Physical Transformation AtlasPTA
Phenomenon · phenomenon:thermoacoustic-effect

Thermoacoustic effect

A sufficiently steep temperature gradient along a porous stack in a resonant gas column drives self-sustained acoustic oscillation. Heat becomes sound with no moving parts.

Thermodynamicsfirst reported 1850also: Rijke tube, Sondhauss tube, thermoacoustic oscillation, thermoacoustic engine, thermoacoustic prime mover, thermoacoustic heat engine, thermoacoustic instability

Atlas record: 8 claims reference this phenomenon — 5 established and 3 demonstrated.

Explorerelations · matrix context · routes · sources · cite

conditions: gas · temperature gradient required
8claims64enumerated routes3routes with complete-composition evidence5candidate routes not searched5cited sources

Relations

drives · 1
Temperature gradient—drives→Thermoacoustic effectestablished
  • temperature gradient along the stack steeper than the critical gradient set by the acoustic pressure and displacement amplitudes
  • a resonant gas column
|∇T_crit| = β T_m ω |p₁| / (ρ_m c_p |u₁|); prime-mover onset requires |∇T| > |∇T_crit| · critical-gradient factor β T_m ω/(ρ_m c_p u₁) [K/(Pa·m)]
produces · 2
Thermoacoustic effect—produces→Acoustic waveestablished
Thermoacoustic effect—produces→Acoustic waveestablished
  • travelling-wave thermoacoustic regime with a non-zero time-averaged acoustic power flux; pressure and particle velocity have the phase relation required for directed acoustic power (a looped tube or a travelling-wave regenerator), unlike the standing wave of a straight resonator
member of · 1
Thermoacoustic effect—member of→Thermoacousticestablished
implemented by · 3
Thermoacoustic effect—implemented by→Thermoacoustic piezoelectric harvesterdemonstrated
Thermoacoustic effect—implemented by→Thermoacoustic triboelectric harvesterdemonstrated
Thermoacoustic effect—implemented by→Thermoacoustic engine with linear alternatordemonstrated
bounded by · 1
Thermoacoustic effect—bounded by→Carnot limitestablished

Matrix context

D = disequilibrium row · C = coupling family column. A cell reads the state of the atlas for that pair.

Enumerated routes through this · 64 (showing 24)

Cited sources · 5

  1. [1]
    Y. Zheng et al.. Thermoacoustic energy harvesting using thermally-stabilized polyacrylonitrile nanofibers (2022)
    Nano Energy 95, 106995 · doi:10.1016/j.nanoen.2022.106995 · record
  2. [2]
    Y. Li et al.. High-temperature energy harvesting via thermoacoustic-triboelectric hybridization: Design, modelling, and application demonstration (2026)
    Nano Energy 155, 112082 · doi:10.1016/j.nanoen.2026.112082 · record
  3. [3]
    G. W. Swift. Thermoacoustic engines (1988)
    Journal of the Acoustical Society of America 84, 1145–1180 · doi:10.1121/1.396617 · crossref ✓ 2026-09-19 · record
  4. [4]
    T. Yazaki et al.. Traveling Wave Thermoacoustic Engine in a Looped Tube (1998)
    Physical Review Letters 81, 3128–3131 · doi:10.1103/PhysRevLett.81.3128 · record
  5. [5]
    S. Backhaus, G. W. Swift. A thermoacoustic-Stirling heat engine: Detailed study (2000)
    Journal of the Acoustical Society of America 107, 3148–3166 · doi:10.1121/1.429343 · record

Cite this entity

Physical Transformation Atlas (2026). entity phenomenon:thermoacoustic-effect: Thermoacoustic effect. Dataset revision rbfbfcbb70e57 (hash of the canonical data). https://physical-transformation-atlas.wldud5192.workers.dev/phenomenon/thermoacoustic-effect

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