L3 Vertical Structure Pt1 1


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L3 Vertical Structure Pt1 1

  1. 1. arc5410 Advanced Structure and Construction
  2. 2. 3.0 Vertical Structural Systems Pt. 1
  3. 3. <ul><li>Vertical Structure in Tall Buildings </li></ul><ul><ul><li>Types of loads on tall buildings: </li></ul></ul><ul><ul><ul><li>Vertical Loads (gravity) both live and dead. </li></ul></ul></ul><ul><ul><ul><li>Lateral Loads. Wind and Earthquake (seismic) </li></ul></ul></ul><ul><ul><ul><li>Other: Temperature differential. Blast/impact. </li></ul></ul></ul><ul><ul><li>Effect of loads on tall buildings: </li></ul></ul><ul><ul><ul><li>Accumulated weight of gravity loads: creates very high column forces at the ground. </li></ul></ul></ul><ul><ul><ul><li>Overturning. Foundations must be able to resist the large moment overturning force. </li></ul></ul></ul><ul><ul><ul><li>Lateral displacement: wind and seismic forces cause building to sway. Lateral forces induce large shear forces in the vertical structure. The structure must be made stiff enough to resist the associated displacements, both throughout the vertical structure of the building as well as at the foundations (sliding shear). </li></ul></ul></ul><ul><ul><li>Types of Vertical Structure Systems </li></ul></ul><ul><ul><ul><li>Wall and pier structure (shear wall) </li></ul></ul></ul><ul><ul><ul><li>Rigid frames both steel and reinforced concrete (stiffness achieved through rigidity of beams and columns and their connections) </li></ul></ul></ul><ul><ul><ul><li>Frame and core systems (lateral stiffness primarily by a rigid core of r/c or braced steel frame) </li></ul></ul></ul><ul><ul><ul><li>Frames with exterior bracing: trussed frames </li></ul></ul></ul><ul><ul><ul><li>Belt and outrigger truss frames with framed core </li></ul></ul></ul><ul><ul><ul><li>Tubular frames (single tube, tube within tube, bundled tube) </li></ul></ul></ul><ul><ul><ul><li>Mega-structural frames </li></ul></ul></ul><ul><ul><ul><li>Other: Cantilever, Suspension, Deep beam systems </li></ul></ul></ul>
  4. 4. Wind loads are dynamic in nature but are applied to buildings as a static wind pressure.
  5. 5. Tacoma Narrows Bridge (collapsed under moderately strong winds in 1940) Washington State, USA
  6. 6. Wind forces on a tall building. Example of variation of wind pressures as measured by a research study at MIT. Wind profiles for three different ground conditions. Example of stipulated wind pressures at set heights. Building Code of New York City ca. 1990.
  7. 7. Wind pressure on buildings (This information is optional) The wind pressure formula that determines the wind pressure acting on a surface due to a given wind speed is formulated from the Bernoulli equation (Daniel Bernoulli 1700-1782) q (pressure in psf) = 1 / 2 p V 2 where p is air mass density and V is the wind speed in mph Then, q = 0.00256 V 2 (for a standard atmosphere at sea level and temperature 15deg, the air density is 0.0765 lb/ft 3 .) Wind speed is measured by weather stations worldwide and given as the fastest velocity at 30ft above ground based on a recurrence period of 50 years. Since the velocity of the wind increases with height, the pressure on the building will vary at different heights. This variation is calculated by formula and the results given in graphic charts such as the example given on the preceding slide of the NYC Building Code wind pressure chart. Another factor that affects wind speed is context, or the type of exposure to wind of the surrounding area. Four exposure conditions are used. Exposure A: large, dense cities a = 3.0 z g = 1500 ft Exposure B: urban and suburban areas, also forested areas a = 4.5 z g = 1200 ft Exposure C: flat, open country and slightly rolling landscape a = 7.0 z g = 900 ft Exposure D: unobstructed coastal areas a = 10.0 z g = 700 ft The factors “a ” and “z g ” are used in the following exposure coefficient formula: K z = 2.58 (z / z g ) 2/ a The final consideration is the shape of the building in plan. For a typical rectangular hi-rise, the shape coefficient C p = 1.3 The full equation then for wind pressure taking into account the height above the ground (z), the exposure condition (K z ), and the shape coefficient C p is: q = 0.00256 V 2 K z C p Therefore, for an exposure condition C, the wind pressure at 250ft high due to a 100mph wind speed on a rectangular bldg. is: q = 0.00256 (100mph) 2 x (2.58) ( 250 / 900) 2/7 (1.3) = 155.22 psf To convert wind pressure into kN/m 2 First, divide the wind speed (if given in km/hr) by 1.609 to get mph, substitute, and multiply the calculated pressure by .04788 to get kN/m 2 . Note: to calculate the complex exponential (250/900) 2/7 it is convenient to refer to the following website: http://www.analyzemath.com/Calculators_2/power_calculator.html
  8. 8. Wind induced sway of tall buildings. As wind hits the surface of a tall building it will wrap around the side of the structure creating wind currents called “eddies” that create negative pressures. The wind fluctuates from side to side of the tall building and this constant fluctuation will cause the building to deflect laterally. If the frequency of the changing pressure from side to side matches the natural resonance frequency of the tower, it will be magnified and deflections will increase dramatically. To counter this effect it has been found that the tapered shape of a tower as well as certain asymmetries in the profile will disrupt the wind currents and counter the effect of sway. Also large openings in a tower, especially near the top, will have a similar effect.
  9. 9. Pirelli Headquarters Tower Milan, Italy Gio Ponti with P. L. Nervi ca. 1963 Wind tunnel tests measure the deflection of the tower and show the torsional deflection resulting from the asymmetric placement of the cores.
  10. 10. Citicorp Tower Arch: Hugh Stubbins Engr: Willliam LeMessurier NYC 1977
  11. 11. Tall buildings with efficient shapes. A rounded shape in plan allows wind to flow more easily around a tall building. Building Codes allow the wind pressure for octagonal and hexagonal shapes to be reduced 20% while circular and elliptical shapes may be reduced by 40%. The tapering of a building as it rises effects a large reduction in wind loads and therefore drift. At higher elevations where wind speeds are high, there is less building surface providing resistance too the wind, thereby lower the amount of wind force on the structure.
  12. 12. The profile of the tall building is shaped to reflect the bending moment diagram. The wider base provides a larger resisting moment to overturning without too large of an increase in stress.
  13. 13. Marina City 1962 Hopewell Centre 1980 RWE Headquarters 1996 Swiss Re Tower 2003
  14. 14. The rigid steel frame provides lateral stiffness and strength while allowing the building to maintain a straight profile. The deflection of a tall frame structure is a combination of the movement due to bending of the whole structure and the horizontal deflection due to the bending of individual beams and columns.
  15. 16. 1 Bearing wall system Three types: cross wall system, long wall system and two-way system.
  16. 17. Shear walls. Openings in shear walls can reduce the effectiveness of lateral force resistance. In fig. a the openings in the wall are small and do not significantly affect performance, The wall acts as a single panel to resist overturning. In fig. e the opening in the wall is continuous and causes the end-wall to act as two independent shear walls with each resisting half the lateral force.
  17. 18. Examples of different configurations of shear resisting panels.
  18. 19. 2 Wall-core system Lateral force resistance is shared between load bearing wall structure and service core structures.
  19. 20. 3 Core-frame system The structural core acts as a shear wall. The frame may contribute also to the lateral stiffness, depending on the type of frame. A hinged frame contributes nothing and only carries vertical loads. A rigid frame contributes significantly.
  20. 21. Lateral force system: stiff core-columns acting like “shear walls” Sendai Mediatheque Toyo Ito & Associates 2000
  21. 22. Lateral force system: braced columns acting like “shear walls”. Hall 26 Thomas Herzog Hanover Expo 2000
  22. 23. Centre Pompidou. Stiff compress struts connecting trusses together at their ends and mid-points to form a braced shear wall. On the long sides the crossed tension rods keep the frames from racking sideways.
  23. 24. Maintenance building at Fiumicino Airport, Rome Italy. Fuhlsbuttel Air Terminal, Hamburg Germany Ricardo Morandi ca. 1960 Von Gerken, Marg and Partners 1993 Slanted columns. Pairs of slanted columns connected across the top with a continuous beam forms a stiff, lateral force resisting structure similar to a braced frame.
  24. 27. Types of vertical structural systems
  25. 28. Type e: core and slab (reinforced concrete flat slab with drop panels) Gateway 2 Wong & Ouyang (HK) Ltd Harbor City, Hong Kong 1999
  26. 29. Gateway 2 Wong & Ouyang (HK) Ltd Harbor City, Hong Kong 1999
  27. 30. Type i: rigid frame (reinforced concrete frame) Stanhope House Lee & So and Associates Quarry Bay, Hong Kong 1990
  28. 31. Stanhope House Lee & So and Associates Quarry Bay, Hong Kong 1990
  29. 32. Type f: interspatial type h: staggered truss Interspatial truss system vs Staggered truss system Trusses every second floor. Trusses every floor but staggered but in alignment in plan. Columns at spacing equal to to the secondary span. Columns at spacing of 1/2 the secondary span (each truss supports a floor on the top chord and also a floor on below on the lower chord).
  30. 33. Type b: cores and wall Knights of Columbus Roche, Dinkaloo & Assocs. New Haven, CT 1969 Cylindrical wall corner service shafts accommodate all vertical and lateral loading. 23 stories, 27.7m x 27.7m column free space with one 9.14m x 9.14m central core.