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Tall buildings

Tall buildings. Wind loading and structural response Lecture 19 Dr. J.D. Holmes. Tall buildings. Very wind-sensitive in synoptic winds (including hurricanes). Stimulated development of boundary-layer wind tunnel.

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Tall buildings

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  1. Tall buildings Wind loading and structural response Lecture 19 Dr. J.D. Holmes

  2. Tall buildings • Very wind-sensitive in synoptic winds (including hurricanes) • Stimulated development of boundary-layer wind tunnel • Resonant dynamic response for along- and cross-wind very significant (> 100 metres) (‘Rule-of-thumb’ first mode frequency : 46/h Hertz (h in metres) ) • Sometimes torsional response is significant depending on geometry and structural system • Usually governed by serviceability response (peak accelerations and deflections in top floors) • Cladding pressures can be v. high especially at unusual corners and change of cross section

  3. Y (N-S) wind a X (E-W) N-S 1.0 0.5 E-W x x x 0 10 20 30 40 50 60 70 80 90 Angle of attack - degrees x Tall buildings • Empire State Building - full-scale and wind-tunnel studies in 1930’s D - Mean deflection (inches) Uh - Mean wind speed at 1250 feet in MPH (uncorrected) Much stiffer in east-west direction

  4. Wind pressure 0 1 2 3 4 5 6 Time (minutes) Tall buildings • Commerce Court building, Toronto, Canada - 1970’s Full-scale and wind-tunnel measurements of local cladding pressures and overall building response (accelerations) Studies of local pressure peaks and implications for glass design : Acceleration measurements showed significance of torsional component (twist) • 1/200 scale aeroelastic model showed good agreement with full scale

  5. Tall buildings • World Trade Center – New York 1973-2001 • First buildings to be tested in a turbulent boundary-layer flow wind tunnel (mid 1960’s)

  6. Tall buildings • Flow around a tall building :

  7. Tall buildings • Pressure fluctuations on a tall building : (movie by Shimizu Corporation, Tokyo, Japan)

  8. Tall buildings • Pressure fluctuations on a tall building : (movie by Shimizu Corporation, Tokyo, Japan)

  9. Cp (t) Time Tall buildings • Cladding pressures : Four values of pressure coefficients :

  10. stagnation point  0.8h minimummaximum 0.8 1.8 1.6 0.0 0.6 1.4 -0.2 -0.2 0.4 1.0 1.2 1.0 -0.4 -0.4 0.2 0.2 Tall buildings • Square cross section - height/width =2.1 Windward wall :

  11. -2.2 -0.9 -2.4 0.6 -2.0 -0.5 0.4 -2.0 -0.6 -2.2 0.2 -0.8 -1.8 -2.4 -0.8 -0.7 0.0 -2.6 -2.6 -2.8 -2.8 mean Cp’s : -0.6 to -0.8 -0.6 -3.2 -3.0 -3.4 -0.5 -3.8 -0.9 -2.4 largest minimum Cp : -3.8 Tall buildings • Square cross section - height/width =2.1 Side wall (wind from left) :

  12. mean Cp’s : -0.35 to -0.45 largest minimum Cp : -1.6 -1.6 -1.6 -0.45 -0.45 -1.4 -1.4 -0.4 -1.2 -0.35 -0.1 -1.6 -1.6 Tall buildings • Square cross section - height/width =2.1 Leeward wall :

  13. Tall buildings • Glass strength under wind loading Glass strength is dependent on duration of loading : Microscopic flaws on tension side grow at a rate dependent on local stress Accumulated damage at constant temperature and humidity (Brown’s integral) : s(t) is stress; T is total time over which it acts; n is a high power (15 to 20)

  14. Tall buildings • Glass strength under wind loading Under wind loading p(t) : assume s(t) = K[p(t)]m/n (nonlinear) i.e. mth moment of probability density function of Cp

  15. pmax load failure time Tall buildings • Glass strength under wind loading Glass testing is usually carried out with a linearly increasing ‘ramp’ load : damage produced by 1-minute ramp load : pmax is specified load in glass design charts

  16. Tall buildings • Glass strength under wind loading writing pmax as Ck. (1/2)aU2 , where Ck is an equivalent glass design pressure coefficient, and equating damage in ramp load test to that in 1 hour (3600 sec.) of wind : Ck = equivalent glass design pressure coefficient - gives pressure which produces same damage in 1 hour of wind loading as that produced by a 1-minute ramp load Ck is approximately equal to the peak pressure coefficient during the hour of storm winds

  17. Tall buildings • Glass strength under debris impact Glazing is vulnerable to damage and failure by roof gravel in the U.S. ASCE-7 (6.5.9.3) requires glazing above 18.3 m above ground level, and over 9.2m above gravel source, to be protected Gravel acts like a sphere or cube – will only go up if there is a vertical wind velocity component

  18. cross wind along wind Tall buildings • Overall loading and dynamic response Cross-wind vibrations are usually greater than along-wind vibrations for buildings of heights greater than 100m (330 feet)

  19. Tall buildings • Overall loading and dynamic response Standard deviation of deflections at top of a tall building : along wind cross wind Ax and Ay - depend on building shape kx - 2 to 2.5 ky - 2.5 to 3.5 (cross-wind) b - average building density n1 - first mode frequency  - critical damping ratio

  20. Tall buildings • Overall loading and dynamic response Standard deviation of deflections at top of a tall building : Circular cross section :

  21. Modification of corners are effective in reducing response Tall buildings • Overall loading and dynamic response Deflections at top of a tall building : Effect of cross section :

  22. Tall buildings • Torsional loading and response Two mechanisms : • applied moments from aerodynamic forces produced by non-uniform pressure distributions or non-symmetric cross-sections • structural eccentricity between elastic center and geometric center (a 10% eccentricity on a square building: doubled mean twist and increased dynamic twist by 40-50%)

  23. 0.2 0.1 0 0.2 0.4 0.6 0.8 1.0 f = Tall buildings • Torsional loading and response Mean torque coefficient : depends on ratio between minimum and maximum projected widths of the cross section

  24. increases increases decreases Tall buildings • Interference effects Surrounding buildings can produce increases or decreases in peak wind loads : shows percentage change in peak cross-wind response of building B, due to a similar building A at position (X,Y)

  25. Tall buildings • Damping Damping is the mechanism for dissipation of vibration energy Structural damping (Japanese buildings) : reinforced concrete steel frame n1 = first mode natural frequency xt = amplitude of vibration

  26. Tall buildings • Damping Auxiliary damping : Viscoelastic damper : used on World Trade Center buildings, New York

  27. Tall buildings • Damping Auxiliary damping : Tuned mass damper : used on CityCorp building, New York (M2=400 ton of concrete)

  28. Tall buildings • Damping Auxiliary damping : Tuned liquid (sloshing) damper : used on Shin-Yokohama hotel, Japan

  29. Tall buildings • Damping Auxiliary damping : Tuned liquid column damper : to be used on Eureka tower building, Melbourne, Australia (under construction)

  30. End of Lecture 19John Holmes225-405-3789 JHolmes@lsu.edu

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