-
1
-
-
84967805396
-
Thermoacoustic engines
-
G. W. Swift, "Thermoacoustic engines," J. Acoust. Soc. Am. 84, 1145-1180 (1988).
-
(1988)
J. Acoust. Soc. Am.
, vol.84
, pp. 1145-1180
-
-
Swift, G.W.1
-
2
-
-
0029342239
-
Thermoacoustic engines and refrigerators
-
July
-
G. W. Swift, "Thermoacoustic engines and refrigerators," Phys. Today 48, 22-28 (July 1995).
-
(1995)
Phys. Today
, vol.48
, pp. 22-28
-
-
Swift, G.W.1
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3
-
-
33744555120
-
-
note
-
The stack is similar to a regenerator in that it acts as a thermal reservoir which can interact with the gas. The essential difference between the two lies in the degree to which the gas is coupled to the reservoir. In a stack, the gas is in imperfect thermal contact with the solid whereas in a regenerator the typical pore dimension is much smaller and the coupling between gas and solid is consequently much stronger.
-
-
-
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4
-
-
1842388162
-
Concepts for thermoacoustic refrigeration and a practical device
-
Monterey CA Wright-Patterson AFB, Wright-Patterson, OH
-
T. J. Hofler, Concepts for thermoacoustic refrigeration and a practical device, Proceedings of the 5th International Cryocoolers Conference, Monterey CA (Wright-Patterson AFB, Wright-Patterson, OH, 1998), pp. 93-101; T. J. Hofler, "Thermoacoustic refrigerator design and performance," Ph.D. thesis, Univ. of California, San Diego, 1986.
-
(1998)
Proceedings of the 5th International Cryocoolers Conference
, pp. 93-101
-
-
Hofler, T.J.1
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5
-
-
0003753524
-
-
Ph.D. thesis, Univ. of California, San Diego
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T. J. Hofler, Concepts for thermoacoustic refrigeration and a practical device, Proceedings of the 5th International Cryocoolers Conference, Monterey CA (Wright-Patterson AFB, Wright-Patterson, OH, 1998), pp. 93-101; T. J. Hofler, "Thermoacoustic refrigerator design and performance," Ph.D. thesis, Univ. of California, San Diego, 1986.
-
(1986)
Thermoacoustic Refrigerator Design and Performance
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-
Hofler, T.J.1
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6
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0026649464
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Analysis and performance of a large thermoacoustic engine
-
G. W. Swift, "Analysis and performance of a large thermoacoustic engine," J. Acoust. Soc. Am. 92, 1551-1563 (1992).
-
(1992)
J. Acoust. Soc. Am.
, vol.92
, pp. 1551-1563
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Swift, G.W.1
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7
-
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0027227409
-
Thermoacoustics in pin-array stacks
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G. W. Swift and R. M. Keolian, "Thermoacoustics in pin-array stacks," J. Acoust. Soc. Am. 94, 941-943 (1993).
-
(1993)
J. Acoust. Soc. Am.
, vol.94
, pp. 941-943
-
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Swift, G.W.1
Keolian, R.M.2
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8
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33744602679
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"Thermoacoustic device," U.S. Patent number 4,625,517 (1986)
-
U. A. Müller, "Thermoacoustic device," U.S. Patent number 4,625,517 (1986).
-
-
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Müller, U.A.1
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9
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33744629343
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note
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κ away from the solid while viscous shear is most intense at the gas-solid interface.
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-
-
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10
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0043190764
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Measurements of a thermoacoustic pin stack
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R. J. Gibson, F. S. Nessler, and R. M. Keolian, "Measurements of a thermoacoustic pin stack (abstract)," J. Acoust. Soc. Am. 100, 2845 (1996); "A thermoacoustic pin stack for improved efficiency," to be published in the proceedings of the National Heat Transfer Conference, Baltimore MD, August 1997.
-
(1996)
J. Acoust. Soc. Am.
, vol.100
, pp. 2845
-
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Gibson, R.J.1
Nessler, F.S.2
Keolian, R.M.3
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11
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33744563100
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to be published in the proceedings of the National Heat Transfer Conference, Baltimore MD, August
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R. J. Gibson, F. S. Nessler, and R. M. Keolian, "Measurements of a thermoacoustic pin stack (abstract)," J. Acoust. Soc. Am. 100, 2845 (1996); "A thermoacoustic pin stack for improved efficiency," to be published in the proceedings of the National Heat Transfer Conference, Baltimore MD, August 1997.
-
(1997)
A Thermoacoustic Pin Stack for Improved Efficiency
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-
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12
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84938896531
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Ueber den Einfluss der Wärmeleitung in einem Gase auf die Schallbewegung
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G. Kirchhoff, "Ueber den Einfluss der Wärmeleitung in einem Gase auf die Schallbewegung," Ann. Phys. Chem. 134, 177-193 (1868).
-
(1868)
Ann. Phys. Chem.
, vol.134
, pp. 177-193
-
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Kirchhoff, G.1
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13
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0000659738
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Thermally driven acoustic oscillations. Part IV. Tubes with variable cross section
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N. Rott and G. Zouzoulas, "Thermally driven acoustic oscillations. Part IV. Tubes with variable cross section," Z. Angew. Math. Phys. 27, 197-224 (1976).
-
(1976)
Z. Angew. Math. Phys.
, vol.27
, pp. 197-224
-
-
Rott, N.1
Zouzoulas, G.2
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14
-
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0026349473
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General formulation of thermoacoustics for stacks having arbitrarily shaped pore cross sections
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W. Pat Arnott, Henry Bass, and Richard Raspet, "General formulation of thermoacoustics for stacks having arbitrarily shaped pore cross sections," J. Acoust. Soc. Am. 90, 3228-3237 (1991).
-
(1991)
J. Acoust. Soc. Am.
, vol.90
, pp. 3228-3237
-
-
Arnott, W.P.1
Bass, H.2
Raspet, R.3
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15
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0017007693
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Eine Modelltheorie zum Faserabsorber Teil I: Reguläre Faserordnung
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F. Mechel, "Eine Modelltheorie zum Faserabsorber Teil I: Reguläre Faserordnung," Acustica 36, 53-64 (1976/77).
-
(1976)
Acustica
, vol.36
, pp. 53-64
-
-
Mechel, F.1
-
16
-
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0017013427
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Eine Modelltheorie zum Faserabsorber Teil II: Absorbermodell aus Elementarzellen und numerische Ergebnisse
-
F. Mechel, "Eine Modelltheorie zum Faserabsorber Teil II: Absorbermodell aus Elementarzellen und numerische Ergebnisse," Acustica 36, 65-89 (1976/77).
-
(1976)
Acustica
, vol.36
, pp. 65-89
-
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Mechel, F.1
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17
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0028392429
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Similitude in thermoacoustics
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J. R. Olson and G. W. Swift, "Similitude in thermoacoustics," J. Acoust. Soc. Am. 95, 1405-1412 (1994).
-
(1994)
J. Acoust. Soc. Am.
, vol.95
, pp. 1405-1412
-
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Olson, J.R.1
Swift, G.W.2
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18
-
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0000229137
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Damped and thermally driven acoustic oscillations in wide and narrow tubes
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N. Rott, "Damped and thermally driven acoustic oscillations in wide and narrow tubes," Z. Angew. Math. Phys. 20, 230-243 (1969).
-
(1969)
Z. Angew. Math. Phys.
, vol.20
, pp. 230-243
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Rott, N.1
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19
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0031055611
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Experimental measurements of scaling properties for acoustic propagation in a single pore
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L. A. Wilen, "Experimental measurements of scaling properties for acoustic propagation in a single pore," J. Acoust. Soc. Am. 101, 1388-1397 (1997); L. A. Wilen, "Measurements of thermoacoustic functions for single pores," submitted to S. Acoust. Soc. Am.
-
(1997)
J. Acoust. Soc. Am.
, vol.101
, pp. 1388-1397
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Wilen, L.A.1
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20
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0031891972
-
Measurements of thermoacoustic functions for single pores
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submitted to
-
L. A. Wilen, "Experimental measurements of scaling properties for acoustic propagation in a single pore," J. Acoust. Soc. Am. 101, 1388-1397 (1997); L. A. Wilen, "Measurements of thermoacoustic functions for single pores," submitted to S. Acoust. Soc. Am.
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S. Acoust. Soc. Am.
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Wilen, L.A.1
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21
-
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0025861905
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Measurement and calculation of acoustic propagation constants in arrays of small air-filled rectangular tubes
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H. S. Roh, W. P. Arnott, J. M. Sabatier, and R. Raspet, "Measurement and calculation of acoustic propagation constants in arrays of small air-filled rectangular tubes," J. Acoust. Soc. Am. 89, 2617-2624 (1991).
-
(1991)
J. Acoust. Soc. Am.
, vol.89
, pp. 2617-2624
-
-
Roh, H.S.1
Arnott, W.P.2
Sabatier, J.M.3
Raspet, R.4
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22
-
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0026753365
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Propagation of sound and the assignment of shape factors in model porous materials having simple pore geometries
-
M. R. Stinson and Y. Champoux, "Propagation of sound and the assignment of shape factors in model porous materials having simple pore geometries," J. Acoust. Soc. Am. 91, 685-695 (1992).
-
(1992)
J. Acoust. Soc. Am.
, vol.91
, pp. 685-695
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-
Stinson, M.R.1
Champoux, Y.2
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23
-
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0026085163
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Measurement of the characteristic impedance and propagation constant of materials having high flow resistivity
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Y. Champoux and M. R. Stinson, "Measurement of the characteristic impedance and propagation constant of materials having high flow resistivity," J. Acoust. Soc. Am. 90, 2182-2191 (1991).
-
(1991)
J. Acoust. Soc. Am.
, vol.90
, pp. 2182-2191
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-
Champoux, Y.1
Stinson, M.R.2
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24
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33744566356
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APS Dynamics (Carlsbad, CA 92000) model 400S
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APS Dynamics (Carlsbad, CA 92000) model 400S.
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-
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25
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33744686444
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-5 Torr at 20°C
-
-5 Torr at 20°C.
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-
-
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26
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33744651257
-
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Lucas Control Systems Products (Hampton, VA 23666) model M12-50
-
Lucas Control Systems Products (Hampton, VA 23666) model M12-50.
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-
-
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27
-
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33744628100
-
-
Lucas Control Systems Products (Hampton, VA 23666) model ATA-101: internal filters were modified to a 3-pole Bessel configuration with a corner frequency of 1 kHz.
-
Lucas Control Systems Products (Hampton, VA 23666) model ATA-101: internal filters were modified to a 3-pole Bessel configuration with a corner frequency of 1 kHz.
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-
-
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28
-
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33744568039
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Endevco Corp. (San Juan Capistrano, CA 92675) model 8510B-5
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Endevco Corp. (San Juan Capistrano, CA 92675) model 8510B-5.
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-
-
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29
-
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33744696484
-
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MKS Instruments, Inc. (Andover, MA 01810) model 390HA-1000 Baratron gauge
-
MKS Instruments, Inc. (Andover, MA 01810) model 390HA-1000 Baratron gauge.
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-
-
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30
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33744590265
-
-
note
-
The calibration of each piezo-resistive transducer was likewise checked against the manometer.
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31
-
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33744675243
-
-
note
-
The cumulative uncertainty in the absolute distance between any pair of holes in both the top plate and the support plates was maintained at the same level.
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-
-
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32
-
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33744625470
-
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Argueso, M., & Co., Inc. (Mamaroneck, NY 10543) type Rigidax WS
-
Argueso, M., & Co., Inc. (Mamaroneck, NY 10543) type Rigidax WS.
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-
-
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33
-
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33744685278
-
-
note
-
-3≪1.
-
-
-
-
34
-
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33744562429
-
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EG&G Instruments Corp. (Princeton, NJ 08543) model PAR 124A
-
EG&G Instruments Corp. (Princeton, NJ 08543) model PAR 124A.
-
-
-
-
35
-
-
33744570530
-
-
note
-
The magnitude of this quantity is of order unity.
-
-
-
-
36
-
-
33744640761
-
-
note
-
The nomenclature used to describe these carefully contrived pin arrangements is intended to distinguish them from the abstract "empty" and "full" configurations of Sec. I, and yet give some indication of the implied analogies.
-
-
-
-
37
-
-
33744714291
-
-
note
-
0 and the total surface area of the support plates is much less than that of the pins.
-
-
-
-
38
-
-
33744596566
-
-
note
-
κ of order the inter-pin spacing, is only a few percent in the present experiment.
-
-
-
-
39
-
-
33744619809
-
-
note
-
tot=1147 pins intersect the support plates in the foreground configuration. Equation (13) is specific to the case of two support plates.
-
-
-
-
40
-
-
33744662935
-
-
note
-
The hydraulic radius is the ratio of the cross-sectional area of the gas to the perimeter of the solid. The data have been plotted in this fashion for ease of comparison between stack geometries.
-
-
-
-
41
-
-
33744693121
-
-
note
-
κ in that it is the characteristic length scale for the diffusion of momentum at the acoustic frequency.
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