local degrees <strong>of</strong> freedom for each member<br />

using the same st<strong>and</strong>ard approach that was<br />

described in Chapter 11. We will start from the<br />

local element stiffness matrices <strong>and</strong> assemble the<br />

full structural global stiffness matrix, just to<br />

illustrate the process.<br />

The local degrees <strong>of</strong> freedom follow the individual<br />

members, while the global degrees <strong>of</strong> freedom are<br />

all aligned to the Cartesian (x-y) system. The<br />

other aspect is that global degrees <strong>of</strong> freedom refer<br />

to nodes <strong>of</strong> a structure, rather than to ends <strong>of</strong><br />

members. This means that several member ends<br />

can share a single set <strong>of</strong> degrees <strong>of</strong> freedom.<br />

The matrices below show the local <strong>and</strong> global<br />

versions <strong>of</strong> the stiffness matrix for beam 1. The<br />

difference is the way the degrees <strong>of</strong> freedom are<br />

defined. In this case the global degrees <strong>of</strong> freedom<br />

are just versions <strong>of</strong> the local d<strong>of</strong>s.

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