Take the clamp at with . An end force without an applied end moment gives the free-end condition . With , the Euler elastica equation is . For , is small, so the leading equation is
Integrating with the two boundary conditions gives
To first order, and . Hence
Equivalently at leading order, the familiar cantilever response. Because , the deflection is downward. The free-end displacement field and slope are and . The remainder notation holds with fixed positive and nondimensional unit rod length.

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