Bouncing-to-merging transitions of droplet impact on heated liquid film
ORAL
Abstract
Droplet impact on a liquid film is ubiquitous in numerous natural
and industrial processes. In many of these applications, the impacting
droplet and the impacted film contain liquids at different temperatures.
In this talk, we will discuss the findings from our study on droplet (radius,
R) impact on a heated liquid film of varied thickness (H). Using n-
tetradecane as our test liquid, we conducted a series of experiments where
the temperature difference (ΔT ) between the liquid film and the droplet
was varied from 0 to 60°C. The primary focus of this work is to identify
changes in the transition between bouncing to merging outcomes as the
film temperature increases. We will first compare the regime diagrams
where bouncing and merging outcomes were mapped in a Weber number
and normalized film thickness (H* = H/R) space for various ΔT . The
regime maps show that, for deep pool (H* >> 1) and shallow pool (H∗ ≈
1) limits, ΔT exhibits varied degrees of influence on the bouncing and
merging transitions. Large ΔT , however, renders merging easier across
all H* and beyond a critical temperature difference (ΔT ≥ 60°C for n-
tetradecane) the bouncing regime essentially disappears. Subsequently, to
explain the observed dynamics, we will discuss the role of evaporation and
vapor layer adjacent to the heated liquid film on the interfacial merging.
and industrial processes. In many of these applications, the impacting
droplet and the impacted film contain liquids at different temperatures.
In this talk, we will discuss the findings from our study on droplet (radius,
R) impact on a heated liquid film of varied thickness (H). Using n-
tetradecane as our test liquid, we conducted a series of experiments where
the temperature difference (ΔT ) between the liquid film and the droplet
was varied from 0 to 60°C. The primary focus of this work is to identify
changes in the transition between bouncing to merging outcomes as the
film temperature increases. We will first compare the regime diagrams
where bouncing and merging outcomes were mapped in a Weber number
and normalized film thickness (H* = H/R) space for various ΔT . The
regime maps show that, for deep pool (H* >> 1) and shallow pool (H∗ ≈
1) limits, ΔT exhibits varied degrees of influence on the bouncing and
merging transitions. Large ΔT , however, renders merging easier across
all H* and beyond a critical temperature difference (ΔT ≥ 60°C for n-
tetradecane) the bouncing regime essentially disappears. Subsequently, to
explain the observed dynamics, we will discuss the role of evaporation and
vapor layer adjacent to the heated liquid film on the interfacial merging.
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Presenters
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Brooklyn Asai
University of California San Diego
Authors
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Brooklyn Asai
University of California San Diego
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Abhishek Saha
University of California, San Diego