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Basic Convective Cloud Dynamics

Basic Convective Cloud Dynamics. Basic equations for vertical acceleration, mass continuity, & buoyancy. 1-D Lagrangian model. Based on classic model of continuous & homogeneous entrainment. 1-D Lagrangian model Temperature equation. Predicts parcel temperature & buoyancy.

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Basic Convective Cloud Dynamics

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  1. Basic Convective Cloud Dynamics

  2. Basic equations for vertical acceleration, mass continuity, & buoyancy

  3. 1-D Lagrangian model Based on classic model of continuous & homogeneous entrainment

  4. 1-D Lagrangian model Temperature equation Predicts parcel temperature & buoyancy

  5. 1-D Lagrangian model Momentum equation Kessler warm cloud microphysics

  6. Entrainment Turbulent jet

  7. Entrainment Thermal 2

  8. Entrainment Starting plume

  9. Entrainment Raymond & Blyth’s Model of discontinuous, inhomogeneous entrainment

  10. Three-dimensional Vorticity Vorticity equations under Boussinesq conditions

  11. Three-dimensional Vorticity Generation of horizontal vorticity by buoyancy

  12. Three-dimensional Vorticity Stretching of vertical vorticity Horizontal convergence

  13. Three-dimensional Vorticity Tilting of horizontal vorticity into the vertical

  14. Three-dimensional Vorticity Linearize vertical vorticity equation around the basic state: At a level in the cloud where the cloud is moving with the basic state velocity:

  15. Three-dimensional Vorticity Linear process leads to vorticity couplet in an convective cloud that develops in a sheared environment

  16. Pressure Perturbation The pressure perturbation field in a convective cloud is governed by:

  17. Pressure Perturbation Pressure gradient force required by the buoyancy field Note! These are lines of force, not air motions

  18. Pressure Perturbation The pressure perturbation field in a convective cloud is governed by: When vortices form in storms, this term requires a low pressure at the center of each vortex. These low pressure centers affect the storm dynamics by producing a pressure field in the storm that is different from that produced by buoyancy alone.

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