basis of structural design · prestress is retained due to the bond between the concrete and the...
TRANSCRIPT
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Basis of Structural Design
Course 4
Structural action:
- prestressing
- plate and shell structures
Course notes are available for download athttps://www.ct.upt.ro/studenti/cursuri/stratan/bsd.htm
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Prestressing
Prestressing: setting up an initial state of stress, that makes the structure work better than without it
Examples:– wall plugs
– spider's web
– bicycle wheel
Main use in structural engineering: prestressed concrete
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Prestressing examples: wall plug
A hole in the wall is filled with a wooden or plastic plug
The screw driven into the plug squeezes the plug against the sides of the hole, generating compressive stresses in the plug and in the wall around it
Compressive prestressing generates frictional resistance to pulling out the screw
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Prestressing examples: spider's web
Spider's web threads: high tensile, but no compressive resistance
Spider pulls its threads tight, creating a tensile prestressing
A load in the centre of the web produces compressive forces in the threads below it
Without the tensile prestress, the lower part of the web would go slack, being more prone to collapse
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Prestressing examples: bicycle wheel
Wire spokes are strong in tension but weak in compression (due to buckling)
Spokes must be kept in tension
When the wheel is assembled, spokes are tightened up uniformly by the turnbuckles at the rim
Under a downward load on the wheel, the spokes in the lower part of the wheel tend to be subjected to compression
Tensile prestress in the spokes must be higher than the compression force to keep all the spokes in tension
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Prestressing examples: bicycle wheel
Other types of loading on the wheel: due to braking and due to taking a sharp corner
Forces due to braking:– could not be resisted if the spokes were arranged radiating from
the centre of the hub
– spokes are set at an angle to the radii, each pair forming a triangulated system which is able to generate tensile and compression forces which oppose the braking force
– tensile prestress ensures that all spokes are in tension and active
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Prestressing examples: bicycle wheel
Forces due to cornering:– force is imposed on the wheel at right
angles to its plane
– the spokes are inclined with respect to the plane of the wheel, forming a triangulated system, which resists the forces due to cornering
– tensile prestress ensures that all spokes are in tension and active
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Other prestressing examples
Pneumatic tire of cycle wheel
Inflated membranes for storage spaces and sport halls– air pressure inside is maintained above the atmospheric pressure
by blowers
– fabric of the membrane permanently in tension
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Other prestressing examples
A set of books: no tensile resistance between the volumes
The books can be moved if a pressure is applied at the middepth:– the row of books act as a simply
supported beam
– the pressure overcomes the tensile stress in the lower part due to own weight of the books, enabling them to act as a unit
The books can be moved with lower pressure if it is applied somewhat lower than the middepth: an upward moment is introduced, which counteracts the downward moment due to own weight of the books
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Reinforced concrete beams
Concrete: weak in tension
When loading is applied on a simply supported beam, the concrete cracks at the tension side:– Concrete active in compression
– Steel reinforcement active in tension
– Only a small part of the concrete cross-section resists the applied loading
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Prestressed concrete beams
Concrete is kept in compression by cables or rods
The whole concrete cross-section can be considered in design
Substantial economy in material
If prestressing is applied in the centroid of the cross-section:– by choosing correctly the
prestressing force, the entire cross-section can be kept in compression
– a large stress is present at the compression side
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Prestressed concrete beams
Position of prestressing force: important
If prestressing is applied at 1/3 of the beam depth from the bottom face:– a negative moment due to eccentric
prestressing counteracts the positive bending moment due to applied moment
– the pestressing force needed to keep the entire cross-section in compression can be reduced
– the stress at the compression side is reduced the required concrete strength can be reduced
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Prestressed concrete beams
Bending moment due to dead weight in a simply supported beam: parabolic shape
The best arrangement of the prestressing tendons?
a parabolic shape along the beam, in order to generate bending moment M=Fe counteracting the bending moment due to dead load
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Prestressed concrete beams
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Prestressed concrete
Type of prestress:– Posttensioning: the prestressing force is applied after concrete
has been cast and has set, through tendons located in holes left in concrete elements. The prestress is retained due to anchorage of steel tendons at the end of the element.
– Pretensioning: prestressing wires are stretched over a long length and the concrete is cast around them in steel forms. The prestress is retained due to the bond between the concrete and the steel wires.
Problems related to prestressing:– When the concrete sets up, it shrinks, leading to loss of
prestressing (in the case of pretensioning)
– Concrete shortens in time (creep) after it sets up due to compression acting on it, leading to loss of compression
– High strength steel required for prestressing, in order to reduce the loss of prestress due to shrinkage and creep
– Higher strength concrete is needed to resist higher compression and to reduce the contraction due to creep and shrinkage
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Plates
Plates: a flat surface element that acts in bending in order to resist out of plane loading
The simplest plate: a flat slab spanning between two supports
It may appear to behave like a wide beam, but it is not as simple as that
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One-way plates
When a narrow beam bends, the material in the lower half of the beam extends longitudinally it contracts in the transversal direction due to Poisson effect ( times the longitudinal strain)
The material in the upper half of the beam contractslongitudinally it expands in the transversal direction
An anticlastic curvature of the beam in the transversal direction equal with times the longitudinal curvature
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One-way plates
In plates the anticlastic curvature is suppressed due to large dimension in the transversal direction (the deflected shape is almost cylindrical, except near the free edges)
At any point of the beam there is a transverse bending moment equal to times the spanwise bending moment
Suppression of the transverse curvature induces an additional spanwise curvature
In one-way plates reinforcement is needed in both spanwise and transverse direction
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Two-way plates
Two-way plates simply supported on all four sides: complicated interaction between the two ways in which a load is supported
If a slab is more than about 4 times as long as it is wide, the bending moment at the center of the plate is almost the same as in a one-way plate supported on longer edges. Why?
Stiffer structural action (bending in the short direction) attracts larger forces
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Stiffness in structural action
A straight bar of length L and rectangular cross-section can support a concentrated force P in two ways:– as a column acting in compression
– as a cantilever acting in bending
In the column the stress 1 is axial and uniform
In the cantilever the stress 2 has a linear variation along the bar and across the cross-section the material is far less efficient
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Stiffness in structural action
Column is much stronger than the beam: 2/1 = 6(L/h)for L/h=20 2/1 = 120
Column is much stiffer than the beam: 2/1 = 4(L/h)2
for L/h=20 2/ 1 = 1600 (P=k∙ k1/k2 = 1600)
If the beam and the column are used in conjunction to support the load P:– the two members deflect by the
same ammount
– P=k∙ P1=k1∙1; P2=k2∙2. If the deflection is the same for the two members 1=2 P1/k1 = P2/k2; P1/P2=k1/k2 = 1600
– the column carries a load of (1600/1601)P
– the beam carries a load of (1/1601)P
Of the two alternative modes of action open to this structure, it chooses the column compression, because it is stiffer
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Membrane action
Some structures can support loads only in bending.Example: simply supported beam
Uniform loading:– the neutral axis becomes curved
– roller support moves slightly toward the other end of the beam
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Membrane action
A beam pinned at both ends
Uniform loading:– the neutral axis becomes curved
– horizontal movement of the support is prevented longitudinal tension H develops the beam begins to support load as a slightly curved cable or catenary
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Membrane action
The catenary action is much stiffer than bending
Beam action: stiffness remains constant
Catenary action: stiffness increases with the square of the deflection
As the load increases, the portion of the load carried axially (w1), as catenary, increases rapidly
It can be shown that w1/w2 = 3.33(/h)2
w2 - the portion of the loading carried through bending.When the deflection ammounts to twice the depth of the beam, w1/w2 = 13.33, so that the catenary action ammounts to 13.33/14.33 = 0.93 of the total resistance to load
Membranes: surface elements in which loading is resisted through direct (axial) stresses
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Shells
Shells: surface elements resisting loading through bending and membrane action
Examples:– dome
– human skull
– turtle's armour
– bird egg
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Shells
Bird's egg: weak under a concentrated loading (breaking against a cup's rim) but strong under distributed loading (squeezing between ends with palms)– distributed loading resisted through membrane action (stronger)
– concentrated loading resisted through bending action (weaker)
Domes: – used since ancient times
– capable of resisting through membrane action a variety of distributed loading
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Dome: structural action
The shape of a cable changes as the shape of the applied loading changes
The same behaviour if a set of cables are hanged around a circular perimeter – uniform loading: "bowl" shape
– larger loading toward the supports: the "bowl" bulges toward supports and the bottom rises slightly
– a different shape of the cable is needed in order to resist the applied loading through axial action only
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Dome: structural action
If a series of circumferential cables are added, capable of resisting both tension and compression
When the load changes, the circumferential cables prevent the dome from changing its shape:– circumferential cables near the rim are
put into tension
– those near the bottom are put into compression
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Dome: structural action
A system formed by using enough cables in order to obtain a surface approximates a thin-shelled dome
Such a structures is capable of carrying a variety of distributed loading through membrane action (stresses which are uniformly distributed over the thickness of the shell)
A shell is capable of resisting loads either through bending stresses or direct (membrane) stresses
Membrane action is "preferred" by the dome, as it is much stiffer for this action
Ideally, for a membrane action to take place in a shell, it must be thin and its shape should be similar to that assumed by a flexible membrane under the same loading
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Dome: structural action
The heaviest load in many domes is their own weight
In a hemispherical dome of a uniform thickness,– the stresses 1 in the direction of meridians are compressive
throughout
– the circumferential stresses 2 are tensile near the rim: tensile reinforcement needed to resist them
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Shells: hyperbolic paraboloid
Rectangular area to be covered: (a) taking a portion of a sphere and arching it between supports
Rectangular area to be covered: (b) hyperbolic paraboloid - can be obtained by taking a rectangular grid of straight lines and lifting one of the corners, so that the lines would remain straight
A flat surface becomes a curved one, known as hyperbolic paraboloid
Lines drawn diagonally are parabolas, humped in one direction and sagging in the other direction
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Shells: hyperbolic paraboloid
Constructional advantage that elaborate formwork is not needed
Hyperbolic paraboloid supports loads by tension/compression, as opposed to a plate, acting in bending
Given the opportunity, a structure will support loads by direct tension and compression rather than bending
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Shells: hyperbolic paraboloid