Mechanical energy storage function
ID: mechanical-energy-storage-function
A mechanical energy storage function assigns a nonnegative stored-energy quantity to the state of a mechanical model so that its increase never exceeds entering work. For a one-port passive mechanical network with entering power , the mechanical dissipation inequality isThis state-based accounting includes energy present before the measurement begins. A temporary outward power is compatible with release of stored energy.[ref]
The Inerter: A Retrospective by Malcolm C. Smith. Accepted manuscript §17, p.24, equation(30), integrated terminal power and passivity
For an ideal linear spring, is elastic potential energy. For an ideal inerter, is kinetic energy associated with terminal relative motion. An ideal dashpot need not store mechanical energy: its entering power is dissipated. If these elements share terminals, their state variables obey andThis equality proves the inequality for . In a larger network, summing element balances cancels internal transfers, leaving power through the external terminals and total dissipation.
For an original numerical check, let , and . Start at and , so . Maintain that relative velocity for : displacement reaches and stored energy becomes . Dissipation is , so input work is . Counting all entering work as newly stored energy would overestimate storage.
The mechanical available storage is the maximum net work that could be recovered under allowed future terminal motions; it is a related operational quantity, rather than automatically every form of internal physical energy. A model's storage function is a certificate that must respect its accessible states and port variables. With zero external power, a positive-definite storage function can supply a Lyapunov function, but nonincreasing energy alone does not establish that every motion decays to rest: a lossless spring–inerter oscillation keeps a constant nonzero stored energy.
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