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                 168    Mechanical Engineering Design



                       EXAMPLE 4–11       For the wire form of diameter d shown in Fig. 4–11a, determine the deflection of
                                          point B in the direction of the applied force F (neglect the effect of transverse shear).

                                Solution  Figure 4–11b shows free body diagrams where the body has been broken in each section,
                                          and internal balancing forces and moments are shown. The sign convention for the force
                                          and moment variables is positive in the directions shown. With energy methods, sign
                                          conventions are arbitrary, so use a convenient one. In each section, the variable  x is
                                          defined with its origin as shown. The variable x is used as a variable of integration for
                                          each section independently, so it is acceptable to reuse the same variable for each sec-
                                          tion. For completeness, the transverse shear forces are included, but the effects of trans-
                                          verse shear on the strain energy (and deflection) will be neglected.
                                              Element BC is in bending only so from Eq. (4–31), 5

                                                             ∂U BC    1     a           Fa 3
                                                                   =        (Fx)(x) dx =                      (1)
                                                              ∂F     EI  0              3EI
                                          Element CD is in bending and in torsion. The torsion is constant so Eq. (4–30) can be
                                          written as
                                                                    ∂U       ∂T     l
                                                                        = T
                                                                    ∂F i     ∂F i  GJ

                  Figure 4–11
                                               G
                                                             c

                                             F
                                                  B                  D
                                              a
                                                               b
                                                    C

                                                        (a)

                                                                                                       = Fb
                                                                                                   M DG2
                                                                                            F
                                                                                                         x
                                           F               F          M CD  = Fx   F    B                  D
                                               B                B
                                                                          T CD  = Fa            = Fa
                                            x                                               M DG1
                                                            a                       a              b
                                                                 C                       C
                                                                       x   V  = F
                                                                            CD
                                                  V  = F
                                                  BC
                                          M  = Fx
                                            BC
                                                                           (b)
                                          5 It is very tempting to mix techniques and try to use superposition also, for example. However, some subtle
                                          things can occur that you may visually miss. It is highly recommended that if you are using Castigliano’s
                                          theorem on a problem, you use it for all parts of the problem.
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