Question 3.14: The bell crank shown in Figure 3-21 is part of a linkage in ...

The bell crank shown in Figure 3-21 is part of a linkage in which the 80-lb horizontal force is transferred to F_2 acting vertically. The crank can pivot about the pin at O. Draw a free body diagram of the horizontal part of the crank from O to A. Then draw the shearing force and bending moment diagrams that are necessary to complete the design of the horizontal arm of the crank.

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Objective         Draw the free-body diagram of the horizontal part of the crank in Figure 3-21. Draw the
shearing force and bending moment diagrams for that part.
Given                 The layout from Figure 3-21.

Analysis Use the entire crank first as a free body to determine the downward force F_2 that reacts to the applied horizontal force F_1 of 80 lb by summing moments about the pin at O.
Then create the free-body diagram for the horizontal part by breaking it through the pin and replacing the removed part with the internal force and moment acting at the break.

Results We can first find the value of F_2 by summing moments about the pin at O using the entire crank:

F_1.a = F_2.b
F_2 = F_1(a/b) = 80 \ lb( 1.50/2.00) = 60 \ 1b

Below the drawing of the complete crank, we have drawn a sketch of the horizontal pai1, isolating it from the vertical part. The internal force and moment at the cut section are shown. The externally applied downward force   F_2 . is reacted by the upward reaction at the pin. Also, because   F_2 causes a moment with respect to the section at the pin, an internal reaction moment exists, where

M = F_2.b = (60 \ lb)(2.00 \ in) = 120  lb-in

The shear and moment diagrams can then be shown in the conventional manner. The result looks much like a cantilever that is built into a rigid support. The difference here is that the reaction moment at the section through the pin is developed in the vertical arm of the crank.

Comments        Note that the shape of the moment diagram for the horizontal part shows that the maximum moment occurs at the section through the pin and that the moment decreases linearly as we
move out toward point A. As a result, the shape of the crank is optimized, having its largest cross section (and section modulus) at the .section of highest bending moment. You could complete the design of the crank using the techniques reviewed in Section 3-15.

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