Given a beam ($\rho, A, l$) rotating with angular velocity $\omega$, find the maximum stress in the beam and its location.
I think the maximum stress occurs at the base, because the resultant force is the entire axial force. The total axial force is:
$$F = \int_0^l\frac{m}{l}\omega^2r\ dr = \frac{m\omega^2l}{2}$$ $$m = \rho Al$$ $$\sigma_{max} = \frac{F}{A} = \frac{\rho\omega^2 l^2}{2}$$
Did I do this right?
The follow-up question is, what happens when the beam is extremely thin: $t << l$
I don't know how to answer the follow-up.
