446 CHAPTER 15 Bending of Open and Closed, Thin-Walled Beams
Fig.15.18
Deflection of a simply supported beam carrying a uniformly distributed load.
SubstitutingforMinthesecondofEq.(15.32),weobtain
EIv′′=
w
2
(Lz−z^2 ) (ii)
Integrating,wehave
EIv′=
w
2
(
Lz^2
2
−
z^3
3
)
+C 1
Fromsymmetryitisclearthatatthemidspansectionthegradientv′=0.
Hence,
0 =
w
2
(
L^3
8
−
L^3
24
)
+C 1
whichgives
C 1 =−
wL^3
24
Therefore,
EIv′=
w
24
( 6 Lz^2 − 4 z^3 −L^3 ) (iii)
Integratingagaingives
EIv=
w
24
( 2 Lz^3 −z^4 −L^3 z)+C 2