The pin-jointed column shown in Fig. 8.10 carries a compressive load P applied eccentrically at a distance e from the axis of the column. Determine the maximum bending moment in the column.
The pin-jointed column shown in Fig. 8.10 carries a compressive load P applied eccentrically at a distance e from the axis of the column. Determine the maximum bending moment in the column.
The bending moment at any section of the column is given by
M=P(e+v)
Then, by comparison with Eq. (8.1),
E I \frac{ d ^{2} v}{ d z^{2}}=-P_{ CR } V (8.1)
E I \frac{ d ^{2} v}{ d z^{2}}=-P(e+v)
giving
\frac{ d ^{2} v}{ d z^{2}}+\mu^{2} v=-\frac{P e}{E I}\left(\mu^{2}=P / E I\right) (i)
The solution of Eq. (i) is of standard form and is
v=A \cos \mu z+B \sin \mu z-e
The boundary conditions are v=0 when z=0 and ( d v / d z)=0 when z=L / 2. From the first of these, A=e, while from the second,
B=e \tan \frac{\mu L}{2}
The equation for the deflected shape of the column is then
v=e\left[\frac{\cos \mu(z-L / 2)}{\cos \mu L / 2}-1\right]
The maximum value of v occurs at mid-span, where z=L / 2; that is,
v_{\max }=e\left(\sec \frac{\mu L}{2}-1\right)
The maximum bending moment is given by
M(\max )=P e+P v_{\max }
so that
M(\max )=P e \sec \frac{\mu L}{2}