Research output: Contribution to journal › Article › peer-review
Mixing and wall heat transfer during vertical coalescence of drops placed over a superhydrophobic surface. / Somwanshi, Praveen M.; Muralidhar, K.; Khandekar, Sameer et al.
In: Interfacial Phenomena and Heat Transfer, Vol. 8, No. 3, 2020, p. 207-224.Research output: Contribution to journal › Article › peer-review
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TY - JOUR
T1 - Mixing and wall heat transfer during vertical coalescence of drops placed over a superhydrophobic surface
AU - Somwanshi, Praveen M.
AU - Muralidhar, K.
AU - Khandekar, Sameer
AU - Vyacheslav, Cheverda
N1 - Funding Information: Financial support for colleagues from India was provided by the Department of Science & Technology, India from an Indo-Russian project (Grant No. DST/ME/2018193) and is gratefully acknowledged. Financial support for colleagues from Russia was received from the Russian Foundation for Basic Research (RFBR Grant No. 18-58-45016). Measurement of the wetting angle of the substrate is performed under state contract with IT SB RAS.
PY - 2020
Y1 - 2020
N2 - The configuration of a pair of liquid droplets of unequal temperatures with one placed initially above the other is encountered in thermal spray applications and investigated in the present study. The lower drop is initially cold and placed above a horizontal superhydrophobic surface of equilibrium contact angle 150 deg. The second drop placed above the first is initially at a higher temperature before coalescence. The two drops merge and spread over the substrate. Three liquids of interest are Cs-alloy, water, and glycerin with Prandtl numbers of 0.036, 6.64, and 7188.6, respectively. Coalescence process takes place under atmospheric conditions while thermal interaction between the liquid medium and the substrate (copper, α ∼ 10−4 m2 /s and Teflon, α ∼ 10−7 m2 /s) makes it a conjugate heat transfer process. With reference to the volume of the combined drop, Bond number is close to 0.2. Flow and heat transfer simulations are performed for the coalescence process of the two drops as they exchange energy with the substrate and approach thermal equilibrium. The interfacial shapes generated in time, temperature distribution, and the wall heat flux are primary quantities of interest. An axisymmetric coordinate system has been adopted for numerical simulations with the Kistler’s model representing contact line motion. Water and Cs-alloy show drop recoil followed by oscillatory spreading over the surface. Thermal convection is visible in water while it is suppressed in glycerin and Cs-alloy owing to high viscosity and thermal diffusivity, respectively, in these media. The instantaneous surface-averaged wall heat flux is initially zero, increases quickly to a maximum, and then gradually decreases to small values. The evolution of wall heat flux in water shows time-dependent oscillations while it is monotonic in glycerin as well as Cs-alloy. Among the three liquids, Cs-alloy displays the highest instantaneous peak in wall heat flux.
AB - The configuration of a pair of liquid droplets of unequal temperatures with one placed initially above the other is encountered in thermal spray applications and investigated in the present study. The lower drop is initially cold and placed above a horizontal superhydrophobic surface of equilibrium contact angle 150 deg. The second drop placed above the first is initially at a higher temperature before coalescence. The two drops merge and spread over the substrate. Three liquids of interest are Cs-alloy, water, and glycerin with Prandtl numbers of 0.036, 6.64, and 7188.6, respectively. Coalescence process takes place under atmospheric conditions while thermal interaction between the liquid medium and the substrate (copper, α ∼ 10−4 m2 /s and Teflon, α ∼ 10−7 m2 /s) makes it a conjugate heat transfer process. With reference to the volume of the combined drop, Bond number is close to 0.2. Flow and heat transfer simulations are performed for the coalescence process of the two drops as they exchange energy with the substrate and approach thermal equilibrium. The interfacial shapes generated in time, temperature distribution, and the wall heat flux are primary quantities of interest. An axisymmetric coordinate system has been adopted for numerical simulations with the Kistler’s model representing contact line motion. Water and Cs-alloy show drop recoil followed by oscillatory spreading over the surface. Thermal convection is visible in water while it is suppressed in glycerin and Cs-alloy owing to high viscosity and thermal diffusivity, respectively, in these media. The instantaneous surface-averaged wall heat flux is initially zero, increases quickly to a maximum, and then gradually decreases to small values. The evolution of wall heat flux in water shows time-dependent oscillations while it is monotonic in glycerin as well as Cs-alloy. Among the three liquids, Cs-alloy displays the highest instantaneous peak in wall heat flux.
KW - Coalescence
KW - Conjugate heat transfer
KW - Copper
KW - Cs-alloy
KW - Glycerin
KW - Heat flux
KW - Liquid drops
KW - Superhydrophobic surface
KW - Teflon
KW - Vertical orientation
KW - Wall temperature
KW - Water
KW - vertical orientation
KW - coalescence
KW - superhydrophobic surface
KW - CONTACT LINE
KW - liquid drops
KW - water
KW - conjugate heat transfer
KW - FLOW
KW - wall temperature
KW - glycerin
KW - copper
KW - heat flux
UR - http://www.scopus.com/inward/record.url?scp=85098864901&partnerID=8YFLogxK
U2 - 10.1615/InterfacPhenomHeatTransfer.2020035034
DO - 10.1615/InterfacPhenomHeatTransfer.2020035034
M3 - Article
AN - SCOPUS:85098864901
VL - 8
SP - 207
EP - 224
JO - Interfacial Phenomena and Heat Transfer
JF - Interfacial Phenomena and Heat Transfer
SN - 2169-2785
IS - 3
ER -
ID: 27416388