- Page 1 and 2: Drop Impact on Dry Surfaces with Ph
- Page 3 and 4: Hiermit versichere ich, die vorlieg
- Page 5: Fachgebiet Reaktive Strömungslehre
- Page 9 and 10: Splash, einseitiger Splash sowie de
- Page 11 and 12: 3.4.2. Calibration of the Infrared
- Page 14 and 15: Nomenclature Latin capitals Unit A
- Page 16 and 17: k angular wavenumber rad m −1 k R
- Page 18 and 19: F G ge i K L lam m max min n opt r
- Page 20 and 21: 1 Introduction 1.1 Motivation Aircr
- Page 22 and 23: of the WCE acquired experimentally
- Page 24: passage was cooled down to −196
- Page 27 and 28: SLD icing conditions have been defi
- Page 29 and 30: −9 ◦ C and layers of freezing r
- Page 31 and 32: adjacent downstream control volume,
- Page 33 and 34: conventional methods. Papadakis et
- Page 35 and 36: Figure 2.5.: Ice horn and clear ice
- Page 37 and 38: This model showed good agreement un
- Page 39 and 40: Xu et al. proposed the following sc
- Page 41 and 42: Figure 2.9.: Splash thresholds of t
- Page 43 and 44: Chen and Wang [28] observed the dro
- Page 45 and 46: 2.14 shows. On stainless steel, tin
- Page 47 and 48: years ago [157]. Another peculiarit
- Page 49 and 50: Figure 2.17.: At an ambient pressur
- Page 51 and 52: The temperature needs to be found o
- Page 53 and 54: The Stefan number St S completely c
- Page 55 and 56: T(x, 0) = T A < T m , 0 < x < ∞ b
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Figure 2.20: Fraction of solidifica
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The mathematical description of the
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asal plane. Without all these facto
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Part I. Impact of Supercooled Water
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3 Experimental Setup This chapter i
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drop and the tube as between such t
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of nucleation ice dendrite growth,
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The boundary condition is then 1
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0.021 W m −1 K −1 at −165 ◦
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outlet of the liquid. There are two
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The maximum depth of water in the c
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Figure 3.11.: Pneumatic drop genera
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Figure 3.13.: Pneumatic drop genera
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Adjusting the Pulse Width Longer el
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(a) Shadowgraph imaging (b) The sid
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Figure 3.21.: The cold plate was co
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Figure 3.25.: The transmittance of
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eproducible. The SHS was created by
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Figure 3.30.: Planck’s law The ot
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Figure 3.32.: Heterogeneity of the
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Figure 3.35.: The valid region afte
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Divided by dΩ, Eq. 3.33 is related
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Figure 3.39.: The wavelength depend
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Figure 3.41.: Orientation dependenc
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wavelength, so that the value for r
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Temperature Gradient In light of th
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(a) 0.00 ms (b) 1.39 ms (c) 2.79 ms
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Figure 3.48.: Synchronization syste
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Figure 3.50.: Experimental setup fo
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(a) 0 ms (b) 0 ms (c) 0.6 ms (d) 0.
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Figure 4.2.: The dynamic spreading
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Figure 4.4.: Influence envelope of
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(a) 0 ms (b) 0.4 ms (c) 0.8 ms (d)
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(a) 0 ms (b) 1.39 ms (c) 2.79 ms (d
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(a) 0 ms (b) 0.05 ms (c) 0.1 ms (d)
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(a) −4 ◦ C, at 6.8 ms. (b) −1
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The contact temperature is closer t
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Obviously, the contact temperature
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Figure 4.13.: The dimensionless min
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always after the receding reached t
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Part II reports the experimental in
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to realize a high-speed rotation of
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Figure 5.2.: Impact surface with di
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Various such devices were developed
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than the values reported in literat
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Figure 5.7.: The monodisperse drop
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This performance is a reminiscence
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Figure 5.11.: The merging distance
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signal and the excitation signal of
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The analogy with a capacitor led to
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The real situation in the applicati
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Figure 5.15.: Static electric field
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Figure 5.19.: Phase shift and pulse
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disadvantage is that the number of
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Zoom Lens Working Distance Spatial
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the impact surface was not a sharp
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5.5 Synchronization Both single pul
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The last note on these two pulse tr
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Figure 5.28.: Calculation of the im
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6 Results and Discussion This chapt
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(a) 0 µs (b) 2 µs (c) 4 µs (d) 6
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high impact velocities approaching
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(a) 32 µs (b) 84 µs (c) 100 µs F
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(a) (b) (c) Figure 6.8.: Examinatio
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Our observations show that the lame
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6.3 Velocity of the Uprising Jet In
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(a) 1 µs (b) 3 µs (c) 4 µs Figur
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(a) 0 µs (b) 8 µs (c) 32 µs Figu
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(a) 45° target (b) 75° target (c)
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Nevertheless, the drop volume was e
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was surface tension. These factors
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the motion of the impinging water,
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of the single-side splash, the latt
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(a) 0 µs (b) 2 µs (c) 4 µs (d) 6
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(a) 0 µs (b) 1 µs (c) 2 µs (d) 3
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(a) 0 µs (b) 3 µs (c) 6 µs (d) 9
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(a) 0 µs (b) 10 µs (c) 11 µs (d)
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(a) 0 µs (b) 3 µs (c) 5 µs (d) 8
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(a) 0 µs (b) 1 µs (c) 2 µs (d) 3
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(a) 0 µs (b) 6 µs (c) 10 µs (d)
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(a) 0 µs (b) 1 µs (c) 3 µs (d) 5
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(a) 0 µs (b) 8 µs (c) 24 µs (d)
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(a) 0 µs (b) 2 µs (c) 5 µs (d) 8
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(a) 0 µs (b) 16 µs (c) 32 µs (d)
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(a) 0 µs (b) 8 µs (c) 20 µs (d)
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A.7 5° target (a) 0 µs (b) 24 µs
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(a) 0 µs (b) 20 µs (c) 36 µs (d)
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(a) 0 µs (b) 8 µs (c) 16 µs (d)
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(a) 0 µs (b) 24 µs (c) 52 µs (d)
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(a) 0 µs (b) 16 µs (c) 32 µs (d)
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(a) 0 µs (b) 20 µs (c) 40 µs (d)
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(a) 0 µs (b) 10 µs (c) 22 µs (d)
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(a) 0 µs (b) 36 µs (c) 68 µs (d)
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(a) 0 µs (b) 36 µs (c) 72 µs (d)
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(a) 0 µs (b) 8 µs (c) 16 µs (d)
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(a) (b) (c) (d) (e) (f) Figure B.4.
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(a) 0 ms (b) 0.4 ms (c) 0.5 ms (d)
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(a) 0 ms (b) 0.35 ms (c) 1 ms (d) 1
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2.15.Prompt splash (left) was docum
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3.12.Time t =0 corresponds to the s
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3.31.The extension ring (left) betw
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4.7. Infrared imaging: total reboun
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5.5. The custom made vibrating orif
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5.14.Static electric field between
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6.6. Capillary wave created by the
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A.5. Drop diameter: 189 µm, impact
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A.29.Drop diameter: 203 µm, impact
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List of Tables 2.1. MVD of Freezing
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Imaging and Computer Simulations. T
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[42] GENT, R. W., N. P. DART and J.
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[70] KOROLEV, ALEXEI V., GEORGE A.
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[99] MUNDO, CHR., M. SOMMERFELD and
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[125] RYERSON, CHARLES C., GEORGE G
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[153] ŠIKALO Š., C. TROPEA and E.
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Curriculum Vitae Personal Informati