Appendix A - Design Comments
Why prestress?
The ultimate load capacity of a prestressed concrete member is no better than that of a reinforced concrete member with reinforcement of similar tensile capacity. Then why prestress? Because at service loads, the two types of construction are markedly different.
The tensile capacity of concrete is notoriously low - only about one-tenth of its compressive capacity. Internal stresses due to shrinkage and temperature changes can often exceed this low tensile capacity, so that even unloaded members will crack.
A reinforced concrete member may be seen as an assembly of loose concrete blocks, prevented only by the reinforcement from falling apart. The reinforcement stretches as it takes tension. This allows the concrete blocks to rotate relative to each other. Corrosive agents can penetrate the cracks. Reinforced concrete deflects more and deteriorates faster than prestressed concrete.
What is prestressing?
If the concrete is put in compression wherever tensile stresses would otherwise cause it to crack, then the problems mentioned above are eliminated. This can be achieved by stretching the reinforcement to its limits and transferring the stretching load to the concrete.
Two methods exist, pre-tensioning and post-tensioning, where 'pre' and 'post' refer to the hardened state of the concrete. Precast planks are prestressed by pre-tensioning.
Unfortunately, losses of the prestress force cannot be avoided. Firstly, as the load is transferred to the concrete, the member will shorten, and some slippage between the tendons and the concrete will occur. Secondly, the concrete continues to shorten with time (a) by its nature to shrink and (b) by its plastic behaviour called creep. Thirdly, steel also displays some plasticity, although much less than concrete, and will relax its load.
These losses can cause a large part of the prestress force to disappear. To ensure that at least some prestress remains for the life of the structure (40 to 60 years), it is imperative that the steel used for prestressing can be stretched considerably more than the sum of the expected shortenings. In precast planks, the tendons are 7-wire super strand to AS 1311 with a minimum tensile strength of 1750 to 1860 MPa, a yield strength of 85% of this value, and a modulus of elasticity of 195 x 10
3 MPa.Solutions create problems
The old saying Every problem has a solution, and every solution creates its own problems is also true of precast prestressed planks. The simple method of design we can employ with reinforced concrete is not enough for prestressed concrete.
The planks and structure have to be checked for a number of conditions, any of which could be critical:
1) At transfer, where the prestress force is at its highest and the concrete strength at its lowest.
2) During handling and construction, where the plain plank is subject to dynamic and superimposed loads.
3) Under service loads before shrinkage and creep have taken effect.
4) Under service loads after the effect of long-term shrinkage and creep.
5) At the limit state, where the structure approaches collapse.
Additionally, thought must be given to the differential shrinkage between the topping and the planks, and provision must be made for the planks to shorten lest the prestress force disappears into the supporting structure.
Basic principles
Clause 8.1.2.1 of AS 3600 states Calculations for strength of cross-sections in bending, or in bending combined with axial force, shall incorporate equilibrium and strain-compatibility considerations and be consistent with the following assumptions:
(a) Plane sections normal to the axis remain plane after bending.
(b) The concrete has no tensile strength.
(c) The distribution of compressive stress is determined from a stress-strain relationship for the concrete.
(d) The strain in compressive reinforcement does not exceed 0.003.
A typical stress-strain relationship for two grades of concrete is shown in Figure 1, reproduced from Clause C6.1.4 in AS 3600 Supplement 1.
Stresses in a homogeneous section due to prestress
Figure 2(a) shows the cross-section of a hypothetical precast plank. If prestress is applied at the centroid of this section, the stress pattern shown in Figure 2(b) will result, so that
f = -P/Ag where f is the average stress, P is the prestress force and Ag is the gross area of the plank.The same prestress force located at a level so that the resultant stress in the top fibre is zero (Figure 2(c)) will lead to a stress in the bottom fibre twice the average stress calculated above. The level at which the prestress is then located is said to be the lower kern line (kern is German for core and defines an area inside which an applied compressive force would cause no tensile stresses anywhere in the cross-section).
If we locate the prestress force below the lower kern line, we get a rapid increase in compressive stress in the bottom fibre and a tensile stress in the top fibre as shown in Figure 2(d). The magnitude of these stresses is:
[Equ. 1]
ft = -P/Ag + P.e/Ztf
b = -P/Ag - P.e/Zb (compression -ve)where e is the offset of the prestress force from the centroid of the section (+ve if below), Z is the modulus of section at the top and bottom fibre respectively and the other values are as previously defined.
Stresses in a homogeneous section due to applied moments
An applied moment M (+ve if it causes tension in the bottom) will produce stresses in the top and bottom fibre of a homogeneous section equal to:
[Equ. 2]
ft = -M/Zt and fb = +M/ZbDeformation at transfer
A precast plank which has tendons located below the centroid of the section will want to hog upwards when the prestress is transferred to it. This hogging effect means that the selfweight of the plank will immediately come into play. Whether the resultant effect will be a hog depends on the location of the tendons. If the superposition of the stresses due to prestress and due to part or all of the selfweight result in an average stress pattern as shown in Figure 2(b), then the plank will remain level, otherwise, it will hog.
The program assesses the combined effect of selfweight and prestress, taking into account the load factors given in Clause 3.3.1 ... Where applicable, the prestressing force, P, shall be included with a load factor of unity in each load combination, except for the case of dead load plus prestress at transfer, when the more severe of -
1.15G + 1.15P; and
0.8G + 1.15P
shall apply.
If only part of the selfweight acts while the plank is still in the stressing bed, then the plank will deflect when it is lifted. The program calculates the initial hogging or this deflection as follows:
1) It determines the true selfweight of the plank and uses this instead of any value specified in Analysis.
2) It sets the load factor for the selfweight to 0.8 if the prestress force is below the centroid, and to 1.15 if it is above the centroid of the plank.
3) It calculates the net deflection thus:
[Equ. 3] d
= (5w.L4/384 - P.e.L2/8)/Em.I, whered is the deflection (-ve if upward hogging)
w is the factored selfweight
L is the cut-off length of the plank
P is 1.15 times the prestress after cut-off losses
e is the offset of the prestress below the plank centroid
E
m is the modulus of elasticity of the concrete at transferI is the moment of inertia of the plank.
It should be noted that the cut-off length is not necessarily the in-service span, for example, if cantilevers are specified at one or both ends, the cut-off length equals the span plus the cantilever(s). Since cut-off usually takes place before 28 days, the modulus of elasticity at transfer is arbitrarily reduced to the value shown in Design Parameters. If a different value applies, the results displayed in Custom Design may be simply ratioed.
Stresses at transfer
Clause 8.1.4.2 stipulates a maximum compressive stress at transfer of
0.5fcp, where fcp is the compressive strength of the concrete at the time. With w being the factored selfweight and L the cut-off length as discussed above, the applied moment M = w.L2/8 is inserted into Equation 2. Stresses calculated from Equation 1 and Equation 2 are superimposed and the results displayed in Selection.Cut-off should not take place until the concrete has attained a compressive strength of at least twice this value.
Crack control
Clause 8.6.2 of AS 3600 states Flexural cracking, in a prestressed beam, shall be deemed to be controlled if, under the short-term service loads, the resultant maximum tensile stress in the concrete does not exceed 0.25Ö f'
c or, if this stress is exceeded, by providing reinforcement or bonded tendons, or both, near the tensile face and limiting either -(a) the calculated maximum flexural tensile stress under short term service loads to 0.6Ö f'
(b) both -
(i) the increment in steel stress near the tension face to 200 MPa, as the load increases from its value when the extreme concrete tensile fibre is at zero stress to the short-term service load value; and
(ii) the centre-to-centre spacing of reinforcement, including bonded tendons, to 200 mm.
Clause 3.4, Load Combinations for Serviceability Design, refers only to deflections. It is assumed that the same short-term load factors apply also to Clause 8.6.2 and the values displayed in Selection are based on this assumption.
It should be noted that the program displays, in addition to the compressive stress at transfer, the tensile stress at transfer, which often exceeds the applicable limit of 0.25Ö f'
c (the higher limit of 0.6Ö f'c does not apply unless the planks are also reinforced in the top, which is not usually the case). Whether transfer stresses should be treated as short-term service loads is open to question.The programmed procedure for arriving at the percentage by which the permissible stress covers the actual stress under service loads, displayed in Selection, is as follows:
1) The permissible stress is taken to be 0.6Ö f'
2) The prestress force is calculated at 0.5f
p, where fp is the tensile strength of the tendons. This is the expected load in the tendons after 30 years and has the more severe effect.3) Gravity loads are taken with a load factor of 1.0.
4) Live loads that would reduce the stress are ignored and other live loads are taken with a load factor of Psi-s, corresponding with Psil-l specified in Design Parameters thus: 0.7 if Psi-l <= .4, otherwise 1.0.
5) The maximum moment in the span is calculated taking into account cantilevers and end fixity as specified in Analysis.
6) Stresses resulting from this moment are calculated using Equation 2 and superimposed with the stresses from Equation 1, where the section values Z and e are based on the composite section of plank and topping as described next.
Composite section
Several questions arise when precast planks are combined with in-situ topping to form a composite section:
1) What is the effect of differential shrinkage? Refer to Topping reinforcement for a comment on this.
2) How effective is the interface between plank and topping? Refer Longitudinal shear for comments.
3) The question that concerns us here is: What are the properties of the composite section?
Frequently, the in-situ topping has a modulus of elasticity that is different from the plank. The answer can be found by examining the stress-strain relationship when a moment is applied to the composite section.
The diagram at left shows a typical stress state before the application of the moment.
The strain resulting from the moment is based on the basic principle that plane sections remain plane.
The resultant stress pattern to be added to the original stresses reflects the difference in concrete grades.
Consider the cross-section divided into horizontal elements. Each element has these properties:
y is its position from an arbitrary level located at a distance a from the bottom fibre;
b is its width (for example the sum of webs) at this level;
s is the stress in the element;
dy is the thickness of the element.
Two equilibrium conditions must be satisfied:
1) The sum of internal stresses must be zero -
This equation is satisfied only if the distance a is the centroid of the section, where the topping is taken at the ratio of E
tpg/Eplk.2) The internal moment must equal the applied moment -
The part in square brackets is the moment of inertia of the composite section, where the topping is taken at the ratio of E
tpg/Eplk, and e b.Eplk is, of course, fb, so that Equation 2 holds true: fb = M.a/I = M/Zb.Strictly speaking, the tendons and topping reinforcement could have been added at (n-1) times their respective areas, where n is the ratio of E
st/Eplk, but the omission of this is on the safe side.Topping reinforcement
Clause 9.4.3 of AS 3600 states The area of reinforcement required to control cracking due to shrinkage and temperature effects shall take into account the influence of flexural action, the degree of restraint against in-plane movements and the exposure classification. Clearly, the plank forms an effective restraint against in-plane movement in the topping. Assuming that a strong degree of control over cracking is required, the minimum area of reinforcement in the topping is
2500.D/fsy in mm2/m, where D is the topping thickness and fsy the yield strength of the steel.This requirement is satisfied by welded mesh to AS 1304 with a minimum yield strength of 450 MPa as follows:
Topping Minimum Nearest Actual
thickness area mesh area
30 166.7 F62 155.8
60 333.3 F92 317.9
90 500.0 F81 502.4
What happens to the original stresses?
The previous statement that the resultant stress pattern is to be added to the original stresses is an over-simplification. In reality, the original stresses adjust themselves to the composite section through creep. To assess this adjustment, let us imagine:
(i) That the plank and topping are prestressed together. Call this the natural stress state.
(ii) That the original stress state is induced by an external load superimposed on the natural state.
How much of the external load remains after creep?
Each element of the composite section is at a different extension in these two states (Figure 5(c)). The stress differential between the two states is D
f. This stress differential causes the element to creep. The creeping causes the stress differential to be reduced.If we divide the total creep into n equal slices, we can assess the effect in each period, where f is the creep factor:
first period- beginning stress differential
= D freduction D D
f1 = D f.f /nending stress
= D f.(1-f /n)second period- reduction D D
f2 = D f.(1-f /n).f /nending stress
= D f.((1-f /n)-(1-f /n).f /n)= D f.(1-f /n)
2by analogy
nth period- ending stress
= D f.(1-f /n)nBy taking n to infinity, this equation reduces to-
ending stress D f¥ = D f.e
-f , in other words, only a small part (0.6% to 13.5%) of the original stress differential remains:concrete grade 20 25 32 40 50
creep factor f
cc.b 5.2 4.2 3.4 2.5 2.0stress multiplier e
-f .006 .015 .033 .082 .135