TY - JOUR
T1 - A Closer Look at the Evolution of Supercooled Cloud Droplet Temperature and Lifetime in Different Environmental Conditions with Implications for Ice Nucleation in the Evaporating Regions of Clouds
AU - Roy, Puja
AU - Rauber, Robert M.
AU - Di Girolamo, Larry
N1 - Acknowledgments. This work was funded by the NASA Earth Venture Suborbital-3 (EVS-3) IMPACTS program under Grant 80NSSC19K0355 and the NASA CAMP2Ex program under Grant 80NSSC18K0144. This research was also supported by the National Science Foundation under Grant NSF AGS-2016106. We thank Tim Brice for providing more information about the thermodynamic wet-bulb temperature calculation procedure used by NWS. We also thank Dr. Zachary J. Lebo and two anonymous reviewers for their thorough reviews and comments to help improve the manuscript.
This work was funded by the NASA Earth Venture Suborbital-3 (EVS-3) IMPACTS program under Grant 80NSSC19K0355 and the NASA CAMP2Ex program under Grant 80NSSC18K0144. This research was also supported by the National Science Foundation under Grant NSF AGS-2016106. We thank Tim Brice for providing more information about the thermodynamic wet-bulb temperature calculation procedure used by NWS. We also thank Dr. Zachary J. Lebo and two anonymous reviewers for their thorough reviews and comments to help improve the manuscript.
PY - 2023/10
Y1 - 2023/10
N2 - This study investigates the evolution of temperature and lifetime of evaporating, supercooled cloud droplets considering initial droplet radius (r0) and temperature (Tr0), and environmental relative humidity (RH), temperature (T∞), and pressure (P). The time (tss) required by droplets to reach a lower steady-state temperature (Tss) after sudden introduction into a new subsaturated environment, the magnitude of ∆T = T∞ - Tss, and droplet survival time (tst) at Tss are calculated. The temperature difference (∆T) is found to increase with T∞, and decrease with RH and P. ∆T was typically 1–5 K lower than T∞, with highest values (~10.3 K) for very low RH, low P, and T∞ closer to 0ºC. Results show that tss is <0.5 s over the range of initial droplet and environmental conditions considered. Larger droplets (r0 = 30–50 mm) can survive at Tss for about 5 s to over 10 min, depending on the subsaturation of the environment. For higher RH and larger droplets, droplet lifetimes can increase by more than 100 s compared to those with droplet cooling ignored. Tss of the evaporating droplets can be approximated by the environmental thermodynamic wet-bulb temperature. Radiation was found to play a minor role in influencing droplet temperatures, except for larger droplets in environments close to saturation. The implications for ice nucleation in cloud-top generating cells and near cloud edges are discussed. Using Tss instead of T∞ in widely used parameterization schemes could lead to enhanced number concentrations of activated ice-nucleating particles (INPs), by a typical factor of 2–30, with the greatest increases (≥100) coincident with low RH, low P, and T∞ closer to 0ºC.
AB - This study investigates the evolution of temperature and lifetime of evaporating, supercooled cloud droplets considering initial droplet radius (r0) and temperature (Tr0), and environmental relative humidity (RH), temperature (T∞), and pressure (P). The time (tss) required by droplets to reach a lower steady-state temperature (Tss) after sudden introduction into a new subsaturated environment, the magnitude of ∆T = T∞ - Tss, and droplet survival time (tst) at Tss are calculated. The temperature difference (∆T) is found to increase with T∞, and decrease with RH and P. ∆T was typically 1–5 K lower than T∞, with highest values (~10.3 K) for very low RH, low P, and T∞ closer to 0ºC. Results show that tss is <0.5 s over the range of initial droplet and environmental conditions considered. Larger droplets (r0 = 30–50 mm) can survive at Tss for about 5 s to over 10 min, depending on the subsaturation of the environment. For higher RH and larger droplets, droplet lifetimes can increase by more than 100 s compared to those with droplet cooling ignored. Tss of the evaporating droplets can be approximated by the environmental thermodynamic wet-bulb temperature. Radiation was found to play a minor role in influencing droplet temperatures, except for larger droplets in environments close to saturation. The implications for ice nucleation in cloud-top generating cells and near cloud edges are discussed. Using Tss instead of T∞ in widely used parameterization schemes could lead to enhanced number concentrations of activated ice-nucleating particles (INPs), by a typical factor of 2–30, with the greatest increases (≥100) coincident with low RH, low P, and T∞ closer to 0ºC.
KW - Cloud droplets
KW - Cloud microphysics
KW - Clouds
KW - Evaporation
KW - Humidity
KW - Ice particles
UR - https://www.scopus.com/pages/publications/85175642958
UR - https://www.scopus.com/pages/publications/85175642958#tab=citedBy
U2 - 10.1175/JAS-D-22-0239.1
DO - 10.1175/JAS-D-22-0239.1
M3 - Article
AN - SCOPUS:85175642958
SN - 0022-4928
VL - 80
SP - 2481
EP - 2501
JO - Journal of the Atmospheric Sciences
JF - Journal of the Atmospheric Sciences
IS - 10
ER -