Abstract

A symmetrical isolated rectangular footing with centered biaxial overturning develops soil pressure that shifts to counter balance the loads. The highest soil pressure is at a corner. The objective of this paper is to extend the uniaxial soil pressure solution to include biaxial loads and to document a simple and understandable way to directly calculate the shape of the soil pressure distribution. Another objective is to make the solution suitable for automation. In uniaxial overturning there are two transition shapes, trapezoidal and triangular. In biaxial overturning there are three transition shapes and they form 4, 5 & 6 sided polyhedrons. This analysis calculates those volumes and compares them to the design vertical load to determine the characteristic shape of the soil pressure distribution. The calculation then proceeds to converge on the precise shape and calculate its centroid and moment capacity. Assemblies of tetrahedrons are used to model all of the soil pressure shapes. The advantage of this methodology is that matrix algebra can be used to organize the calculations and make them computationally efficient. The assumed soil pressure and footing dimensions can be adjusted until the calculated moment capacity matches the overturning moment.

Highlights

  • A symmetrical isolated rectangular footing with centered biaxial overturning loads develop soil pressure that shifts to counter balance the loads

  • The range of volumes through all transitions is from uniform soil pressure and no overturning on the high end, to small tetrahedrons with highest possible eccentricities on the low end

  • When the footing vertical load is compared to the range of possible volumes, the characteristic soil pressure shape for the footing is found

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Summary

Introduction

A symmetrical isolated rectangular footing with centered biaxial overturning loads develop soil pressure that shifts to counter balance the loads. Equation 1 is used to compute the fictitious pressures at the corners as if tension across the soil footing contact plane could exist. The moments create highest soil pressure at the corner labeled 1. The axis of zero soil pressure is located on the basis of pressures calculated from Equation 1. Including the moments of inertia accounts for the tendency of the footing to roll toward the weak axis. This is most evident for a footing with significant differences in the dimensions of L and W. For a square footing with length and width the same, the axis of zero soil pressure is aligned perpendicular to the moment vector

Uniaxial Overturning Soil Pressure
Biaxial Overturning
Maximum Soil Pressure
Calculation Method
Transition volumes
Transition Volume 2
Transition Volume 3
Soil Pressure Solutions
Tower Footing
Bridge Pier
Conclusion
Full Text
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