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

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ExAmpLE 9.1

M A = 11.0 kN·m

A

z

(1)

B

(2)

(3)

30 mm 150 mm

30 mm

(1)

(2)

y

(3)

x

M B = 16.5 kN·m

30 mm

100 mm

A beam segment is subjected to the internal bending moments

shown. The cross-sectional dimensions of the beam are given.

(a) Sketch a side view of the beam segment, and plot the

distribution of bending stresses acting at sections A and B.

Indicate the magnitude of the key bending stresses in the

sketch.

(b) Determine the resultant forces acting in the x direction on

area (2) at sections A and B, and show these resultant

forces in the sketch.

(c) Is the specified area in equilibrium with respect to forces

acting in the x direction? If not, determine the horizontal

force required to satisfy equilibrium for the specified

area and show the location and direction of this force in

the sketch.

Plan the Solution

After the section properties are computed, the normal stresses

produced by the bending moment will be determined from the flexure

formula. In particular, the bending stresses acting on area (2) will be calculated.

From these stresses, the resultant forces acting in the horizontal direction at each end of

the beam segment will be computed.

SolutioN

(a) The centroid location in the z direction can be determined from symmetry. The

centroid location in the y direction must be determined for the U-shaped cross section.

The U shape is subdivided into rectangular shapes (1), (2), and (3), and the y centroid

location is calculated from the following:

50 mm

30 mm 150 mm

30 mm

Ref. axis

15 mm

(1)

(2)

(3)

30 mm

100 mm

A i (mm 2 ) y i (mm) y i A i (mm 3 )

(1) 3,000 50 150,000

(2) 4,500 15 67,500

(3) 3,000 50 150,000

10,500 367,500

yA

3

i i 367,500 mm

y = = = 35.0 mm

2

A 10,500 mm

i

Thus, the z centroidal axis is located 35.0 mm above the reference axis for the U-

shaped cross section. Next, the moment of inertia about the z centroidal axis is calculated.

The parallel-axis theorem is required, since the centroids of areas (1), (2), and

(3) do not coincide with the z centroidal axis for the U shape. The complete calculation

is summarized in the following table.

322

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