Let be the cylinder centre's small displacement away from the wall. Rolling without slipping gives rotation angle of magnitude . The material point initially at the top moves horizontally by another relative to the centre to first order, so the spring extension is , not . Its small vertical displacement affects the extension only at higher order.
The kinetic and potential energies are
The linearized equation is , giving
Static friction enforces the rolling constraint and does no work at the instantaneous contact point. Omitting rotational kinetic energy, or attaching the spring to the centre instead of the top material point, would change the result.

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