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Blévot & Frémy

The classic method for rigid pile caps, also called the Strut Method. It assumes a truss as the resisting model inside the cap: planar in caps on two piles, spatial in the others. The compressed members are resisted by the concrete — the struts — and the tensioned members by reinforcement — the ties.

It is the most widely used simplified method in Brazil, for three reasons: it has broad experimental support — 116 tests by Blévot & Frémy, among others —, it has an established tradition here and in Europe, and the truss model is intuitive.

When the method is recommended

  • The loading is nearly centred. It can be used for non-centred loading by assuming that all piles carry the highest load — which tends to make the design uneconomical.
  • All piles are equally spaced from the centre of the column.

The model, for a cap on two piles

The load \(N\) arrives through the column and goes down through two inclined struts to the piles. The force polygon gives the tension at the bottom and the compression in the strut.

The inclination of the strut is the parameter that governs everything:

\[ \tan\alpha = \frac{d}{\dfrac{e}{2} - \dfrac{a_p}{4}} \]

where \(d\) is the effective depth, \(e\) the distance between pile axes and \(a_p\) the column dimension in the direction of \(e\). The term \(a_p/4\) is the centre of the column's sub-area: the column is divided into as many parts as there are piles, and the load leaves from the geometric centre of each sub-area.

Hence:

\[ R_s = \frac{N}{8}\cdot\frac{2e - a_p}{d} \qquad\qquad R_c = \frac{N}{2\sin\alpha} \]

\(R_s\) is the tensile force in the tie and \(R_c\) the compression in the strut.

The general form

For any number of piles, the force in the tie is

\[ F_{td} = N_{d,estaca}\cdot\cot\theta \qquad\text{with}\qquad \cot\theta = \frac{L_{proj}}{d} \]

where \(L_{proj}\) is the horizontal projection of the strut — the distance from the centre of the load sub-area to the pile axis. In a symmetric cap on four piles, \(L_{proj} = \left(\dfrac{\ell}{2} - \dfrac{a_p}{4}\right)\sqrt{2}\).

In caps on three or more piles, \(F_{td}\) is resolved into the directions of the reinforcement.

The formulas for each arrangement

This chapter develops the cap on two piles, where the geometry is clearest. The closed-form expressions for three to seven piles — with their effective depth ranges, stress limits and reinforcement — are in Formulas by arrangement.


Effective depth

The compressed struts present no risk of punching failure as long as the inclination stays within the tested range:

\[ 40^\circ \le \alpha \le 55^\circ \]

which bounds the effective depth to

\[ 0.419\left(e - \frac{a_p}{2}\right) \;\le\; d \;\le\; 0.714\left(e - \frac{a_p}{2}\right) \]

Machado (1985) recommends the narrower range \(45^\circ \le \alpha \le 55^\circ\), giving \(d_{min} = 0.5\left(e - a_p/2\right)\) and \(d_{máx} = 0.71\left(e - a_p/2\right)\).

The depth has a second constraint too

NBR 6118 (22.7.4.1.4) requires that the cap be deep enough to allow the anchorage of the column starter bars:

\[ d > \ell_{b,\phi,pil} \]

In a shallow cap with a heavily reinforced column, it is this condition that governs — not the strut inclination.

The total depth is \(h = d + d'\), with \(d' \ge \max(5\ \text{cm};\ a_{est}/5)\), where \(a_{est} = \dfrac{\sqrt{\pi}}{2}\,\phi_e\) is the side of the square pile with an area equivalent to the circular one.


Strut check

The strut area varies along the depth, so the two end sections are checked — at the column and at the pile:

\[ A_b = \frac{A_p}{2}\sin\alpha \quad \text{(at the column)} \qquad A_b = A_e \sin\alpha \quad \text{(at the pile)} \]

With \(R_{cd} = N_d/(2\sin\alpha)\), the stresses are:

\[ \sigma_{cd,b,pil} = \frac{N_d}{A_p \sin^2\alpha} \qquad\qquad \sigma_{cd,b,est} = \frac{N_d}{2\,A_e \sin^2\alpha} \]

\(\sin^2\alpha\) appears twice for the same reason: one projection converts the force to the strut direction, the other converts the area.

The limit, and the KR coefficient

\[ \sigma_{cd,b,lim} = \alpha_{lim}\,K_R\,f_{cd} \]
No. of piles \(\alpha_{lim}\)
2 1.4
3 1.75
4 or more 2.1

The limit increases with the number of piles because of confinement: the more piles, the more confined the concrete in the nodal region, and the higher the stress it can bear.

What KR is

\(K_R\) lies between 0.90 and 0.95 and is the coefficient that accounts for the loss of concrete strength over time due to sustained loads — the Rüsch effect.

It has nothing to do with the cap geometry or the tie reinforcement: it acts only on the stress limit. Adopting 0.90 is the conservative choice.

A failed strut is not fixed with reinforcement

If \(\sigma_{cd,b} > \sigma_{cd,b,lim}\), the concrete crushes. The way out is to increase the cap depth, enlarge the column section or raise \(f_{ck}\).


Main reinforcement

Blévot found in the tests that the force measured in the main reinforcement was 15 % higher than indicated by the theoretical calculation. That is why the tie is increased:

\[ R_s = \frac{1.15\,N}{8}\cdot\frac{2e - a_p}{d} \qquad\Longrightarrow\qquad A_s = \frac{1.15\,N_d\,(2e - a_p)}{8\,d\,f_{yd}} \]

The 1.15 factor is specific to caps on two piles

In caps on three or more piles this factor does not exist. There, instead of increasing it, \(F_{td}\) is resolved into the directions of the reinforcement.

Blévot proposed 1.15 so as not to obtain lower safety factors than those specified at the time.

Where the reinforcement goes

NBR 6118 (22.7.4.1.1) is explicit: the flexural reinforcement must be placed essentially — more than 85 % — within the strips defined by the piles, in equilibrium with the respective struts. The strips are 1.2 times the pile diameter wide.

The bars must extend from face to face of the cap and end in hooks at both ends. The anchorage is measured from the inner faces of the piles.

To estimate the length of a cap on two piles, with anchorage without hooks and \(\alpha = 0.7\):

\[ \ell_{bl,2} = e - \phi_e + 2\left(0.7\,\ell_b + c + \phi_\ell\right) \]

Complementary reinforcement

NBR 6118 (22.7.4.1.5) makes side and top reinforcement mandatory in caps with two or more piles in a single line.

Reinforcement Value
Top \(A_{s,sup} = 0.2\,A_s\)
Skin and vertical stirrups, per face \(\left(\dfrac{A_{sp}}{s}\right)_{min} = \left(\dfrac{A_{sw}}{s}\right)_{min} = 0.075\,B\) cm²/m

with \(B\) the width of the cap in cm.

Spacing:

  • Skin reinforcement: \(s \le \min(d/3;\ 20\ \text{cm})\), and \(s \ge 8\) cm as a practical recommendation.
  • Vertical stirrups over the piles: \(s \le \min\left(15\ \text{cm};\ 0.5\,a_{est}\right)\).
  • Vertical stirrups elsewhere: \(s \le 20\) cm.

Cap on one pile

A special case: the cap is a transfer element, needed because the base of the column does not match the pile area. The main reinforcement resists splitting, and consists of closed horizontal stirrups:

\[ T = \frac{1}{4}\,P\,\frac{\phi_e - a_p}{\phi_e} \cong 0.25\,P \qquad\qquad A_s = \frac{T_d}{f_{yd}} \]

The effective depth can be estimated at around \(1.0\) to \(1.2\,\phi_e\).


Limits of validity

Range of application

  • Valid for a rigid cap. In a slender cap the strut does not form in a defined way and the behaviour is bending — see flexible pile caps.
  • The tested range is \(40^\circ < \theta < 55^\circ\), with \(\theta \ge 45^\circ\) recommended. Outside it, the method extrapolates the experimental basis.
  • It assumes nearly centred loading and piles equally spaced from the centre of the column. With moments acting, the pile loads differ and the pure formulation does not apply: the practice is to adopt, as the equivalent vertical load, the reaction of the most heavily loaded pile multiplied by the number of piles — a conservative simplification.
  • The tests covered caps with up to six piles. High counts, an eccentric column or several columns extrapolate the experimental basis.
  • Blévot's stress limits are not those of the current NBR 6118. The 2014 revision introduced more restrictive nodal limits, and a cap that passed by Blévot may not pass them. See MBT and Checks.
  • Compared with tests, the method is slightly conservative: the ratio between measured and predicted failure load averages 1.19.