Page 412 - Design of Reinforced Masonry Structures
P. 412

WALLS UNDER GRAVITY AND TRANSVERSE LOADS      6.63

           First iteration:

                          5Mh  2  5 M(  − M )  h 2
                      δ  =   cr  +   ser  cr
                       ser
                          48EI      48EI cr
                                       m
                             mg
                                               −
                                                       ×
                           (
                                    12
                                            .
                                                  .
                         =  518.. )(96 20 2 )( )  +  ( 5 2882 1896))(20 12 ) 2
                           48 (1800 )(443 . )  48 (1800 )(20 .54 )
                                     3
                         =  . 0 143 1 .6
                              +
                         =  . 1 743 in.. > 000.  h  = 168  in.  NG
                                         .
           Therefore, increase wall reinforcing so as to increase I  which would reduce d . Try
                                                                    ser
                                                   cr
                                                2
           No. 4 vertical bars @ 16 in. on center; A  = 0.15 in.  (Table A.23).
                                        s
                             P +  A f  1 81 + 0 15 60)
                                           . (
                                       .
                         A =  u   s y  =         = 018.  in. 2
                          se
                                f  y      60
                          n = 16.11 (Table A.14)
                                    .
                          ρ =  A se  =  018  = 0 0039.
                             bd   () (  .
                                  12 3 81)
                         rn = (0.0039)(16.11) = 0.063
           From Table A.15, nr = 0.063, k = 0.2975
                   c = kd = (0.2975)(3.81) ≈ 1.13 in. < 1.25 in. (shell thickness)
           Therefore, the centroidal axis lies in the shell and the section can be treated as a rect-
           angular section.
                                      −
                         I =  bc 3  +  nA d c)  2
                                    (
                         cr
                             3     se
                             12 1 13)
                           =  () (  .  3  + 16 11 0.118 3 81 1 13)−  .  2
                                      (.)(
                                               )( .
                                3
                            =  26 6 . in. 4
                      δ  =  5Mh  2  +  5 M(  ser  − M )  h 2
                                         cr
                             cr
                       ser
                          48EI      48EI
                             mg        m  cr
                                               −
                                                       ×
                                                  .
                                    12
                                            .
                           (
                         =  518.. )(96 20 2 )( )  +  ( 5 2882 1896))(20 12 ) 2
                           48 (1800 )(443 . )  48 (1800 )(26 . )
                                     3
                                                      6
                              +
                         =  . 0 143 1 .236
                         =  . 1 379 inn. < 000.  h  = 168  in.  OK
                                         .
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