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 is
This state-based accounting includes energy present before the measurement begins. A temporary outward power is compatible with release of stored energy.[ref]
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 and
This 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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