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

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ExAmpLE 7.7

Draw the shear-force and bending-moment diagrams for the

simply supported beam shown. Determine the maximum

bending moment that occurs in the span.

Plan the Solution

A

This example focuses on finding the maximum moment in a

beam that has a uniformly distributed load. To calculate the

maximum moment, we must first find the location where V = 0.

To do this, we will determine the slope of the shear-force diagram from the intensity of

the distributed loading, using Rule 3. Once the location where V = 0 is established, the

maximum bending moment can be calculated from Rule 4.

SolutioN

Support Reactions

An FBD of the beam is shown. For the purpose of calculating

external beam reactions, the −1.5 kN/m distributed load can be

replaced by its resultant force of (1.5 kN/m)(4 m) = 6 kN

acting downward at the centroid of the loading. The equilibrium

equations are as follows:

Σ F = A + C − 6kN = 0

y y y

Σ M = − (6 kN)(2 m) + C (6m) = 0

A

From these equations, the beam reactions are

A

y

= 4kN and C = 2kN

y

y

A

y

y

A y

2 m

1.5 kN/m

4 m 2 m

6 kN

1.5 kN/m

4 m 2 m

B

B

C

C

C y

x

x

Construct the Shear-Force Diagram

On the load diagram, show the reaction forces acting in their proper directions. The original

distributed load—not the 6 kN resultant force—should be used to construct the V

diagram. The resultant force can be used to determine the external beam reactions; however,

it cannot be used to determine the variation in shear force in the beam.

The steps that follow are used to construct the V diagram. (Note: The lowercase

letters on the diagram correspond to the explanations given for each step.)

a V(0 – ) = 0 kN (zero shear at end of beam).

b V(0 + ) = 4 kN (Rule 1: V diagram jumps up by an amount

equal to the 4 kN reaction force).

c V(4) = −2 kN (Rule 2: The change in shear force, ∆V, is

equal to the area under the w curve). The area under the

w curve between A and B is (−1.5 kN/m) (4 m) = −6 kN;

therefore, ∆V = −6 kN. Since V b = +4 kN, the shear force

at c is V b = +4 kN – 6 kN = −2 kN.

Because w is constant between A and B, the slope of

the V diagram is also constant (Rule 3) and equal to

−1.5 kN/m between b and c. Consequently, the V diagram

is linear in this region.

d V(6 − ) = −2 kN (Rule 2: The area under the w curve is

zero between B and C; therefore, ∆V = 0).

A

y

1.5 kN/m

4 m 2 m

4 kN 2 kN

4 kN

V

b

a

(1)

1

2.667 m

1.5 kN/m

e V(6 + ) = 0 kN (Rule 1: V diagram jumps up by an amount equal to the 2 kN reaction

force and returns to V = 0 kN).

f

B

(2) (3)

c

e

d

C

x

–2 kN

215

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