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  • 1
    In: Biomaterials, Elsevier BV, Vol. 213 ( 2019-08), p. 119212-
    Type of Medium: Online Resource
    ISSN: 0142-9612
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2019
    detail.hit.zdb_id: 2004010-6
    SSG: 12
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  • 2
    In: Toxicological Sciences, Oxford University Press (OUP), Vol. 121, No. 1 ( 2011-05), p. 132-139
    Type of Medium: Online Resource
    ISSN: 1096-6080 , 1096-0929
    Language: English
    Publisher: Oxford University Press (OUP)
    Publication Date: 2011
    detail.hit.zdb_id: 1471974-5
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  • 3
    Online Resource
    Online Resource
    Elsevier BV ; 2013
    In:  International Journal of Heat and Mass Transfer Vol. 59 ( 2013-04), p. 316-327
    In: International Journal of Heat and Mass Transfer, Elsevier BV, Vol. 59 ( 2013-04), p. 316-327
    Type of Medium: Online Resource
    ISSN: 0017-9310
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2013
    detail.hit.zdb_id: 240652-4
    detail.hit.zdb_id: 2012726-1
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  • 4
    Online Resource
    Online Resource
    Elsevier BV ; 2013
    In:  International Journal of Heat and Mass Transfer Vol. 63 ( 2013-8), p. 301-312
    In: International Journal of Heat and Mass Transfer, Elsevier BV, Vol. 63 ( 2013-8), p. 301-312
    Type of Medium: Online Resource
    ISSN: 0017-9310
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2013
    detail.hit.zdb_id: 240652-4
    detail.hit.zdb_id: 2012726-1
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  • 5
    Online Resource
    Online Resource
    Cambridge University Press (CUP) ; 2021
    In:  Journal of Fluid Mechanics Vol. 918 ( 2021-07-10)
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 918 ( 2021-07-10)
    Abstract: Interaction of droplets with vortical structures is ubiquitous in nature, ranging from raindrops to a gas turbine combustor. In this work, we elucidate the mechanism of co-axial interaction of a droplet with a vortex ring of different circulation strengths ( $\varGamma = 45\text {--}161\ \textrm {cm}^2\ \textrm {s}^{-1}$ ). We focus on both the droplet and the vortex dynamics, which evolve in a spatio-temporal fashion during different stages of the interaction, as in a two-way coupled system. Vortex rings of varying circulation strengths are generated by injecting a slug of water into a quiescent water-filled chamber. Experimental techniques such as high-speed particle image velocimetry, planner laser-induced fluorescence imaging and high-speed shadowgraphy are used in this work. In the droplet dynamics, different regimes of interaction are identified, including deformation (regime-I), stretching and engulfment (regime-II) and breakup of the droplet (regime-III). Each interaction regime is explained using existing theoretical models that closely match the experimental data. In the vortex dynamics, we compare the interaction's effect on different characteristics of the vortex rings, such as pressure and the vorticity distribution, circulation strength, total energy and enstrophy variation with time. It is found that the interaction leads to a reduction in these parameters.
    Type of Medium: Online Resource
    ISSN: 0022-1120 , 1469-7645
    Language: English
    Publisher: Cambridge University Press (CUP)
    Publication Date: 2021
    detail.hit.zdb_id: 1472346-3
    detail.hit.zdb_id: 218334-1
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  • 6
    Online Resource
    Online Resource
    Cambridge University Press (CUP) ; 2019
    In:  Journal of Fluid Mechanics Vol. 866 ( 2019-05-10), p. 61-81
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 866 ( 2019-05-10), p. 61-81
    Abstract: Manipulation of an array of surface droplets organised in an ordered structure turns out to be of immense consequence in a wide variety of applications ranging from photonics, near field imaging and inkjet printing on the one hand to bio-molecular analysis and DNA sequencing on the other. While evaporation of a single isolated sessile droplet has been well studied, the collective evaporative dynamics of an ordered array of droplets on a solid substrate remains elusive. Physically, the closed region between the centre and side droplets in the ordered array reduces the mobility of the diffusing vapour, resulting in its accumulation along with enhanced local concentration and a consequent increment in the lifetime of the centre droplet. Here, we present a theoretical model to account for evaporation lifetime scaling in closely placed ordered linear droplet arrays. In addition, the present theory predicts the limiting cases of droplet interaction; namely, critical droplet separation for which interfacial interaction ceases to exist and minimum possible droplet separation (droplets on the verge of coalescence) for which the droplet system achieves maximum lifetime scaling. Further experimental evidence demonstrates the applicability of the present scaling theory to extended dimensions of the droplet array, generalising our physical conjecture. It is also worth noting that the theoretical time scale is applicable across a wide variety of drop–substrate combinations and initial droplet volumes. We also highlight that the scaling law proposed here can be extended seamlessly to other forms of confinement such as an evaporating droplet inside a mini-channel, as encountered in countless applications ranging from biomedical engineering to surface patterning.
    Type of Medium: Online Resource
    ISSN: 0022-1120 , 1469-7645
    Language: English
    Publisher: Cambridge University Press (CUP)
    Publication Date: 2019
    detail.hit.zdb_id: 1472346-3
    detail.hit.zdb_id: 218334-1
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  • 7
    Online Resource
    Online Resource
    Cambridge University Press (CUP) ; 2023
    In:  Journal of Fluid Mechanics Vol. 955 ( 2023-01-25)
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 955 ( 2023-01-25)
    Abstract: We study drop impacts on an immiscible viscous liquid pool and investigate the formation of droplet surface craters using experimental and theoretical analyses. We attribute the formation of air craters to the rapid deceleration of the droplet due to viscous drag force. The droplet response to the external impulsive decelerating force induces oscillatory modes on the surface exposed to the air forming capillary waves that superimpose to form air craters of various shapes and sizes. We introduce a non-dimensional parameter ( ${\varGamma }$ ), that is, the ratio of the drag force to the capillary force acting on the droplet. We show that ${\varGamma }$ is directly proportional to the capillary number. We show that droplets forming air craters of significant depths have ${\varGamma }〉1$ . Further, we demonstrate that Legendre polynomials can locally approximate the central air crater jet profile. We also decipher that the air crater response time scale ( $T$ ) varies as the square root of impact Weber number ( $T\sim We^{1/2}$ ). Further, we generalize the local droplet response with a global response model for low impact energies based on an eigenvalue problem. We represent the penetrating drop as a constrained Rayleigh drop problem with a dynamic contact line. The air–water interface dynamics is analysed using an inviscid droplet deformation model for small deformation amplitudes. The local and global droplet response theories conform with each other and depict that the deformation profiles could be represented as a linear superposition of eigenmodes in Legendre polynomial basis. We unearth that the droplet response in an immiscible impact system differs from the miscible impact systems due to the presence of such a dynamic contact line.
    Type of Medium: Online Resource
    ISSN: 0022-1120 , 1469-7645
    Language: English
    Publisher: Cambridge University Press (CUP)
    Publication Date: 2023
    detail.hit.zdb_id: 1472346-3
    detail.hit.zdb_id: 218334-1
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  • 8
    Online Resource
    Online Resource
    Cambridge University Press (CUP) ; 2017
    In:  Journal of Fluid Mechanics Vol. 827 ( 2017-09-25), p. 572-613
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 827 ( 2017-09-25), p. 572-613
    Abstract: This paper discusses the fundamental mechanisms of vortex–droplet interactions leading to flow distortion, droplet dispersion and breakup in a complex swirling gas flow field. In particular, the way in which the location of droplet injection determines the degree of inhomogeneous dispersion and breakup modes has been elucidated in detail using high-fidelity laser diagnostics. The droplets are injected as monodispersed streams at various spatial locations such as the vortex breakdown bubble and the shear layers (inner and outer) exhibited by the swirling flow. Simultaneous time-resolved particle image velocimetry ( $3500~\text{frames}~\text{s}^{-1}$ ) and high-speed shadowgraphy measurements are employed to delineate the two-phase interaction dynamics. These measurements have been used to evaluate the fluctuations in instantaneous circulation strength $\unicode[STIX]{x1D6E4}^{\prime }$ caused by the flow field eddies and the resultant angular dispersion in the droplet trajectories $\unicode[STIX]{x1D703}^{\prime }$ . The droplet–flow interactions show two-way coupling at low momentum ratios ( $MR$ ) and strong one-way coupling at high momentum ratios. The gas phase flow field is globally altered at low airflow rates (low $MR$ ) due to impact of droplets with the vortex core. The flow perturbation is found to be minimal and mainly local at high airflow rates (high $MR$ ). Spectral coherence analysis is carried out to understand the correlation between eddy circulation strength $\unicode[STIX]{x1D6E4}^{\prime }$ and droplet dispersion $\unicode[STIX]{x1D703}^{\prime }$ . The droplet dispersion shows strong coherence with the flow in certain frequency bands. Subsequently, proper orthogonal decomposition (POD) is implemented to elucidate the governing instability mechanism and frequency signatures associated with the turbulent coherent structures. The POD results suggest dominance of the Kelvin–Helmholtz (KH) instability mode (axial and azimuthal shear). The frequency range pertaining to high coherence between dispersion and circulation shows good agreement with KH instability quantified from POD analysis. The droplets injected at the inner shear layer (ISL) and outer shear layer (OSL) show different interaction dynamics. For instance, droplet dispersion at the OSL exhibits secondary frequency (shedding mode) coupling in addition to the KH mode, whereas ISL injection couples only in a single narrow frequency band (i.e. KH mode). Further, high-speed shadow imaging ( $7500~\text{frames}~\text{s}^{-1}$ ) is employed to visualize the breakup dynamics of the droplets. The effect of coherent structures on the droplet breakup modes is shown as a function of the Weber number ( $We$ ) defined based on the circulation strength. The wide fluctuations caused in the instantaneous circulation strength lead to different breakup modes (bag, multimodal, shear thinning, catastrophic) even for fixed airflow rates. These fluctuations also lead to inhomogeneous spatial dispersion of the droplets in the swirling gas flow field. We are able to present the dispersion contours in terms of the Stokes number and a spatial homogeneity parameter. In essence, the dispersion inhomogeneity is found to be a strong function of the injection location, the phase relationship with the eddies and the momentum ratio ( $MR$ ).
    Type of Medium: Online Resource
    ISSN: 0022-1120 , 1469-7645
    Language: English
    Publisher: Cambridge University Press (CUP)
    Publication Date: 2017
    detail.hit.zdb_id: 1472346-3
    detail.hit.zdb_id: 218334-1
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  • 9
    Online Resource
    Online Resource
    Springer Science and Business Media LLC ; 2021
    In:  Nature Vol. 597, No. 7875 ( 2021-09-09), p. 178-178
    In: Nature, Springer Science and Business Media LLC, Vol. 597, No. 7875 ( 2021-09-09), p. 178-178
    Type of Medium: Online Resource
    ISSN: 0028-0836 , 1476-4687
    RVK:
    RVK:
    RVK:
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2021
    detail.hit.zdb_id: 120714-3
    detail.hit.zdb_id: 1413423-8
    SSG: 11
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  • 10
    Online Resource
    Online Resource
    Royal Society of Chemistry (RSC) ; 2017
    In:  Physical Chemistry Chemical Physics Vol. 19, No. 36 ( 2017), p. 24961-24970
    In: Physical Chemistry Chemical Physics, Royal Society of Chemistry (RSC), Vol. 19, No. 36 ( 2017), p. 24961-24970
    Type of Medium: Online Resource
    ISSN: 1463-9076 , 1463-9084
    Language: English
    Publisher: Royal Society of Chemistry (RSC)
    Publication Date: 2017
    detail.hit.zdb_id: 1476283-3
    detail.hit.zdb_id: 1476244-4
    detail.hit.zdb_id: 1460656-2
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