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Timothy A. Philpot - Mechanics of materials _ an integrated learning system-John Wiley (2017)

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112

AxIAL dEFORMATION

(1) (2)

P

x B

x C

A B C D

FIGURE 5.11a Configuration with two tension members.

(1) (2)

P

x B

A B C D

v B

v C

FIGURE 5.11b Deformation diagram.

x C

(1) (2)

x B L 1

L

L 1+ v 2

B

L 2+ v

A B C C

D

x C

v B

v C

FIGURE 5.11c Showing member deformations.

Therefore, the geometry-of-deformation equation can be written in terms of member

deformations as

δ1 δ2

=

x x

(5.7)

B

For the structure with two opposing axial members (Figure 5.11d), the geometry-of-deformation

equation in terms of joint deflections v B and v C is the same as before (Figure 5.11e):

v

x

B

B

C

v

=

x

From Figure 5.11f, the member deformations δ 1 and δ 2 are related to the joint deflections

v B and v C by

δ

= L − L = ( L + v ) − L = v ∴ v = δ

1 final initial 1 B 1 B B 1

C

C

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