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Acoustic properties · Dissipation

Loss factor and internal friction

Where does the energy go after a tap?

Loss factor describes the dissipative part of a material’s dynamic response. It supplies information that density and elastic modulus alone cannot provide.

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Start with something familiar

A playground swing gradually slows even after you stop pushing. Some mechanical energy becomes heat or leaves through the surroundings. Wood vibrations also lose energy, though the loss mechanisms are more varied.

Amplitude in time

Time →

f = 500 Hz · Q = 50 / 150

Peak width

Frequency →

Green: Q = 50 · Blue: Q = 150

Diagram · Equal-frequency, equal-start envelopes with different losses. These are calculated amplitude envelopes, not microphone recordings.
  1. Notice what changes

    Elastic storage is the recoverable part of deformation. Loss describes the portion not returned as mechanical vibration in each cycle; it is not the same quantity as mass or stiffness.

  2. Understand why

    At the same mode frequency and initial amplitude, greater loss leads to faster decay. Compare equal conditions: a quiet initial tap can disappear sooner simply because it began closer to noise.

  3. Connect it to wood and making

    A held blank also loses energy into the fingers or support. Separate material behaviour from the test arrangement before connecting a measured decay to wood selection.

Put names to the ideas

01

Storage and loss

For linear harmonic response, tan δ = E″/E′. Here η denotes that loss factor; notation varies, so define it rather than confusing it with a viscous coefficient in N·s/m.

02

An independent measurement

Two samples can share density and modulus yet have different decay. A damping measurement is required; deriving c, R and Z from the elastic quantities does not reveal η.

03

Measured loss includes the setup

Support contact, radiation, room contamination and recording processing can alter an observed decay. Reproducible specimen conditions are needed before attributing all measured loss to the material.

η≡tan⁡δ=E′′E′,Q≈1η\eta\equiv\tan\delta=\frac{E''}{E'},\qquad Q\approx\frac{1}{\eta}

η or tan δ compares the loss part with the storage part in a harmonic test. For weak damping, Q is approximately its reciprocal: more loss means smaller Q.

A worked example

In a lightly damped, isolated mode, η = 0.01 corresponds approximately to Q = 100. Halving η doubles Q, but decay time also depends on frequency.

Explore it yourself

Compare decay at the same frequency or state the frequency explicitly. Keep damping measured rather than inferred from a material grade.

TEACHING MODEL · LOCAL CALCULATION
τA
63.7 ms
Δf (−3 dB)
5.00 Hz
T60
0.44 s
A/A₀Time · 0–600 ms01
Normalized amplitude envelope. Same initial amplitude; a fixed 600 ms axis makes frequency and Q effects comparable.
A/Amaxf/f₀ · 0.8–1.201
Isolated-mode, weak-damping resonance approximation. Half-power amplitude is 0.707 of the peak.

Check your understanding

Can density and elastic modulus alone determine a sample’s measured loss?

References