Oscillations, Waves, and Interactions - GWDG

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Thomas Kurz, Ulrich Parlitz, and Udo Kaatze (Eds.) Oscillations, Waves, and Interactions Except where otherwise noted, this work is licensed under a Creative Commons License
Page 1: Thomas Kurz, Ulrich Parlitz, and Ud
Page 5 and 6: Thomas Kurz, Ulrich Parlitz, Udo Ka
Page 7 and 8: Contents Preface . . . . . . . . .
Page 9: Preface This year we celebrate the
Page 12 and 13: 2 M. R. Schroeder, D. Guicking and
Page 36 and 37: 26 H. W. Strube 3 Acoustic analysis
Page 38 and 39: 28 H. W. Strube that overlap at mos
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Page 42 and 43: 32 H. W. Strube 3.5.1 Glottis pulse
Page 44 and 45: 34 H. W. Strube the expectations: t
Page 46 and 47: 36 H. W. Strube (1985). [30] M. Fr
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42 A. Kohlrausch and S. van de Par
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Oscillations, Waves and Interaction
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Sound absorption, sound amplificati
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(pressure drop) / (dynamic pressure
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Active control of sound and vibrati
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primary sound reference microphone
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01 01 01 01 01 engine synchronisati
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amplitude Active control of sound a
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3.8 Control of nonlinear dynamical
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number of publications per 5 years
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pressure, and The single bubble - a
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2.3 Response curves The single bubb
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The single bubble - a hot microlabo
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Normalized Energy 0.5 0.4 0.3 0.2 0
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seeding phase [deg] 0 50 100 150 20
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(a) (b) The single bubble - a hot m
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Acoustic cavitation 173 strated in
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(a) 1 mm (b) Acoustic cavitation 17
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(Rmax - R0) / R0 30 25 20 15 10 5 0
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Acoustic cavitation 179 λ =1 λ=10
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Acoustic cavitation 181 Figure 8. C
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Acoustic cavitation 183 up to some
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Acoustic cavitation 185 A convenien
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Acoustic cavitation 187 of the forc
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p a [kPa] 200 150 100 50 0 SI BJ RD
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Acoustic cavitation 191 the bubble
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Acoustic cavitation 193 (a) (b) (c)
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Acoustic cavitation 195 structures
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Acoustic cavitation 197 [30] D. F.
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Wide-focus low-pressure ESWL 201 Fi
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Wide-focus low-pressure ESWL 211 5
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Wide-focus low-pressure ESWL 213 lo
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Wide-focus low-pressure ESWL 215 [9
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Dynamics of pulsed laser tissue abl
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volumetric energy density ε(r) by:
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Laser speckle metrology 261 of roug
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Laser speckle metrology 263 Figure
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Laser speckle metrology 265 We have
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Laser speckle metrology 269 saw too
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6 Sounding the depth by vibration E
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Laser speckle metrology 275 that al
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A B Large ring laser gyroscopes 281
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Large ring laser gyroscopes 283 Fig
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Large ring laser gyroscopes 285 Rin
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el. Allan Deviation 10 -4 10 -5 10
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Split-mode Sagnac [Hz] 282.800 282.
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4 1 5 4 3 1 1 2 cam 1 Large ring la
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Variation in Area [*1e6] 3.0 2.0 1.
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∆f [mHz] 5 0 -5 -10 -15 -20 Large
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∆f [mHz] 6.0 4.0 2.0 0.0 -2.0 -4.
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Δf [µHz] 100 50 0 -50 Large ring
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ot. rate [nrad/s] 600 400 200 0 -20
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Sagnac frequency [Hz] 348.80 348.70
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Large ring laser gyroscopes 305 loc
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Large ring laser gyroscopes 307 ing
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Large ring laser gyroscopes 309 Ack
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Charge order in one-dimensional sol
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Temperature (K) (TMTTF) 2 SbF 6 100
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Reflectivity (%) Conductivity (10 5
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10 6 / ε 30 20 10 0 Charge order i
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Dielectric constant ε 400 300 200
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Multistep association of cations an
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References Multistep association of
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Liquids: Formation of complexes and
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Figure 1. Resonance curves of the d
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Complex dynamics of nonlinear syste
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2.3 Hybrid systems Complex dynamics
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3 Characterising complex dynamics C
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attractor in the unknown state spac
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(a) U(∆ Φ) Complex dynamics of n
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Figure 15. Mean rotation frequencie
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6 Chaos Control Complex dynamics of
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1.3 Optical trapping DPI60plus - a
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DPI60plus - a future with biophysic
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Index ablation, 217, 223 dynamics,
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pinch-off, 174 radius, critical, 23
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diurnal polar motion, 296-299 DNA,
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identical synchronisation, 425, 426
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control, 107, 108 freefield, 118 sy
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pressure, 234, 236, 238, 239 stress
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structural control, 124 vibration,
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A broad variety of research topics
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