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

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To distinguish clearly bet ween elongations

4.5 m

that occur in the rods and deflections at locations

2.0 m

along the rigid bar, rigid-bar transverse deflections

(i.e., deflections up or down in this case) will be A B C D

denoted by the symbol v. Therefore, the rigid-bar

v B = δ 1

deflection at joint C is designated v C .

v C = δ 2

We will assume that there is a perfect fit in the

pin connection at joint C; therefore, the rigid-bar

deflection at C is equal to the elongation that occurs

in rod (2) (v C = δ 2 ).

From the deformation diagram of the rigid-bar geometry, the rigid-bar deflection v B

at joint B can be determined from similar triangles:

vB

vC

2.0 m

= ∴ vB

= (2.16 mm) = 0.96 mm

2.0 m 4.5 m

4.5 m

If there is a perfect fit in the connection between rod (1) and the rigid bar at joint B, then

rod (1) elongates by an amount equal to the rigid-bar deflection at B; hence, δ 1 = v B .

Knowing the deformation produced in rod (1), we can now compute its strain:

ε

1

δ1

0.96 mm

= = = 0.000640 mm/mm = 640 µε Ans.

L 1,500 mm

1

(b) As in part (a), the deformation in the rod can be computed as

ε

2

δ 2

⎡ 1mm/mm ⎤

= ∴ δ2 = ε2L 2 = (800 µε)

(2,700 mm) 2.16 mm

L

2

⎣1, 000,000 µε

⎥ =

Sketch the configuration of the rotated

rigid bar for case (b). In this case, there is

a 1 mm gap between rod (2) and the rigid

bar at C. Because of this gap, the rigid bar

will deflect 1 mm downward at C before it

begins to stretch rod (2). The total deflection

of C is made up of the 1 mm gap plus

the elongation that occurs in rod (2); hence,

v C = 2.16 mm + 1 mm = 3.16 mm.

As before, the rigid-bar deflection v B

at joint B can be determined from similar

triangles:

2.0 m

4.5 m

A B C D

v B = δ 1

δ 2 v C = δ 2 + 1 mm

1 mm

vB

vC

2.0 m

= ∴ vB

= (3.16 mm) = 1.404 mm

2.0 m 4.5 m

4.5 m

Since there is a perfect fit in the connection between rod (1) and the rigid bar at joint B,

it follows that δ 1 = v B , and the strain in rod (1) can be computed:

ε

1

δ1

1.404 mm

= = = 0.000936 mm/mm = 936 µε Ans.

L 1,500 mm

1

Compare the strains in rod (1) for cases (a) and (b). Notice that a very small gap at C

caused the strain in rod (1) to increase markedly.

33

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