ANALYSIS OF SETTLEMENT OF FOUNDATION PLATES BY FINITE DIFFERENCE METHOD.
Prskalo, Maja ; Vrdoljak, Anton
ANALYSIS OF SETTLEMENT OF FOUNDATION PLATES BY FINITE DIFFERENCE METHOD.
1. Introduction
To do the high-quality calculation and reliable performance of the
foundations of the building, it is necessary, among other things, to
resolve the interaction of the object, foundations and soil during all
phases of construction. In all these cases, if the foundation feet are
too close, or if they overlap, or if we have to reduce the differential
settlement, we have to determine for the foundation plates. The
mechanical properties of the soil are very complex and the solution to
the problem of interaction between foundation soil with the structural
elements requires certain simplifications, because without them the
problem will be unsolvable or economic unprofitable. With this in mind,
the greatest number of solutions is developed for the soil as linearly
elastic, homogenous and isotropic half-space [5]. These simplifications
and the improvement of the computer technology allow us the use of the
numerical methods for calculation of the stress as well as for
settlement of foundation plates [4]. In this paper we will use finite
difference method (FDM), the oldest numerical method for solving partial
differential equations [3], [4].
2. Previous research
Various theoretical and numerical procedures are developed to
obtain approximate solutions of real distribution of stresses in a
structure-soil interface. A practically reasonable approximation of the
actual state is achieved by developing numerical procedures and
thoroughly investigating deformation properties of soil [7].
The problem of numerical resolution of partial differential
equations, or finding and/or improving the algorithms for solving them
is studied in numerical analysis--a branch of numerical mathematics. The
most famous numerical method for solving such problems is the finite
difference method (or mesh method) which idea is to approximate the
derivatives of function (of one or more variables) with the divided
differences. There are several other methods in use, such are
collocation method, Galerkin method, Ritz method and finite element
method.
Finite difference method replaces the main differential equation
with the system of algebraic equations that links shifts of observed
points relative to neighbouring points. These points are distributed in
a grid/mesh of the surface of the plate. The method was first formulated
(introduced) by Allen and Severn, and is described in different
publications.
3. Numerical method--finite difference method
Finite difference method replaces the main differential equation
with the system of algebraic equations that links shifts of observed
points relative to neighbouring points. It is placed in every point of
the grid/mesh on the surface of the plate, thus a system of algebraic
equations is formed, the system based on a rectangular coordinate
system, and on a load, as well as on the physical and elastic constants
of the loaded plate. This load-deformation equation establishes a linear
relationship between the load at the focal point and the unknown value
of the deformation of the plate at that point, but in the other active
points too, so by solving these equations the approximate values of the
deformation of the plate in the active points of the mesh are obtained.
Refinement of the mesh will result with increasing of the order for
matrix of the system, and with growing of the complexity for the
algorithm which would be almost impossible to solve without using a
computer [1].
Figure bellow is showing a division/distribution of the surface of
the plate with grid lines, what is resulting with rectangular elements
of the grid/mesh. In direction, we are having a interval between grid
lines h, and rh in x direction. Places of intersecting for two grid
lines we will call grid/mesh points. Some of them are marked with
letters (N, E, S, W, ...) and are called active points, and a
central/middle point of an active group of points is called the focal
point (Z). To simplify the writing of equations, the marks of the active
grid points are used also as the size of settlement w, and the middle
plains are observed in specific grid point on the plate.
By using a standard procedure of finite difference method, then by
including a value of deflection of the plate in the form of designation
of active grid points and finally by arranging, the Lagrange
differential equation will translate into the following equation:
[mathematical expression not reproducible] (1)
Equation (1) is the basic load-deformation relation to any internal
active point. Next, this general form of the equation is being used for
special cases which involving the boundary cases, as well as for all
relations connecting the deformation of the plate with the loads,
momentums, reactions and shear [2]. Essentially, this load-deformation
equation establishes a linear relationship between the load at the focal
point and the unknown value of the deformation of the plate at that
point, but in the other active points too, so by solving these equations
the approximate values of the deformation of the plate in the active
points of the mesh are obtained.
4. Determination for the modulus of soil reaction
The foundation of the building/object is defined as an integral
part of the structure that is in direct contact with soil or rock massif
and which receives and transmits the load from the building to the
soil/ground or rock massif. Due to object's load the soil is being
deformed, and while deformed it returns the reactive load to the
building structure. The soil and the structure of the building are being
deformed together, which is why it is necessary to consider
projecting/designing the foundations together with the construction of
the building and vice versa. Their mutual consideration and design leads
to more favourable technical and economic solutions for entire
building/object [8]. During the analysis of the foundation plate, the
soil can be observed in two ways:
* as a group of springs, according Winkler's theory;
* as a continuum, which is usually observed as elastic half-space.
The modulus of soil reaction can be determined in the following
ways:
* by using circular plate;
* by using a table of typical values and correlations;
* by calculating of settlement.
The usual way of obtaining for modulus of soil reaction is by
applying loads to the soil through a circular plate with a diameter of
30 cm. The disadvantage of this method is regarding the load, but only
for the layer of lower thickness (lower in comparison to the layer
loaded with the foundation plate). The modulus of soil reaction can also
be estimated on the basis of predicted settlement for real foundation.
In this case it can be assumed that the foundation is solid and under
pressure corresponding to the total load on the foundation. The
settlement is projected by standard methods of soil mechanics. In this
case, the modulus of soil reaction we can calculate as follows:
k = [bar.q]/[bar.w] (2)
where [bar.q] is average pressure, and [bar.w] is settlement for
solid foundation.
This procedure can take into account the different layers exposed
to different levels of stress, what was not possible in the previous
known methods. In addition, thanks to short-term and long-term
predictions for the settlement, we are able to get modules for
short-term and long-term analysis of the behaviour of the foundation,
taking into account both, the consolidation and creep of soil. It is
difficult to find a relation between k and Young's modulus for
elastic half-space because the answer depends on the stiffness of the
foundation itself. Such a relation is obtained by equating the
settlement of solid plate in homogeneous elastic half-space, with the
settlement of the same plate on Winkler's springs. It follows:
k = 1/B x [I.sub.B] (E/1 - [v.sup.2]) (3)
The modulus of soil reaction is not constant value, but depends on
the quantity of the load (p), and on the shape and the size of the
loaded test plane. Terzaghi is suggesting the values for the modulus of
soil reaction ([k.sub.1]), for test surface 30 cm x 30 cm and for
different types of soil and its compaction (1955), which are given in
table (1). In a case of larger test areas, Terzaghi is proposing
corrections in the form of [6]:
* for incoherent soil:
k = [k.sub.1] [(B' + 1/2B').sup.2] (4)
* for coherent soil:
k = [k.sub.1]/B (5)
where
B' = B/30.3,
and B is width of the foundation (cm).
The following examples will demonstrate the results of calculations
for foundation foot and foundation plate for different types of soil,
with an accent on their maximum settlements. In these calculations we
used the modified program code, which is initially developed by Salar
Delaware Ghashghaei in Matlab [9].
First example is an example of a foundation foot with the following
characteristics:
[L.sub.x] = 120 cm, [L.sub.y] = 120 cm, h = 100 cm, E = 2.1 x
[10.sup.5] MPa, v = 0.20,
and the results of calculations are represented with table 2 and
figure 3.
Second example is an example of a foundation plate, with dimension
500 cm x 500 cm, height h = 100 cm, and with total load/force
distributed symmetrically in four ultimate points of internal network.
For this example, the results of calculations are represented with table
3 and figure 4.
5. Conclusion
Examples of calculations for foundation plates, taken from practice
and references, shows differences in accuracy for some numerical methods
in the analysis of stresses and deformations/strains. In most of
calculations the compressible soil is replaced with the system of
elastic springs, which are deformed just below the loaded part of the
plate. This model is not entirely satisfactory because deformations in
real soil are spread beyond the loaded parts, but is still very widely
used because the analytical solutions of differential equations is
relatively simple, and the results are more realistic than those
obtained with the assumption of linear distribution of soil reaction.
Furthermore, in this model are not considered elongations (stresses) due
to temperature.
By summarizing our results we obtain that finite difference method
gives results similar to those obtained with the finite element method,
but the contours of the bending moments obtained with finite difference
method are less smooth than those obtained with finite element method.
The density of the network has an impact on the results of each of the
numerical methods. The higher density gives smoother diagrams of bending
moments and deformation of the foundation plate. Our examples with
calculations made by using modified Matlab program code, and their
results, indicates that plate' settlement is less dependent on the
change of modulus of soil reaction, as well as that the maximum values
of those settlings are less than the values of settlings for foundation
foot. These benefits and reduction of differential settlements are the
most common reasons for selection of the foundation plate as a way of
foundation of the building. The focus of further study has to be on
including temperature strains, as well as dynamic load in calculations.
DOI: 10.2507/27th.daaam.proceedings.123
6. References
[1] Hemsley, J. A. (2000). Design applications of raft foundations,
Thomas Telford Publishing, London
[2] Moody, W. T. (1990). Moments and reactions for rectangular
plates, U.S. Government Printing Office, Washington
[3] Scitovski, R. (2004). Numerical mathematics, Department of
Mathematics, University of Osijek, ISBN 953-6032-24-4, Osijek
[4] Bowles, J. E. (1974). Analytic and computer methods in
foundation engineering, McGraw-Hill Inc., US, ISBN 978-0070067530, New
York
[5] Aron, C. & Jonas, E. (2012). Structural element approaches
for soil-structure interaction, M.Sc. Thesis, Department of Civil and
Environmental Engineering, Chalmers University of Technology, Goteborg,
Sweden
[6] Nonveiller, E. (1990). Soil mechanics and foundations of
buildings, Skolska knjiga, ISBN 978-8603996456, Zagreb
[7] Veric, F. (2000). Savitljive temeljne konstrukcije (Flexible
foundation structure), Authorized lectures, Faculty of Civil
Engineering, University of Zagreb, Institute of Geotechnics, Zagreb
[8] Roje-Bonacci, T. (2007). Posebna poglavlja temeljenja (Special
chapters of foundation), Faculty of Civil Engineering and Architecture,
University of Split, Split
[9] Matlab, The language of technical computing,
http://www.mathworks.com/products/matlab/
This Publication has to be referred as: Prskalo, M[aja] &
Vrdoljak, A[nton] (2016). Analysis of Settlement of Foundation Plates by
Finite Difference Method, Proceedings of the 27th DAAAM International
Symposium, pp.0854-0859, B. Katalinic (Ed.), Published by DAAAM
International, ISBN 978-3-902734-08-2, ISSN 1726-9679, Vienna, Austria
Caption: Fig. 1. The system of marking for the grid points
Caption: Fig. 2. Foundation foot on Winkler's springs with
stiffness k
Caption: Fig. 3. Diagrams of deflections for foundation foot on
elastic soil/base, obtained by finite difference method [9]
Caption: Fig. 4. Diagrams of deflections for foundation plate on
elastic soil/base, obtained by finite difference method [9]
Table 1. Examples of calculations for selected modulus of soil
reaction
Sand Incoherent Half- Coherent
coherent
1. Dry or wet 0.6-1.9 1.9-9.6 9.6-32
2. Partially 1.3 4.2 16
sunken
3. Sunken 0.8 2.6 9.6
Clay Consistency
Stiff Very stiff Solid
1. [q.sub.u] 100-200 200-400 > 400
(kN/[m.sup.2])
2. Limits 1.6-3.2 3.2-6.4 6.4
3. Partially 2.4 4.8 9.6
sunken
Table 2. Results of settlement' calculations for foundation foot
[k.sub.1] k
([10.sup.4] ([10.sup.4] [[delta].sub.mar]
Type of soil: kN/[m.sup.3]) kN/[m.sup.3]) (cm)
Incoherent sand 1.9 0.47975 -3.353
(dry or wet)
Coherent sand 32 8.08 -2.321
(dry or wet)
Clay with stiff 2.4 0.606 -3.326
consistency
Clay with solid 9.6 2.424 -2.986
consistency
Table 3. Results of settlement' calculations for foundation plate
[k.sub.1] k
([10.sup.4] ([10.sup.4] [[delta].sub.max]
Type of soil: kN/[m.sup.3]) kN/[m.sup.3]) (cm)
Incoherent sand 1.9 1279.3 -2.06
(dry or wet)
Coherent sand 32 19392 -1.55
(dry or wet)
Clay with stiff 2.4 14544 -2.05
consistency
Clay with solid 9.6 5817.6 -1.9
consistency
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