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Strut-and-Tie Method (MBT)

The model of Santos, Marquesi & Stucchi (2015), published in IBRACON's Comentários Técnicos e Exemplos de Aplicação da ABNT NBR 6118:2014 (technical commentaries and worked examples on NBR 6118:2014).

It arose from a concrete need: the 2014 revision of NBR 6118 introduced strength limits for nodes and struts that did not exist before, and those limits are lower than those of Blévot's method. A cap that passed by Blévot might not pass the code — and a method was missing that reconciled the two without the excessive conservatism of Fusco's method.

MBT combines Blévot's classic model with Fusco's load spreading concept.


The spreading problem

In Blévot, the vertical projection of the strut is the effective depth \(d\), and the column dimension enters through a tabulated term.

MBT looks at the node under the column. The load does not enter the cap through the exact area of the column: it spreads as it penetrates the concrete, at 45°, and the effective compression area grows with depth. The strut starts at the point where the stress over this enlarged area drops to the resisting limit.

Calling this depth \(y\), the enlarged area is

\[ A_{amp} = (a_p + 2y)\,(b_p + 2y) \]

and the internal lever arm becomes

\[ z = d - \frac{y}{2} \]

The difference in geometry, in one sentence

Blévot defines the tangent of the angle by the ratio \(d/L_{proj}\); MBT defines it by \(z/L_{proj}\), with \(z = d - 0.5y\).

Since \(z < d\), the MBT strut is flatter than Blévot's — and the tie is more heavily loaded, so there is more reinforcement.

The width of the strut in the node region comes from

\[ a_{bie} = \frac{a_p}{2} + y\cos\theta \qquad\text{or}\qquad a_{bie} = \frac{a_{p,amp}}{2}\,\sin\theta \]

The two nodal limits, and they are different

This is the point most often got wrong. NBR 6118 (item 22.3.2) defines different limits depending on the node type:

\[ \sigma^{bie}_{cd,pilar} = \frac{F_{d,pilar}}{A_{amp,pilar}\,\sin^2\theta} \;\le\; f_{cd1} \]
\[ \sigma^{bie}_{cd,est} = \frac{F_{d,est}}{A_{amp,est}\,\sin^2\theta} \;\le\; f_{cd3} \]

with

\[ f_{cd1} = 0.85\,\alpha_{v2}\,f_{cd} \qquad f_{cd3} = 0.72\,\alpha_{v2}\,f_{cd} \qquad \alpha_{v2} = 1 - \frac{f_{ck}}{250} \]
Node Type Forces acting on it Limit
Under the column CCC Compression only \(f_{cd1} = 0.85\,\alpha_{v2}f_{cd}\)
Over the pile CCT Two compressions and one tension \(f_{cd3} = 0.72\,\alpha_{v2}f_{cd}\)

The pile node allows 15 % less stress

It is the tie that makes the difference: the node over the pile anchors the tension reinforcement, and the tension cracks the concrete in the nodal region, reducing the compressive stress it can bear.

Using \(f_{cd1}\) at both nodes — the easy mistake — overestimates the capacity of the pile node by 18 %. In a cap where the pile governs, it is the difference between passing and failing.

The strength of the node under the column is adopted, on the safe side, as the value from item 22.1 of NBR 6118 for the CCC node, regardless of the number of piles.


The iterative procedure

Since the stress depends on \(\sin^2\theta\), and \(\theta\) depends on \(y\), there is no closed-form solution. The procedure is:

  1. Adopt a value of \(y\) — for example, \(y = 0.2d\).
  2. Determine the inclination of the strut, with \(\theta \ge 45^\circ\) desirable.
  3. Check the compressive stress at the node under the column.
  4. If it is not equal to the strength limit, iterate \(y\) until the design stress equals the resistance.
  5. Determine the final inclination of the strut and the main reinforcement over the piles.
  6. Check the compressive stresses at the nodes over the piles.
  7. Determine the distribution, skin and other secondary reinforcement.

PCO automates steps 1 to 4: it searches directly for the \(y\) at which the stress at the column node equals \(f_{cd1}\).

Three restrictions of the method

  1. The spreading is always at 45°. The method does not allow another inclination, and the program does not let you change it.
  2. In caps on two piles, spreading occurs only in the longitudinal direction of the cap.
  3. The strut starts from the centre of the original column's sub-area, at height \(y/2\).

The limit on y

Spreading does not grow indefinitely: it is confined by the dimensions of the cap.

\[ a_p + 2y \le 0.85\,L_{x,bloco} \qquad b_p + 2y \le 0.85\,L_{y,bloco} \]

Why not 0.4d

A limit \(y \le 0.4d\) appears in the literature, often quoted as if it were part of MBT. It is not: it comes from another formulation.

What MBT recommends is to control the depth of the neutral axis, in the same way as is done in bending to ensure plastic deformation capacity. The criterion indicated in the preliminary studies is

\[ \frac{y}{d} \le 0.3 \]

The method's assumption is that the ULS is reached when the strength of the upper node and the resisting force of the reinforcement are exhausted at the same time — and this is only appropriate if the lower node over the pile, or the strut, does not exhaust its strength first.


Blévot or MBT?

Blévot & Frémy MBT
Tangent of the angle \(d / L_{proj}\) \(z / L_{proj}\), with \(z = d - 0.5y\)
Column dimension Sub-area \(a_p/4\) Area enlarged by 45° spreading
Limit at the column node \(\alpha_{lim} K_R f_{cd}\) — 1.4 to 2.1 depending on the no. of piles \(f_{cd1} = 0.85\,\alpha_{v2}f_{cd}\)
Limit at the pile node The same \(f_{cd3} = 0.72\,\alpha_{v2}f_{cd}\)
Reinforcement Less; with a 15 % increase in two-pile caps More, in general
Backing 116 tests of its own IBRACON Commentaries on NBR 6118

How to choose

MBT is the model aligned with the IBRACON Commentaries on the current code, and it builds the node check into the lever arm calculation itself. If you need to justify the design against the current NBR 6118, it is the direct route.

Blévot remains useful as a reference and an order-of-magnitude check — it is the method with which most of the built stock was designed.

MBT produces more reinforcement than Blévot in most cases. The exception may occur precisely in caps on two piles, because of the 1.15 factor Blévot applies there.

Comparison with tests

The ratio between measured and predicted failure load, over the set of tests analysed by Santos et al.:

Method Mean Coefficient of variation
Blévot 1.19 0.21
MBT (Santos et al.) 1.21 to 1.23 0.19 to 0.20
Fusco 1.49 0.17

MBT has a safety level equivalent to Blévot's, with slightly lower scatter. Fusco is much more conservative, because of the vertical stress limit in the pile region.


Limits of validity

Range of application

  • Valid for a rigid cap, like Blévot.
  • The search for \(y\) caps at the geometric limit. When it caps without the stress dropping to the limit, the cap does not have the geometry for the load: the way out is to increase the depth, the column section or \(f_{ck}\) — not the reinforcement.
  • The 45° spreading is an idealisation. The real stress field is curved, and that is what the finite element model lets you check.
  • The NBR 6118 node and strut limits were established for planar elements and do not account for the confinement present in a three-dimensional cap. That is why they are conservative here — Blévot observed struts failing at stresses above 150 % of the mean concrete strength, an effect of the confinement produced by cage detailing.
  • Based on that observation, Santos et al. propose removing the \(\alpha_{v2}\) factor in the upper node check for caps with four or more piles. PCO does not adopt this proposal: it keeps \(\alpha_{v2}\), which is the code text.