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Meteorology of Windstorms Wind loading and structural response Lecture 1  Dr. J.D. Holmes
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object],[object Object]
Meteorology of windstorms ,[object Object],Pressure gradient force per unit mass  = p   y   z  z (p+   x)   y   z  x  y  x   y   z
Meteorology of windstorms ,[object Object],[object Object],AA   =    U (  t) 2   a = 2 U     = ( ½)a  (  t) 2   (S. Pole)
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object],   = angle of latitude    = angular velocity of the earth f= 2   sin   Coriolis force is zero where    and f are zero  i.e. at Equator f U
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object]
Meteorology of windstorms ,[object Object],[object Object],[object Object]
Meteorology of windstorms ,[object Object],[object Object],Clockwise rotation in Southern Hemisphere  ,[object Object],Near the equator (   < 5° N), hurricanes cannot form
Meteorology of windstorms ,[object Object],Includes centrifugal force : (U 2 /r) per unit mass  r = radius of curvature of isobars   ,[object Object],[object Object],Quadratic equations for gradient wind speed, U cyclone
Meteorology of windstorms ,[object Object],[object Object],[object Object],U is limited to  for an anti-cyclone, but unlimited for a cyclone cyclone
Meteorology of windstorms ,[object Object],[object Object],[object Object],Direction change with height -  Ekman spiral  <30 o
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Meteorology of windstorms ,[object Object],[object Object],(S. Hemisphere)
Meteorology of windstorms ,[object Object],Wind speed Direction (Figure 1.7 in book shows low wind speed in ‘eye’)
Meteorology of windstorms ,[object Object]
Meteorology of windstorms ,[object Object]
Meteorology of windstorms ,[object Object]
Meteorology of windstorms ,[object Object],pressure gradient wind speed pressure gradient  p = p n -p 0  where p 0  is central pressure Holland (1980)
Meteorology of windstorms ,[object Object],pressure profile gradient wind speed profile Cyclone ‘Tracy’ 1974
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object],[object Object],warm air cool air cumulus cloud
Meteorology of windstorms ,[object Object],Wind speed Direction Max gust 1 hour
Meteorology of windstorms ,[object Object],15m/s 20 30 40 50 Direction of storm
Meteorology of windstorms ,[object Object],Funnel-shaped vortex created in thunderstorms
Meteorology of windstorms ,[object Object],‘ Supercell’ - intense convective cell
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object],[object Object]
Meteorology of windstorms ,[object Object]
Meteorology of windstorms ,[object Object]
Meteorology of windstorms ,[object Object],[object Object],Tangential velocity Static pressure Radial V r     0.5V    Vertical V v     0.62V 
Meteorology of windstorms ,[object Object]
Meteorology of windstorms ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
End of Lecture 1 John Holmes 225-405-3789 JHolmes@lsu.edu

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Meteorology of Windstorms Forces and Wind Field Characteristics

  • 1. Meteorology of Windstorms Wind loading and structural response Lecture 1 Dr. J.D. Holmes
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  • 33. End of Lecture 1 John Holmes 225-405-3789 JHolmes@lsu.edu