Oscillations, Waves, and Interactions - GWDG

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460 S. Lakämper and C. F. Schmidt dimensional tracking of ncd motility by back focal plane interferometry’, Biophys. J. 74, 1074 (1998). [18] L. C. Kapitein, E. J. Peterman, B. H. Kwok, J. H. Kim, T. M. Kapoor, and C. F. Schmidt, ‘The bipolar mitotic kinesin Eg5 moves on both microtubules that it crosslinks’, Nature 435, 114 (2005). [19] B. J. Alder and T. E. Wainwright, ‘Velocity autocorrelations for hard spheres’, Phys. Rev. Lett. 18, 988 (1967). [20] M. Buchanan, M. Atakhorrami, J. F. Palierne, F. C. MacKintosh, and C. F. Schmidt, ‘High-frequency microrheology of wormlike micelles’, Phys. Rev. E 72, 011504 (2005). [21] M. Buchanan, M. Atakhorrami, J. F. Palierne, and C. F. Schmidt, ‘Comparing macrorheology and one- and two-point microrheology in wormlike micelle solutions’, Macromolecules 38, 8840 (2005). [22] G. H. Koenderink, M. Atakhorrami, F. C. MacKintosh, and C. F. Schmidt, ‘Highfrequency stress relaxation in semiflexible polymer solutions and networks’, Phys. Rev. Lett. 96, 138307 (2006). [23] D. Mizuno, C. Tardin, C. F. Schmidt, and F. C. MacKintosh, ‘Nonequilibrium mechanics of active cytoskeletal networks’, Science 315, 370 (2007). [24] S. Jabbari-Farouji, D. Mizuno, M. Atakhorrami, F. C. MacKintosh, C. F. Schmidt, E. Eiser, G. H. Wegdam, and D. Bonn, ‘Fluctuation-dissipation theorem in an aging colloidal glass’, Phys. Rev. Lett. 98, 108302 (2007).
Index ablation, 217, 223 dynamics, 222, 236, 243 efficiency, 231, 236, 245, 248, 250, 251 explosive, 244 microsecond, 242, 245 model, 250 nanosecond, 237, 244 photochemical, 225 photothermal, 225 plume, 236 dynamics, 238, 240 shielding, 249, 251 recoil pressure, 234, 236, 238, 239 threshold, 228, 236, 237, 244–246, 249– 251 absorber active, 111, 115, 117 matched, 109 absorption coefficient, ultrasonic, 341 optical, 222 spectra, ultrasonic, 333 acoustic cavitation, 139, 171, 184, 191, 194, 195 feedback, 110 force on bubble, 171, 183, 194 quadripole, 113 stimuli, 37, 41 transfer function, 110 tripole, 109 acoustical spectrometry, 368 actin, 457, 458 filament, 445, 453, 455–457 network, 455, 457 active absorber, 111, 115, 117 flow control, 107, 125 headset, 115 hydromount, 122 impedance control, 117 muffler, 114, 118 noise control, 107, 108 freefield, 118 optics, 123 sound control, 107 structural control, 124 vibration control, 107, 119 isolation, 121 adaptive digital filter, 110 feedforward control, 111 noise cancelling, 112 optics, 107, 123 windowing (ESPI), 268 added mass, 173, 187 Adler’s equation, 423 afterbounce, 147 amphiphiles, 368 ANC – see: active noise control anisotropic crystal, 314 anti-sound, 108 antiphase signal, 107, 108, 113, 114 aqueous solution, 333 Arnol’d tongue, 423 artificial cell, 435, 438 artwork deterioration, 261 monitoring, 260, 264 aspherical bubble collapse, 149, 150, 152, 153, 156, 157 association multistep, 333, 334, 360 scheme of Eigen-Tamm, 343, 344 atomic force microscopy, 435, 440, 441, 444 attenuation spectra, 374 spectrometry, 371 attractor, 143, 408, 417 chaotic, 409, 411, 418, 427 coexisting, 144, 408, 412 periodic, 409 audiology, 67 auditory filter, 38, 40, 43 amplitude characteristic, 44 gamma-tone, 44 phase characteristic, 41 autocorrelation, 46, 47 automaton, 406, 415 autoregression frequency analysis, 302 backscattering, 288 basilar membrane, 41, 43, 45, 64
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Thomas Kurz, Ulrich Parlitz, and Ud
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erschienen im Universitätsverlag G
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Bibliographische Information der De
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iv Contents Laser speckle metrology
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Oscillations, Waves and Interaction
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Applied physics at the “Dritte”
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noise component [GNE] 5 4 3 2 1 can
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3.4 Transfer to running speech Spee
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3.4.2 Analysis of running speech Sp
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Speech research 33 Area [Pixels] 60
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Speech research 35 [13] D. Michaeli
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Specific signal types in hearing re
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74 D. Ronneberger et al. Mechel fou
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76 D. Ronneberger et al. (flow velo
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78 D. Ronneberger et al. |t + acous
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80 D. Ronneberger et al. Figure 6.
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82 D. Ronneberger et al. Figure 8.
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84 D. Ronneberger et al. (flow velo
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86 D. Ronneberger et al. R / L ⋅
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88 D. Ronneberger et al. e. g. temp
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90 D. Ronneberger et al. 3.2 Qualit
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92 D. Ronneberger et al. As usual t
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94 D. Ronneberger et al. (wavenumbe
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96 D. Ronneberger et al. powers of
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98 D. Ronneberger et al. an increas
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100 D. Ronneberger et al. The term
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102 D. Ronneberger et al. Neverthel
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104 D. Ronneberger et al. [4] J. Br
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106 D. Ronneberger et al. strömung
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108 D. Guicking synchronised tuning
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110 D. Guicking primary noise micro
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112 D. Guicking primary sensor desi
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114 D. Guicking by an antiphase sou
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116 D. Guicking R L C C + + 1 1−C
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118 D. Guicking More involved than
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120 D. Guicking In the 1980s, longi
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122 D. Guicking with electrodynamic
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124 D. Guicking 3.6 Noise reduction
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126 D. Guicking the turbulence of a
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128 D. Guicking References [1] Lord
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130 D. Guicking [44] Falcke, H.,
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132 D. Guicking [84] J. Melcher,
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134 D. Guicking [125] D. Heyland et
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136 D. Guicking [166] S. Zommer et
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138 D. Guicking [212] M. L. Post an
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140 W. Lauterborn et al. liquid κ
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142 W. Lauterborn et al. Figure 2.
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144 W. Lauterborn et al. nator, and
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146 W. Lauterborn et al. by types a
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148 W. Lauterborn et al. bubble rad
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154 W. Lauterborn et al. P koll [kb
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156 W. Lauterborn et al. Pulse widt
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158 W. Lauterborn et al. laser puls
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168 W. Lauterborn et al. R [µ m] 1
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170 W. Lauterborn et al. [17] M. P.
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172 R. Mettin (a) (b) Figure 1. Bub
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174 R. Mettin 0 ms 2 mm 1 ms 2 ms 3
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176 R. Mettin important quantity ch
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178 R. Mettin 100 kPa 200 kPa | | F
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180 R. Mettin Figure 7. Trapped sin
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182 R. Mettin concentration of spec
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184 R. Mettin which is called the p
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186 R. Mettin R 02 [µm] R 02 [µm]
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188 R. Mettin constant to M a = 2π
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190 R. Mettin (a) p a [Pa] 140 120
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192 R. Mettin z [mm] 5 4 3 2 1 0 -1
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194 R. Mettin Figure 17. Left: Expe
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196 R. Mettin - a hot microlaborato
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198 R. Mettin [52] R. Mettin, C.-D.
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200 W. Eisenmenger and U. Kaatze Th
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202 W. Eisenmenger and U. Kaatze Fi
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214 W. Eisenmenger and U. Kaatze 6
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216 W. Eisenmenger and U. Kaatze Pr
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218 A. Vogel, I. Apitz, V. Venugopa
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260 K. D. Hinsch Generally, any of
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262 K. D. Hinsch Figure 1. Monitori
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264 K. D. Hinsch Figure 3. ESPI stu
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266 K. D. Hinsch Figure 4. Deterior
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268 K. D. Hinsch Often, in-plane mo
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270 K. D. Hinsch Figure 7. Optical
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272 K. D. Hinsch Figure 9. Humidity
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274 K. D. Hinsch locations that tak
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276 K. D. Hinsch Figure 13. Map of
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278 K. D. Hinsch References [1] D.
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280 Schreiber not moving along with
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282 Schreiber These properties made
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284 Schreiber Figure 3. The G ring
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286 Schreiber Rotation Rate [rad/s]
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288 Schreiber and it is currently b
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290 Schreiber n1 D A B n Figure 8.
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292 Schreiber Beamwalk [µm] 80.0 7
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294 Schreiber ∆ Perimeter [*10e12
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296 Schreiber and the last term acc
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298 Schreiber Δf [µHz] 100 50 0 -
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300 Schreiber formation of a new wo
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302 Schreiber PSD [*10 16 (rad/s) 2
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304 Schreiber 7.2 The ring laser co
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306 Schreiber Demodulator Signal [V
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308 Schreiber Est. Phase Vel. (m/s)
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310 Schreiber [18] V. Frede and V.
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312 Martin Dressel tice is reduced
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314 Martin Dressel Metallic whisker
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316 Martin Dressel (a) (b) (c) CH 3
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318 Martin Dressel 3.1 Charge densi
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320 Martin Dressel Absorptivity σ
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322 Martin Dressel brought a confir
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324 Martin Dressel a charge disprop
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326 Martin Dressel Conductivity 70
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328 Martin Dressel Reflectivity Con
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330 Martin Dressel References [1] M
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332 Martin Dressel and L. Montgomer
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334 R. Pottel, J. Haller and U. Kaa
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368 U. Kaatze and R. Behrends with
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370 U. Kaatze and R. Behrends Figur
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386 U. Kaatze and R. Behrends of th
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398 U. Kaatze and R. Behrends [6] M
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400 U. Kaatze and R. Behrends [49]
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402 U. Kaatze and R. Behrends (2002
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404 U. Kaatze and R. Behrends Copyr
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406 U. Parlitz here chaos control m
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408 U. Parlitz Figure 2. Amplitude
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Page 472 and 473: 462 Index basin of attraction, 144
Page 474 and 475: 464 Index cone bubble structure, 19
Page 476 and 477: 466 Index turbulent, 111, 126 fluct
Page 478 and 479: 468 Index LPC, 29 luminescence of b
Page 480 and 481: 470 Index peak factor, 38, 43 Peier
Page 482 and 483: 472 Index laser-induced bubble, 152
Page 484 and 485: 474 Index ultraharmonic resonance,
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