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instrument mechanism / verified-with-binding-errata
Damped Vibration Response Calculator mechanism
The inspectable method record for Damped Vibration Response Calculator, kept separate from implementation and qualification.
Model scope
The honest label correctly identifies a linear single-DOF viscous damping model, but it should additionally state that the cosine response and logarithmic decrement apply only to underdamped free vibration. The instrument needs explicit ωn, logarithmic-decrement, domain, and initial-condition definitions before it can be considered correct.
- The damped-frequency formula ωd=ωn√(1−ζ²) is valid only for the underdamped domain 0≤ζ<1; ζ=1 is critical damping and ζ>1 produces no real oscillation frequency.
- The response formula x(t)=Xe^(−ζωnt)cos(ωdt−φ) is valid only for underdamped free vibration and requires X and φ, or equivalent initial conditions x(0) and v(0), which are not listed as inputs.
- The logarithmic decrement output is listed but its formula is missing. For an underdamped system it should be δ=ln(x_n/x_(n+1))=2πζ/√(1−ζ²), using successive same-sign peak amplitudes.
- The formula does not specify the undamped natural frequency ωn=√(k/m), which is required to evaluate both ωd and the decay exponent.
- The specification does not define behavior for critically damped or overdamped systems, although the stated inputs permit those cases.
Units and conventions
- k is positive stiffness in N/m.
- m is positive mass in kg.
- c is viscous damping coefficient in N·s/m.
- ωn and ωd are angular frequencies in rad/s; radians are dimensionless in arithmetic.
- ζ is dimensionless and, for passive viscous damping, must satisfy ζ≥0.
- When c is supplied, ζ=c/(2√(km)); when ζ is supplied instead, c is implied by c=2ζ√(km).
Inspectable vector
One of 4 source-bound review vectors:
{
"inputs": {
"k": 100,
"m": 1,
"c": 0,
"X": 0.05,
"phi": "0 rad",
"sample_times": [
"0 s",
"π/20 s",
"π/10 s"
]
},
"expected_outputs": {
"omega_n": "10 rad/s",
"zeta": 0,
"omega_d": "10 rad/s",
"logarithmic_decrement": 0,
"sampled_points": {
"t=0 s": "x=0.05 m",
"t=π/20 s": "x=0 m",
"t=π/10 s": "x=-0.05 m"
},
"curve_features": {
"decay_envelope": "x=±0.05 m",
"roots": "t=(π/2+nπ)/10 s, n integer",
"successive_extrema": "t=nπ/10 s, x=0.05(-1)^n m"
}
},
"working": "ωn=√(k/m)=√(100/1)=10 rad/s. ζ=c/(2√(km))=0/(2√(100·1))=0. ωd=10√(1−0²)=10 rad/s. δ=2π·0/√(1−0²)=0. Response: x(t)=0.05e^(−0·10t)cos(10t)=0.05cos(10t). At t=0: x=0.05cos(0)=0.05 m. At t=π/20: 10t=π/2, so x=0.05cos(π/2)=0 m. At t=π/10: 10t=π, so x=0.05cos(π)=−0.05 m."
}Failure boundary
BREAK_CLAIMED · SELF_FLAGGED
The instrument breaks at zero mass through division by zero, reaches a validity failure at critical damping, produces a non-real damped frequency when the damping-ratio branch switches to overdamping, and has an unresolved signed-damping convention that can reverse decay into growth.
Other records
Sources and evidence
These pointers bind the page to evidence. They do not grant authority or collapse verification into deployment.
VERIFIED_LEDGER.jsonevidence-tranche6/tranche6-results.jsonBOUNDARY_HAZARD_CATALOG.json