The elastic strain energy stored in a rectangular cantilever beam of length $L$, subjected to a bending moment $M$ applied at the end of it is:
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For cantilever beams with a moment at the end, remember that bending moment is constant throughout the length. Use $\dfrac{M^2 L}{2EI}$ for stored strain energy.
The elastic strain energy $U$ stored in a beam due to bending is given by:
\[
U = \int_0^L \frac{M(x)^2}{2EI} dx
\]
For a cantilever beam of length $L$ with a moment $M$ applied at the free end, the moment throughout the beam is constant and equal to $M$.
Substitute this into the equation:
\[
U = \int_0^L \frac{M^2}{2EI} dx = \frac{M^2}{2EI} \int_0^L dx = \frac{M^2 L}{2EI}
\]
Hence, the strain energy stored is $\dfrac{M^2 L}{2EI}$.