2013
DOI: 10.1007/s00348-013-1611-6
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Wide band Fresnel super-resolution applied to capillary breakup of viscoelastic fluids

Abstract: We report a technique based on Fresnel diffraction with white illumination that permits the resolution of capillary surface patterns of less than 100 nanometers. We investigate Rayleigh Plateaux like instability on a viscoelastic capillary bridge and show that we can overcome the resolution limit of optical microscopy. The viscoelastic filaments are approximately 20 microns thick at the end of the thinning process when the instability sets in. The wavy distortions grow exponentially in time and the pattern is … Show more

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Cited by 3 publications
(9 citation statements)
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References 15 publications
(24 reference statements)
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“…At these small concentrations the viscosity of the suspensions can be considered to remain equal to the viscosity of the suspending fluid and the change in thinning dynamics can unambiguously be attributed to the presence of single beads in the thread. High-speed imaging in combination with a "super resolution technique" [19] are used to characterize the break-up dynamics (fig. 1).…”
mentioning
confidence: 99%
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“…At these small concentrations the viscosity of the suspensions can be considered to remain equal to the viscosity of the suspending fluid and the change in thinning dynamics can unambiguously be attributed to the presence of single beads in the thread. High-speed imaging in combination with a "super resolution technique" [19] are used to characterize the break-up dynamics (fig. 1).…”
mentioning
confidence: 99%
“…Light that passes through the center of the filament is not diffracted and produces a bright line in the middle of the filament, while the light that interacts with the boundaries of the filament gets diffracted so they appear dark. In principle, the intensity profile of the diffracted light can be evaluated to achieve spatial resolutions below 100 nm [19]. The filament is filmed by a 10 bit high-speed camera (X-Stream XS-5, IDT, Tallahassee, USA) at up to 8.2 kHz frame rate depending on the spatial resolution.…”
mentioning
confidence: 99%
“…The bottom rod motion was the superposition of two harmonic oscillations: a fundamental vibration with the frequency and amplitude A determined by the power amplifier, and a subdominant oscillation of frequency ω and amplitude a. In all the cases considered, ω and aω 2 A 2 , and thus the rod vibration could be regarded as quasi-periodic within the time interval analyzed. The shaker exhibited lateral resonances for a number of frequencies within the range (900 Hz-10 kHz).…”
Section: Methodsmentioning
confidence: 99%
“…, where Z is the instantaneous vertical position of the bottom rod end in the image. This position is approximately given by the function Z(t ) − Z(0) = A sin(2π t )+a 2πω), where the last term has been introduced to take into account the effect of the low-frequency (ω ) subdominant (aω 2 A 2 ) oscillation produced by the shaker. Therefore,…”
Section: Methodsmentioning
confidence: 99%
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