Application of numerical cloud model in hail suppression of cold clouds Javanmard, Sohaila1; Karimpirhayati, Mahla2; BodaghJamali, Javad3; Abedini, Yusefali2 Atmospheric Science and Meteorological Research Center (ASMERC), Pajuhesh Blvd., Tehran-Karaj Highway, Tehran, I. R. of Iran, [email protected], [email protected] 2 Department of Physics, Zanjan University, Zanjan, I. R. of Iran, [email protected], [email protected] 3 University of Environment, standard Squar, Karaj, I. R. of Iran, [email protected], [email protected] 1 1. Introduction Hail induces many damages to agriculture, transportation, economical affairs in hail prone area over Iran annually (Jamali et al., 2010). In order to achieve hail risk management to decrease eht induced destruction in Iran, application of hail suppression methods is necessary. In order to asses the performance of operational cloud seeding operations and achieve desirable results, application of numerical cloud model is one of the most important tools to assess the seeding effect on hail suppression. In this paper, effects of Silver Iodide (AgI) cloud seeding in order to hail suppression have been examined using one dimensional time dependent numerical cloud model. 2. Hail suppression model The governing dynamical equations of model is based on Ogura and Takahashi (1971), microphysical parameterization of natural precipitation process is based on Lin et al., (1983), and cloud seeding parameterization is based on Zhen and Heng-Chi (2010). Ogura and Takahashi model is a time dependent and one dimensional model with bulk parameterization. In this model, the cloud is modelled as a circular air column with a time dependent radius in an environment at rest. All dynamical equations have been formulated in a one dimensional space based on Asai and Kasahara(1967). In Ogura and Takahashi model, nine microphysical processes has been parameterized with four water substances including water vapor, cloud droplet, raindrop and hail. Lin et al. model (1983) is a two dimensional, time dependent cloud model which it has been used to simulate a moderate intensity thunderstorm. In this model, six forms of water substance (water vapor, cloud water, cloud ice, rain, snow and hail/graupel) are simulated and 32 microphysical processes are considered as shown in Fig .1. In hail suppression model, dynamic and thermodynamic equations are based on Ogura and Takahashi model (1971) that cloud ice and snow are added and microphysics of natural precipitation is based on Lin et al. model (1983). Three microphysical processes for seeding are added to model that is based on Zhen and Heng-Chi (2010). When AgI is inserted to the cloud base, it affects on six cloud hydrometeors including cloud droplet, raindrop, snow and hail mixing ratios via contact and deposition nucleation, transportation from rain drop to snow and droplet to cloud ice due to seeding. The equation of the vertical component of velocity in a cylindrical coordinate may be written as: 2 ∂w ∂w 2α ~ )+ − = −w w w + u~a ( w − w a ∂t ∂z a a T − Tν 0 g ν − g (Qc + Qr + Qi + Qs + QG + X s )(1) ν0 The first term in the right-hand side of Eq. (1) represents the vertical advection, the second term the lateral eddy exchange, the third term the dynamic entertainment that is required to satisfy the mass continuity between the cloud and the environment, the fourth term the buoyancy, and the last term the drag force that is assumed to be provided by the weight of cloud droplets, raindrops, cloud ice, hail, snow, and AgI. In this research, dynamical equations with 32 microphysical processes have been coded by Fortran programming according to Javanmard et al. (2010), then three seeding microphysical parameterization have been added to cloud model. Finally, results have been compared before and after seeding. Water Vapor PIMLT Cloud Droplet PIDW PIHOM PSFW PSAUT PSACI PSACW PREVP PGACW Cloud Ice PSFI PRACI PSSUB PSDEP Snow PRACW PGSUB PSACR PSACW PRAUT PGAUT PIACR PGACS PRACI PRACS PSMLT PGACR Rain Water PGACR PIACR PGMLT PGFR PSACR Hail/Graupel Precipitation at Ground Fig. 1. Microphysical processes in Lin et al. model (1983). 3. Results and conclusion In this paper, effects of cloud seeding by AgI have been simulated in one dimensional cloud model. It is concluded that as AgI introduced into the cloud at height about 6.5 km above the surface (temperature less than -20 degree Celsius) within 30 minutes after cloud formation, and with mixing ratio about 2.5*10-9 gg-1 resulting in rainfall intensity enhancement about %20. Moreover, heterogeneous nucleation of AgI enhanced the cloud ice, so snow increased and rainfall enhanced by melting of snow and cloud ice. On the other hand, cloud ice consumed to produce snow and they did not grow up to reach hail size, so the processes that related to growth of hail decreased strongly. (dry growth of hail) before seeding and they are (wet growth of graupel/hail) graupel/hail) and after seeding. From Figs. 6 and 7, it has been concluded that the most effective sink terms is (melting of hail to form rain) before seeding and it is (sublimation of hail) after seeding. HIAL MIXING RATIO (gr/kg) BEFORE SEEDING 14 7.09685 5.67748 4.73123 4.25811 3.31186 2.83874 2.36562 1.41937 0.473123 12 2.37 8 1.42 6 6 3.3 1 4.2 HEIGHT(km) 0.47 10 4.73 2.84 4 Fig. 4. Hail sources terms ( 0.47 ) before seeding 2 20 40 60 80 TIME(min) Fig. 2. Hail mixing ratio versus height and time before seeding HAIL MIXING RATIO (gr/kg) AFTER SEEDING 14 3.33154 2.88733 2.44313 1.99892 1.55472 1.11051 0.666308 0.222103 0.22 1 1.1 10 1.55 0.67 6 Fig. 5. Hail sources terms ( 9 2.44 2.8 8 3 3.3 0 7 2.0 0.6 HEIGHT(km) 12 ) after seeding 4 0.2 2 20 2 40 60 80 TIME(min) Fig. 3. Hail mixing ratio versus height and time after seeding The contours of hail mixing ratio versus height and time have been shown in Figs. 2 and 3, which the maximum values of hail mixing ratio are7.1 and 3.3 before and after seeding, respectively. Hail mixing ratio has been reduced about %53. From Figs. 4 and 5, the most effective (accretion of rain by cloud source terms are (accretion of rain by snow; ice; produces hail), (freezing of rain to form produces hail), and Fig. 6. Hail sinks terms ( ) before seeding Fig. 7. Hail sinks terms ( ) after seeding References Asai T. and A. Kasahara, A Theoretical study of the compensating downward motions associated with cumulus clouds, J. Atmos. Sci., 24, 487-496, 1967. Jamali J. B., S. Javanmard and Sh. Fateh, Investigating about hail event in Iran and methods of control and hail th suppression, 14 Geophys. Conf., Iran, 2010. Javanmard S., J. B. Jamali, M. Karimpirhayati and Y. Abedini, Numerical study for role of cold convective cloud parameterization in precipitation pattern at ground, 14th Geophys. Conf., Iran, 2010. Lin Y. L., R. D. Farely and H .D. Orville, Bulk parameterization of the snow field in a cloud model, J.Climate Appl. Meteor., 23, 1065-1092, 1983. Ogura Y. and T. Takahashi, Numerical simulation of the life cycle of A thunderstorm cell, Mon. Wea. Rev., 19, 895-911, 1971. Zhen Z. and L. Heng-Chi, Numerical simulation of seeding extra-area effects of precipitation using a three-dimensional mesoscale model, Atmos. Ocea. Sci., 3, 19−24, 2010.
© Copyright 2026 Paperzz