Determine the deflection curve and the deflection of the free end of the cantilever shown in Fig. 15.17(a). The cantilever has a doubly symmetrical cross-section.
Determine the deflection curve and the deflection of the free end of the cantilever shown in Fig. 15.17(a). The cantilever has a doubly symmetrical cross-section.
The bending moment, M, at any section Z is given by
M=\frac{w}{2}(L-z)^{2} (i)
Substituting for M in the second of Eqs. (15.31) and rearranging, we have
u^{\prime \prime}=-\frac{M_{y}}{E I_{y y}}, \quad v^{\prime \prime}=-\frac{M_{x}}{E I_{x x}} (15.31)
E I v^{\prime \prime}=-\frac{w}{2}(L-z)^{2}=-\frac{w}{2}\left(L^{2}-2 L z+z^{2}\right) (ii)
Integration of Eq. (ii) yields
E I v^{\prime}=-\frac{w}{2}\left(L^{2} z-L z^{2}+\frac{z^{3}}{3}\right)+C_{1}
When z = 0 at the built-in end, v^{\prime}=0 so that C_{1}=0 and
E I v^{\prime}=-\frac{w}{2}\left(L^{2} z-L z^{2}+\frac{z^{3}}{3}\right) (iii)
Integrating Eq. (iii), we have
E I v=-\frac{w}{2}\left(L^{2} \frac{z^{2}}{2}-\frac{L z^{3}}{3}+\frac{z^{4}}{12}\right)+C_{2}
and since v = 0 when z = 0, C_{2}=0. The deflection curve of the beam therefore has the equation
v=-\frac{w}{24 E I}\left(6 L^{2} z^{2}-4 L z^{3}+z^{4}\right) (iv)
and the deflection at the free end when z = L, is
v_{\text {tip }}=-\frac{w L^{4}}{8 E I}
which is again negative and downward.