Page 461 - Design of Reinforced Masonry Structures
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SHEAR WALLS                       7.23

                                                y
                                 k 1






                                 k 2
                                                           P



                                 k 3



                     FIGURE 7.19  “Springs in parallel” concept.
             The left side of Eq. (7.32) represents force per unit displacement, which is defined
             as rigidity. If we express P/y = k = system stiffness, then
                                    k = k  + k  + k                  (7.33)
                                       1
                                              3
                                          2
             In general, Eq. (7.33) can be expressed as Eq. (7.34):
                                         n
                                      k = ∑ k                        (7.34)
                                           i
                                         i=1
             Equation (7.34) states that the rigidity of a system of springs in parallel equals the sum
             of the rigidities of individual springs. Method A is essentially based on this concept.
                                          (b)   Springs in series concept: In a system
                                            of springs in a series, all springs experi-
                                            ence the same spring force because the
                                            same force must be transferred from one
                k 1
                                   y 1 =  P  spring to the other (Fig. 7.20). However,
                               k 1
                                      k 1   each spring undergoes different dis-
                                            placement depending on its stiffness.
                k 2  y 1
                                            Consider again that three springs, having
                                            stiffnesses,  k ,  k , and  k , respectively,
                                                              3
                                                      1
                                                         2
                k 3                    P    are connected to each other end-to-end.
                               k 2  y 2 =
                                            can be expressed as spring force divided
                  y 1 + y 2           k 2   The displacements of these three springs
                                            by spring stiffness. Thus,
                                      P
                                   y =                   P
            y 1 + y 2 + y 3    k 3                   y =
                                      k 3             1
                                                         k
                                                         1
                                                     y =  P          (7.35)
                                                      2
                                                         k 2
                            P                        y =  P
                                                      3
         FIGURE 7.20  “Springs in series” concept.       k 3
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