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THE case now to be considered is shown diagrammatically in FIG. 12, which also gives the additional notation required. The problem is to determine how a bending moment, applied at one end to the longerons only, is diffused into the whole section, being finally distributed according to the usual beam theory of bending. The differential equation to be satisfied by the displacement w is equation B2, and if we take the origin at the centre we may take sR, hr, xR sin and yR cos . Equation B2 then becomes
Aircraft Engineering and Aerospace Technology – Emerald Publishing
Published: Sep 1, 1946
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