Bearing and anchorage zones – Partially loaded areas

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When designing concrete structures, we meet two large groups of partially loaded areas (PLA) – the first of these comprises bearings, while the other consists of anchoring areas

According to currently valid standards for the design of reinforced concrete structures ACI 318-19 chap. 22.8, local crushing of concrete and transverse tension forces should be considered for bearings. For a uniformly distributed load on an area, Ac1, the compressive capacity of concrete may be increased by up to two times depending on the design distribution area Ac2. See the ACI 318-19 table 22.8.3.2.

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\[ \textsf{\textit{\footnotesize{Fig. 49\qquad Partially loaded areas for bearings according to ACI 318-19}}}\]

For post-tensioned anchorage zones, the following should be followed ACI 318-19 chap. 25.9.

The partially loaded area must be sufficiently reinforced with transverse reinforcement designed to transmit the splitting forces that occur in the area. Without the required transverse reinforcement, it is not possible to consider increasing the compressive capacity of the concrete.


Partially loaded areas in CSFM

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\[ \textsf{\textit{\footnotesize{Fig. 50\qquad Fictitious struts with concrete finite element mesh.}}}\]

Using CSFM, it is possible to design and assess reinforced concrete structures while including the influence of the increasing compressive resistance of concrete in partially loaded areas. Because CSFM is a wall (2D) model and the partially loaded areas are a spatial (3D) task, it was necessary to find a solution that combines these two different types of tasks (Fig. 50). If the “partially loaded areas” function is activated, the allowable cone geometry is created according to the ACI (Fig. 49). All geometric collisions are solved fully in 3D for the specified concrete member geometry and the dimensions of each PLA. Subsequently, a computational model of the partially loaded area is created.

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\[ \textsf{\textit{\footnotesize{Fig. 51\qquad Allowable cone geometries.}}}\]

The modification of the material model proved to be an unsuitable approach, which was mainly because the mapping of properties to the finite element mesh is problematic. It was determined that an approach independent of the finite element mesh is a more appropriate solution. Absolutely coherent fictitious struts are created for the known compression cone geometry (Fig. 51 and Fig. 52). These struts have identical material properties to the concrete used in the model, including the stress-strain diagram. The shape of the cone determines the direction of the struts, which gradually distributes the load over the PLA to the design distribution area. The area density of the fictitious struts is variable at each part of the cone, and it adds a fictitious concrete area in the load direction. At the level of the loaded area (Ac1), a fictitious area of concrete is added according to the ratio \(\sqrt{A_{c1} \cdot A_{c2}} - A_{real}\)  (where Areal is an area of the support assumed in the 2D computational model), and this area decreases linearly to zero towards the design distribution area (Ac2). This solution ensures that the compressive stress in the concrete is constant over the entire cone volume.

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\[\rho \left( {\beta ,z} \right) = \left( {\sqrt {\frac{A_{c2}}{A_{c1}}}  - \frac{A_{real}}{A_{c1}}} \right)\,\cdot\,\left( {1 - \frac{z}{h}} \right)\,\cdot\,\frac{1}{{\cos \beta }}\]

\[ \textsf{\textit{\footnotesize{Fig. 52\qquad Fictitious struts in the computational model}}}\]

The resistance of the partially loaded area is increased according to the ratio of the design distributed area and the loaded area laid in ACI 318-19 chap. 22.8.  It should be remembered that this is a design model that cannot precisely describe the stress state over a partially loaded area whose actual flow is much more complicated. However, this solution allows the correct distribution of load to the whole model while respecting the increased load capacity of the partially loaded area. In addition, it correctly introduces transverse stresses in this area to correctly design reinforcement for splitting forces.

The permissible bearing stress of 0.85fc' is listed in Table 22.8.3.2. The density is limited so that the maximum double capacity given in the formula in Table 22.8.3.2(b) is not exceeded.  

For the anchorage zones, PLA is used in the same way as for bearings in the application. That is why the local zones defined in ACI 318-19 chapter 25.9 must checked according to the ACI 318-19 25.9.3 manually. The PLA is, therefore, only used to avoid exceeding strain criterion in the local zone and thus prematurely stopping the calculation. On the other hand, according to ACI 318-19, Cl. 25.9.4.3.1 (b), reinforcement resisting the bursting and spalling in-plane stresses can be directly and advantageously verified in the application.

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