Simply supported beam—the Myosotis method

The sixth way we’ll derive the formula for the center deflection of a uniformly loaded simply supported beam is the Myosotis method, which I wrote about over a decade ago. This is the method popularized1 by J.P. Den Hartog in his Strength of Materials textbook.

Forget-me-not from Wikipedia

Image from Wikipedia.

Myosotis is the genus of the forget-me-not flower, and the idea behind the Myosotis method is to memorize the following six equations for the tip angle and deflection of a cantilever beam under different loading conditions.

Myosotis excerpt from Den Hartog

Once you have the formulas memorized, you can combine them to generate the solution for almost any beam that’s subjected to point and uniformly distributed loads. I wouldn’t say the Myosotis method is, or has ever been, a practical tool for working engineers, but it’s a great pedagogical tool for teaching engineering students how to take advantage of symmetry, antisymmetry, and superposition. Using it even a few times will get you thinking about how complex structural problems can be broken down into a combination of simpler solutions, and that will stay with you even if you never use the Myosotis method again.

We mentioned in the slope-deflection post that the left half of our simply supported beam behaves like a simple-guided beam. Let’s be more explicit about that. The symmetry of the problem we want to solve,

Simply supported beam with uniform load

means it deflects like two simple-guided beams back to back:

Shape of two half-beams back-to-back

This time, we’ll consider the right half:

Half-beam with guided and simple ends

Statics tells us that the upward reaction at the right support is wL/2.

This is, apart from an overall downward displacement, the same as a fixed-free beam with both a uniform load over its length and an upward load at its tip:

Half-beam with fixed and free ends

So the downward deflection at the center of our full-length simple-simple beam is equal to the left end deflection of our half-length guided-simple beam, which in turn is equal to the upward right end deflection of our half-length fixed-free beam. One of the purposes of a structural engineering education is to get you to see these relationships in a lot less time than it takes to type them out.

Now we can use superposition and two of the Myosotis formulas to get our answer. Here’s a graphical expression of how the superposition works:

Superposition for Myosotis solution

So the upward deflection of the right end of the fixed-free beam is

w(L/2)48EI+(wL/2)(L/2)33EI=wL4128EI+wL448EI=5wL4384EI

and that’s the same as the downward center deflection of our original problem, as expected.


  1. “Popularized” may be going a bit far; I’ve never seen the Myosotis method in any other book. Still, thanks to Dover, Den Hartog’s book is still in print, something you can’t say about many other textbooks from 1949.