Page 208 - Handbook of Civil Engineering Calculations, Second Edition
P. 208

HANGERS, CONNECTORS, AND WIND-STRESS ANALYSIS  1.191

                              it is clockwise; an angular displacement is positive if the rotation is clockwise; the trans-
                              verse displacement   is positive if it rotates the member in a clockwise direction.
                                Computing the end rotations gives 	 a   (L/6EI)(2M a , – M b ) +  /L; 	 b   (L/6EI)(–M a
                              + 2M b ) +  /L. These results may be obtained by applying the moment-area method or
                              unit-load method given in Sec. 1.
                              2. Solve the foregoing equations for the end moments
                              Thus,

                                         
 
            3           
 
           3
                                          2EI
                                                                     2EI
                                    M a        2	 a + 	 b –     M b       	 a + 2	 b –      (4)
                                                                      L
                                                                                   L
                                                        L
                                           L
                              These are the basic slope-deflection equations.
                              3. Compute the value of I/L for each member of the bent
                              Let K denote this value, which represents the relative stiffness of the member. Thus K ab
                                100/20   5; K cd   144/24   6; K be   300/30   10; K ce   60/15   4. These values are
                              recorded in circles in Fig. 18.
                              4. Apply Eq. 4 to each joint in turn
                              When the wind load is applied, the bent will deform until the horizontal reactions at the
                              supports total 10 kips (44.5 kN). It is evident, therefore, that the end moments of a mem-
                              ber are functions of the relative rather than the absolute stiffness of that member. There-
                              fore, in writing the moment equations, the coefficient 2EI/L may be replaced with I/L; to
                              view this in another manner, E   /2.
                                                      1
                                Disregard the deformation associated with axial forces in the members, and assume
                              that joints B and C remain in a horizontal line. The symbol M ab denotes the moment ex-
                              erted on member  AB at joint  A. Thus  M ab   5(	 b – 3 /20)    5	 b – 0.75 ;  M dc
                              6(	 c – 3 /24)   6	 c – 0.75 ; M ec   4(	 c + 3 /15)   4	 c + 0.80 ; M ba   5(2	 b – 3 /20)
                                10	 b – 0.75 ; M cd   6(2	 c – 3 /24)   12	 c – 0.75 ; M ce   4(2	 c + 3 /15)   8	 c +
                              0.80 ; M cd   10(2	 b + 	 c )   20	 b + 10	 c ; M cb   10(	 b + 2	 c )   10	 b + 20	 c .
                              5. Write the equations of equilibrium for the joints
                              and for the bent
                              Thus, joint B, M ba + M bc   0, Eq. a; joint C, M cb + M cd + M ce   0, Eq. b. Let H denote the
                              horizontal reaction at a given support. Consider a horizontal force positive if directed to-
                              ward the right. Then H a , + H d + H e + 10   0, Eq. c.
                              6. Express the horizontal reactions in terms of the end moments
                              Rewrite Eq. c. Or, (M ab + M ba )/20 + (M dc + M cd )/24 – (M ec + M ce )/15 + 10   0, or 6M ab +
                              6M ba + 5M dc + 5M cd – 8M ec – 8M ce   –1200, Eq. c
.
                              7. Rewrite Eqs. a, b, and c
 by replacing the end moments
                              with the expressions obtained in step 4
                              Thus, 30	 b + 10	 c – 0.75   0, Eq. A; 10	 b + 40	 c + 0.05   0, Eq. B; 90	 b – 6	 c –
                              29.30   –1200, Eq. C.
                              8. Solve the simultaneous equations in step 7 to obtain the
                              relative values of 	 b , 	 c , and
                              Thus 	 b   1.244; 	 c   –0.367;    44.85.
                              9. Apply the results in step 8 to evaluate the end moments
                              The values, in foot-kips, are: M ab   –27.42 (–37.18 kN·m); M dc   –35.84 (–48.6 kN·m);
                              M ec   34.41 (46.66 kN·m); M ba   –21.20 (–28.75 kN·m); M cd   –38.04 (–51.58 kN·m);
                              M ce   32.94 (44.67 kN·m); M bc   21.21 (28.76 kN·m); M cb   5.10 (6.92 kN·m).
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