STATICS & STRENGTH OF MATERIALS - Example

A loaded, cantilever beam is shown below. For this beam:

A. Draw a Free Body Diagram of the beam, showing all external loads and support forces (reactions).
B
. Determine expressions for the internal shear forces and bending moments in each section of the beam.
C
. Make shear force and bending moment diagrams for the beam.
Unless otherwise indicated, all joints and support points are assumed to be pinned or hinged joints.

Solution:

Part A:
STEP 1: Draw a free body diagram showing and labeling all load forces and support (reaction) forces, as well as any needed angles and dimensions.
STEP 2
: Break any forces not already in x and y direction into their x and y components.
STEP 3
: Apply the equilibrium conditions.

Sum Fy = Ax = 0
Sum Fy =( -1,500 lbs/ft)(6 ft) - (1,000 lbs/ft)(4 ft) - 5,000 lbs + Ay = 0
Sum TA = (-1,500 lbs/ft)(6 ft)(3 ft) - (1,000 lbs/ft)(4 ft)(8 ft) - (5,000 lbs)(16 ft) + Mext = 0
Solving for the unknowns
:
Ay = 18,000 lbs; Mext = 139,000 ft-lbs

Part B: Determine the Shear Forces and Bending Moments expressions for each section of the loaded beam. For this process we will ‘cut’ the beam into sections, and then use Statics - Sum of Forces to determine the Shear Force expressions, and Integration to determine the Bending Moment expressions in each section of the beam.

Section 1: Cut the beam at x, where 0 <>

1. FBD. (Shown in Diagram)
2
. All forces in x & y components (yes)
3
. Apply translational equilibrium conditions (forces only):

Sum Fx = 0 (no net external x- forces)
Sum Fy = 18,000 lbs - 1,500 lbs/ft(x) - V1 = 0
Solving
:
V1 = [-1,500x + 18,000] lbs

4. Integration

M1 = -750x2 + 18,000x + C1

a)Boundary condition to find C1: at x=0 M=-139,000 ft-lbs (That is, for a cantilever beam, the value of the bending moment at the wall is equal to the negative of the external moment.)
Apply BC: -139,000 = -750(0)2 + 18000(0) + C1

Solving: C1 = -139,000
Therefore…
M1 = [-750x2 + 18,000x - 139,000] ft-lbs for 0 <>

Section 2: Cut the beam at x, where 6 <>

1. FBD. (Shown in Diagram)
2
. All forces in x & y components (yes)
3
. Apply translational equilibrium conditions (forces only):

Sum Fx = 0 (no net external x- forces)
Sum Fy = 18,000 lbs - (1,500 lbs/ft)(6 ft) -(1,000 lbs/ft)(x - 6)ft - V2 = 0
Solving
:
V2 = [-1,000x + 15,000] lbs

4. Integration

M2 = -500x2 + 15,000x + C2

a)Boundary condition to find C2: at x=6 ft M=-58,000 ft-lbs (from equation M1)
Apply BC: -58,000 ft-lbs = -500(6)2 + 15,000(6) + C2

Solving: C2 = -130,000 ft-lbs
Therefore…
M2 = [ -500x2 + 15,000x - 130,000] ft-lbs for 6 <>

Section 3: Cut the beam at x, where 10 <>

1. FBD. (Shown in Diagram)
2
. All forces in x & y components (yes)
3
. Apply translational equilibrium conditions (forces only):

Sum Fx = 0 (no net external x- forces)
Sum Fy = 18,000 lbs - (1,500 lbs/ft)(6 ft) - (1,000 lbs/ft)(4 ft) - V3 = 0
Solving
:
V3 = 5,000 lbs

4. Integration

M3 =5,000x + C3

a)Boundary condition to find C3: at x=16 ft M=0 ft-lbs (free end of beam, no external torque so M3=0)
Apply BC: 0 = 5,000(16) + C3

Solving: C3 = -80,000 ft-lbs
Therefore…
M3 = [5,000x - 80,000] ft-lbs for 10 <>

Part C: Shear Force and Bending Moment Diagrams: Now using the expressions found in Part B above, we can draw the shear force and bending moment diagrams for our loaded beam.

V1 = [-1,500x+18,000] lb V2 = [-1,000x+15,000] lb V3 = 5,000 lb
M1 =
[-750x2+18,000x-139,000] ft-lb M2 = [-500x2+15,000x-130,000] ft-lb M3 = [5,000x - 80,000] ft-lb

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