________________________________________________________________________ PROBLEMS (10.10 and 10.11) A cantilever beam is loaded as depicted in Fig. P10.10 and P10.11. Using the double-integration approach, determine: (a) The equation of the deflection curve. (b) The slope at the free end. (c) The deflection at the free end. SOLUTION (10.10) (a) y PL P A L/2 C L/2 B x M 1 = PL (0 ≤ x ≤ L 2) 3 L M 2 = PL − Px ( ≤ x ≤ L) 2 2 Segment AC EIv1 '' = PL EIv1 ' = PLx + C1 1 EIv1 = PLx 2 + C1 x + C2 2 Segment BC 3 EIv2 '' = PL − Px 2 3 1 EIv2 ' = PLx − Px 2 + C3 2 2 3 1 EIv2 = PLx 2 − Px3 + C3 x + C4 4 6 Boundary conditions: 3 2 1 2 v2 '( L) = 0 : PL − PL + C3 = 0, C3 = − PL2 2 2 3 3 1 3 5 v2 ( L) = 0 : PL − PL − PL3 + C4 = 0, C4 = PL3 4 6 12 Thus, P (3Lx − x 2 − 2 L2 ) v2 ' = 2 EI P (9 Lx 2 − 2 x 3 − 12 L2 x + 5 L3 ) v2 = 12 EI (1) (2) Continued on next slide Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. Continuity conditions: 1 2 3 L L v1 '( ) = v2 '( ) : PL + C1 = − PL2 , 2 2 2 8 5 L L PL3 , v1 ( ) = v2 ( ) : − PL3 + C2 = − 2 2 16 12 7 C1 = − PL2 8 19 C2 = − PL2 48 Therefore, P (−8 Lx − 7 L2 ) 8 EI P (24 Lx 2 − 42 L2 x + 19 L3 ) v1 = 48 EI v1 ' = (3) (4) (b) x=0 in Eq. (3): 7 PL2 7 PL2 θA = − = 8 EI 8 EI (c) x=0 in Eq. (4): 19 PL3 vA = − ↑ 48 EI SOLUTION (10.11) y (a) w MA=2wa2 A 2a C a B x RA=2wa M1 = 1 w(−4a 2 + 4ax − x 2 ) 2 M2 = 0 (0 ≤ x ≤ 2a ) L ( ≤ x ≤ L) 2 Continued on next slide Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. Segment AC w EIv1 '' = (−4a 2 + 4ax − x 2 ) 2 w x3 EIv1 ' = (−4a 2 x + 2ax 2 − ) + C1 2 3 2 3 x4 w 2 2 EIv1 = (−2a x + ax − ) + C1 x + C2 2 3 12 Boundary conditions: v1 '(0) = 0 : C1 = 0, v1 (0) = 0 : C2 = 0 Thus, w (−12a 2 x + 6ax 2 − x 3 ) v1 ' = 6 EI w (−24a 2 x 2 + 8ax 3 − x 4 ) v1 = 24 EI Segment BC EIv2 '' = 0, EIv2 ' = C3 , (1) (2) EIv2 = C3 x + C4 Continuity conditions: 4 v1 '(2a) = v2 '(2a) : − wa 3 = C3 3 8 v1 (2a ) = v2 (2a ) : − 2wa 4 = − wa 4 + C4 , 3 2 C4 = − wa 4 3 Therefore, 4 wa 3 3 EI wa 3 (−4 x + 2a) v2 = 3EI v2 ' = − (3) (4) (b) x=3a in Eq. (3): 4 wa 3 4 wa 3 θB = − = 3 EI 3 EI (c) x=3a in Eq. (4): 10 wa 4 10 wa 4 vB = − = ↓ 3 EI 3 EI Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful.