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

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Longitudinal plane

of symmetry

y

B′ B

= 0

y

B′

τ B = 0

B

363

SHEAR STRESS ANd SHEAR

FLOw IN THIN-wALLEd

MEMbERS

z

x

z

V

x

τ B′

τ C′ = 0

C′

C

τ C = 0

C′

(a) Closed thin-walled section with a longitudinal

plane of symmetry

C

FIGURE 9.23 Shear stress in a thin-walled box cross section.

Shear flow and shear stress

must vanish on a longitudinal

plane of symmetry.

(b) Shear stresses at the plane of symmetry

ExAmpLE 9.7

A beam with the thin-walled inverted-tee-shaped cross section shown is

subjected to a vertical shear force V = 37 kN. The location of the neutral

axis is shown on the sketch, and the moment of inertia of the inverted-tee

shape about the neutral axis is I = 11,219,700 mm 4 . Determine the shear

stresses in the tee stem at points a, b, c, and d, and in the tee flange at points

e and f. Plot the distribution of shear stress in both the stem and flange.

Plan the Solution

The location of the neutral axis and the moment of inertia of the invertedtee

shape about the neutral axis are given. The value of Q associated with

each point will be determined from Q = y – ′A′ for the applicable portion A′

of the cross-sectional area. After Q is determined, the shear stress will be

calculated from Equation (9.16).

143.0 mm

43.0 mm

8 mm

50 mm

a

50 mm

b 186 mm

N.A.

c 8 mm

V

d

f e

55 mm

220 mm

SolutioN

Points a, b, and c are located in the stem of the inverted-tee shape. A horizontal cutting

plane that is perpendicular to the walls of the stem defines the boundary of area A′. For

these locations, area A′ begins at the cutting plane and reaches upward to the top of the

stem. Point d is located at the junction of the stem and the flange. For this location, the area

A′ is simply the area of the flange. Point e is also at the junction of the stem and the flange;

however, the shear stress in only the flange is to be determined at e. The area A′ corresponding

to point e extends from the left end of the flange to a vertical cutting plane located at the

centerline of the stem. (Note that the centerline location for the cutting plane is acceptable

because the shape is thin walled.) For point f in the flange, a vertical cutting plane defines

the boundary of area A′, which extends horizontally from the cutting plane to the outer edge

of the flange. For all points, the first moment Q is the moment of the area A′ about the neutral

axis of the inverted-tee shape. The shear stress at each point is calculated from

τ =

where V = 37 kN and I = 11,219,700 mm 4 . The thickness t is 8 mm for each location. The

results of these analyses are summarized in the following table:

VQ

It

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