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Posted: October 23rd, 2024

Investigation into the Mobilised Bearing Capacity and Head Displacement of Energy Piles

An Investigation into the Mobilised Bearing Capacity and Head Displacement of Energy Piles

Abstract

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Energy piles offer a promising new method of reducing CO2 emissions by utilising geothermal energy to heat and cool buildings. Despite an increase in implementation over recent years a lack of understanding of energy pile behaviour due to thermal effects remains, with current designs either based upon the structural requirements alone or exacerbated safety factors. Existing literature has demonstrated that thermal loading has a significant impact on pile strains. However, little investigation has been conducted into the effect of thermal loading on the mobilised bearing capacity, or pile head displacements which are imperative to the design integrity of the pile and founded superstructure.

This dissertation aimed to assess if varying material properties and increasing thermal loads affect the pile factor of safety and head displacements. A parametric study was conducted where a finite element model, validated against a known field experiment, tested varying values of pile length, pile diameter, soil shear modulus and soil strength under thermal loading. The results of the testing indicated that while the factor of safety showed little variation, pile head displacements were quite sensitive to thermal loads. It was further demonstrated that pile length was the most critical property, as results showed the most significant trend in this data.

It is clear from this research that further industry understanding and formalised design codes are required for the design of energy piles, as the current approach does not account for the substantial change in pile head displacements indicated by this study.

Contents

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1 Introduction

2 Literature Review

2.1 Energy Piles

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2.2 Framework

2.3 Field Testing

2.4 Numerical Modelling

3 Numerical Model

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3.1 Model Description

3.2 Validation

4 Parametric Study

4.1 Analysis Arrangement

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4.2 Results

4.3 Critical Evaluation

5 Conclusion

6 References

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List of Figures

Figure 1: Annual Relationship between Surface Air Temperature and Ground Temperature, (Preene & Prowrie, 2009)

Figure 2: UK Energy Pile Installations 2005-10, (Laloui & Donna, 2011)

Figure 3: Typical Energy Pile Arrangement, (Laloui & Donna, 2011)

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Figure 4: Thermal Behaviour Pile Profiles (a) unrestrained heating (b) unrestrained cooling      (c) fixed heating (d) fixed cooling, (Bourne-Webb, et al., 2012)

Figure 5: Thermal Behaviour Pile Profiles (a) shaft restraint heating (b) shaft restraint cooling (c) shaft and end restraint heating (d) shaft and end restraint cooling, (Bourne-Webb, et al., 2012)

Figure 6: Mechanical Behaviour Pile Profile

Figure 7: Thermomechanical Behaviour Pile Profiles (a) shaft restraint heating (b) shaft restraint cooling (c) shaft and end restraint heating (d) shaft and end restraint cooling, (Bourne-Webb, et al., 2012)

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Figure 8: Strain Profiles (a) Lambeth College (b) Lausanne

Figure 9: T-z Beam Spring Method

Figure 10: T-z Load Transfer Curve

Figure 11: Lambeth College Test Pile, (Bourne-Webb, et al., 2009)

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Figure 12: Lambeth College Test Temperature Variation

Figure 13: Verification Mechanical Loading Results

Figure 14: Verification Heating Results

Figure 15: Verification Cooling Results

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Figure 16: Finite Element Results for E=40MPa

Figure 17: Finite Element Model Varying Properties

Figure 18: Test A – Strain Profiles (a) Heating (b) Cooling

Figure 19: Test A – Mobilised Shaft Friction Profiles (a) Heating (b) Cooling

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Figure 20: Test A – Pile Head Displacements due to Thermal Loading only

Figure 21: Test A – Factor of Safety

Figure 22: Test B – Pile Head Displacement due to Thermal Loading only

Figure 23: Test B – Factor of Safety

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Figure 24: Test C – Pile Head Displacements due to Thermal Loading only

Figure 25: Test C – Factor of Safety

Figure 26: Test D – Pile Head Displacement due to Thermal Loading only

Figure 27: Test D – Factor of Safety

Figure 28: Test E – Pile Head Displacements due to Thermal Loading only

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Figure 29: Test E – Factor of Safety

Figure 30: Test F – Pile Head Displacement due to Thermal Loading only

Figure 31: Test F – Factor of Safety

Figure 32: Test G – Pile Head Displacements due to Thermal Loading only

Figure 33: Test G – Factor of Safety

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Figure 34: Test H – Pile Head Displacement due to Thermal Loading only

Figure 35: Test H – Factor of Safety

Figure 36: Test I – Pile Head Displacement due to Thermal Loading only

Figure 37: Test I – Factor of Safety

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Figure 38: Test J – Pile Displacement due to Thermal Loading only

Figure 39: Test J – Factor of Safety

Figure 40: Test K – Pile Head Displacement due to Thermal Loading only

Figure 41: Test K – Factor of Safety

Figure 42: Test L – Pile Head Displacement due to Thermal Loading

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Figure 43: Test L – Factor of Safety

Figure 44: Test M – Pile Displacement due to Thermal Loading only

Figure 45: Test M – Factor of Safety

Figure 46: Test N – Pile Displacement due to Thermal Loading only

Figure 47: Test N – Factor of Safety

Figure 48: Test O – Pile Displacement due to Thermal Loading only

Figure 49: Test O – Factor of Safety

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Figure 50: Test P – Pile Head Displacement due to Thermal Loading only

Figure 51: Test P – Factor of Safety

Figure 52: Factor of Safety Change for Increasing Loading

Figure 53: Pile Head Displacement Change for Increasing Loading (a) 80% (b) 90%

Figure 54: Factor of Safety for Varied Pile Lengths

Figure 55: Pile Head Displacement under Thermal Loading Only for Varied Pile Lengths

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Figure 56: Factor of Safety for Varied Pile Diameters

Figure 57: Pile Head Displacement under Thermal Loading Only for Varied Pile Diameters

Figure 58: Factor of Safety for Varied Soil Shear Modulus

Figure 59: Pile Head Displacement under Thermal Loading Only for Varied Soil Shear Modulus

Figure 60: Factor of Safety for Varied Soil Strength

Figure 61: Pile Head Displacement under Thermal Loading Only for Varied Soil Strength

List of Tables

Table 1: Verification Model Loading

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Table 2: Verification Model Pile Properties

Table 3: Verification Model Soil Properties

Table 4: Model Varying Properties Values

Table 5: Parametric Study Constant Properties

Table 6: Test A – Input Values

Table 7: Test B – Input Values

Table 8: Test C – Input Values

Table 9: Test D – Input Values

Table 10: Test E – Input Values

Table 11: Test F – Input Values

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Table 12: Test G – Input Values

Table 13: Test H – Input Values

Table 14: Test I – Input Values

Table 15: Test J – Input Values

Table 16: Test K – Input Values

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Table 17: Test L – Input Values

Table 18: Test M – Input Values

Table 19: Test N – Input Values

Table 20: Test O – Input Values

Table 21: Test P – Input Values

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Table 22: Summary of Results

List of Symbols

GSHP Ground Source Heat Pump
αc Coefficient of thermal expansion
ΔT Temperature Change
εT-Free Unrestrained pile strains
εT-Fixed Fixed pile strains
εT-Obs Observed pile strains
εT-Rest Restrained pile strains
PT Thermal loading
E Young’s Modulus
A Pile cross-sectional area
kEL Local beam element stiffness matrix
kspring Local spring element stiffness matrix
t Shaft friction
z Pile displacements (t-z model)
tm,undrained Maximum shaft friction undrained soil
tm,drained Maximum shaft friction drained soil
α Soil adhesion factor
Su Soil undrained shear strength
As Area of pile in contact with soil
k0 Coefficient of earth pressure
ϕ’ Soil friction angle
σ’v Effective vertical soil stress
km Maximum stiffness for displacement
G Soil shear modulus
r Pile radius
L Pile length
ν Poisson’s Ratio
γ Unit weight of soil
h Hardening parameter
d Degradation parameter (t-z model)
k Global stiffness matrix
kp Global pile stiffness matrix
ks Global soil stiffness matrix
P Mechanical load
u Displacements
c’ Soil cohesion factor
d Pile diameter
Nc Empirical factor
Qult Ultimate pile bearing capacity
Qmob Mobilised pile bearing capacity
Ab Area of pile base

1                Introduction

Geothermal energy is heat which is stored within the ground. It is considered a good source of renewable energy and is receiving increasing interest with the ever-growing pressures regarding carbon reductions. One method of accessing this energy is with a ground source heat pump system (GSHP). The GSHP involves laying a series of tubes below the ground surface, which allow for the circulation of a fluid. As the ground remains at a constant temperature throughout the year, as shown in Figure 1, a transfer of heat energy takes place with the fluid heated or cooled depending on the seasonal surface temperature. This energy can be exchanged using a heat pump to meet the heating requirements of buildings.

Figure 1: Annual Relationship between Surface Air Temperature and Ground Temperature, (Preene & Prowrie, 2009)

A more recent innovation the integration of the GSHP with foundation piles. This system is termed ‘energy pile’ and, in theory, is an excellent idea as it utilises an element which is already structurally required, resulting in a significant reduction in construction costs.  This has led to an increase in energy pile installations in recent years, as shown in Figure 2.

Figure 2: UK Energy Pile Installations 2005-10, (Laloui & Donna, 2011)

However, concerns have been raised as to the effects of the heating and cooling cycles on the pile structure. Without a comprehensive understanding of the energy pile behaviour, it is hypothesised that the structure expansion and contraction associated with the temperature cycles may have a detrimental effect on the pile-soil interaction and the overall bearing capacity of the foundation.

This project aims to expand the current understanding of energy pile behaviour, specifically the effect of varied properties and temperature cycles on the mobilised bearing capacity and head displacements.  The objectives are detailed below:

  • Research current understanding of energy pile behaviour
  • Validate a finite element model against existing field data
  • Perform a parametric study using a finite element model in order to simulate energy pile behaviour under different parameters
  • Analyse produced results in order to form an understanding of the energy pile behaviour throughout testing

2                Literature Review

This section aims to explain current understanding of energy piles and identify gaps in the knowledge which require further study.

2.1          Energy Piles

Energy pile installation involves the incorporation of U-shaped tubes into the pile structure which is usually achieved by attaching them to the reinforcement, as shown in Figure 3Error! Not a valid bookmark self-reference..

Figure 3: Typical Energy Pile Arrangement, (Laloui & Donna, 2011)

This simple system has shown to produce 20-100W per m of pile of renewable heating energy, which is popular with developers as it assists in meeting the 10% on site renewable energy obligation enforced for medium and large scale developments in the UK (Laloui & Donna, 2011; Boennec, 2008). Despite a significant increase in the number of energy piles installed around the world, concerns remain regarding their structural integrity (Laloui & Donna, 2011). This stems predominantly from a lack of understanding in the behaviour of the piles during the heating and cooling cycles associated with their geothermal applications (Laloui & Donna, 2011). Furthermore, few design codes exist with those that do based upon limited field testing (Laloui & Donna, 2011). Today most energy piles are either designed based purely upon their structural requirements, or with significantly increased safety factors (Ouyang, et al., 2011; Abuel-Naga, et al., 2015). Neither approach specifically addresses thermal behaviour, leading to potentially dangerous or over conservative designs. Therefore, the development of standardised design practices and wider industry understanding is crucial for the successful widespread usage of energy piles.

2.2          Framework

A framework for the behaviour of energy piles was first suggested by Bourne-Webb et al. (2009) which was further developed by Bourne-Webb et al. (2012) and Amatya et al. (2012). Energy piles are subjected to two loads; mechanical and thermal. Mechanical loading is specified by the above ground superstructure, the traditional application of piles. Thermal loading induced by the heating or cooling effects associated with the geothermal applications. Each load has a specific effect on the behaviour of a pile and each will now be analyses separately before their combined effects are considered.

2.2.1         Thermal Loading

First, the pile response under thermal loading only is considered. If the pile is unrestrained it will expand or contract in proportion to the coefficient of thermal expansion (αc) and temperature change (ΔT):

εT-Free=αc∆T

           (1)

Thus, when the pile is heated (+ΔT) it expands and contracts when cooled (-ΔT). Similarly, under fully fixed conditions, where movement is restricted in all directions, thermal strains will be induced within the pile (εT-Fixed). Under heating conditions, where the pile wants to expand compressive strains will be induced and tensile strains will be induced where the pile wishes to contract under cooling, as illustrated in Figure 4.

εT-Fixed

εT-Fixed

Figure 4: Thermal Behaviour Pile Profiles (a) unrestrained heating (b) unrestrained cooling      (c) fixed heating (d) fixed cooling, (Bourne-Webb, et al., 2012)

However, in reality, a pile is unlikely to act either as a free body or fully restrained. It will be somewhere in between due to partially restrained conditions from the soil surrounding the pile. The degree of pile restraint will depend upon the individual site conditions, but it can be stated that:

εT-Free≥εT-Obs

(2)

where

εT-Obsrepresents the limited expansion or contraction of the pile under the partially restrained conditions. Therefore, it can be said that the restrained strains within the pile (resulting from the pile being unable to move freely) are expressed as:

εT-Rest=εT-Free-εT-Obs

(3)

The restrained strains will induce axial loading within the pile which is expressed as a function of pile cross sectional area, A, and Young’s Modulus, E:

PT=EAεT-Rest

(4)

Assuming that the temperature change is constant over the entire pile length (Bourne-Webb, et al., 2009), the shaft friction can be seen to be mobilised in the upwards and downwards direction of the pile, meeting at a zero movement point which will vary in position depending upon the ground conditions. This behaviour can be visualised, Figure 5, for a pile with and without end restraint.

Figure 5: Thermal Behaviour Pile Profiles (a) shaft restraint heating (b) shaft restraint cooling (c) shaft and end restraint heating (d) shaft and end restraint cooling, (Bourne-Webb, et al., 2012)

2.2.2         Mechanical Loading

Mechanical behaviour of the pile results from the structural load bearing requirements. Vertical loading is applied to the top of the pile inducing compressive strains which reduce over the length, as shown in Figure 6.

Figure 6: Mechanical Behaviour Pile Profile

2.2.3         Thermomechanical Loading

Thermomechanical loading results as a combination of mechanical and thermal loading. Thus, the behaviour of the pile under combined loading is formed from a superposition of the individual mechanical and thermal profiles, as shown in Figure 7.

Figure 7: Thermomechanical Behaviour Pile Profiles (a) shaft restraint heating (b) shaft restraint cooling (c) shaft and end restraint heating (d) shaft and end restraint cooling, (Bourne-Webb, et al., 2012)

As shown in Equation 1, when a pile is cooled tensile strains occur. This can have a positive effect on the pile, in reducing the compressive strains caused by the mechanical loading to reduce. However, as shown in Figure 7b, if the cooling effect is significant and the mechanical loading is minimal this can lead to tensile strains within the pile, which have detrimental effects on the concrete structure.

2.3          Field Testing

Field testing has been limited due to its costly and time-consuming nature. However, two notable investigations have been performed in recent years. The first was conducted by Laloui, et al., (2006) at the Swiss Federal Institute of Technology in Lausanne, where a pile was subjected to thermal and mechanical loads after the completion of the construction of each storey of the building structure, allowing the observation of how the behaviour changed with increasing load. The pile was restrained at the shaft, top and base for testing as it was part of a larger pile raft (Knellwolf, et al., 2011).  The second was conducted by Bourne-Webb, et al. (2009) at Clapham Centre of Lambeth College, South London, where a single test pile was subjected to thermal and mechanical loading in order to measure the behaviour after heating and cooling cycles. The pile was restrained at the shaft, and free at the ends due to a lack of top fixity (Knellwolf, et al., 2011).

Figure 8: Strain Profiles (a) Lambeth College (b) Lausanne

The in-situ tests produced some notable results, with the most important of these strain profiles shown in Figure 8. These profiles demonstrated that the pile strains were significantly affected by the temperature cycles and that tensile strains were generated in the cooling case.

The results produced from these in-situ tests were the basis for the framework described above. As can be seen from Figure 8 the in-situ testing approximately follows the expected profiles: Lambeth College and Figure 7a and Figure 7b; Lausanne and Figure 7c and Figure 7d. This assists somewhat to explain energy pile behaviour, however, is limited to the two sites where the investigations were performed.

2.4          Numerical Modelling

Restraints surrounding in-situ testing of energy piles have led to the development of a number of numerical models, which aim to further the current understanding. Most methods utilise finite elements with two popular approaches applied:

  • T-z load transfer curve
  • Numerical mesh analysis

The t-z load transfer curve has been successfully utilised by Ouyang, et al. (2011) and Knellwolf, et al. (2011), to back-analyse the Lambeth College and Lausanne field tests producing a good correlation between results. Similar simulations have been performed by Gawecka, et al. (2016) with comparable outcomes. Thus, previous numerical tests have demonstrated via back-analysis that they are a viable method to analyse the behaviour of energy piles. However, as this approach is still relatively new, literature has not advanced much past developing and validating these models.

Research has now provided a solid understanding of energy pile strain behaviour. However, tests regarding the mobilised bearing capacity and pile head displacements are currently limited, often produced alongside strain data for limited conditions without further exploration. Therefore, a gap in the knowledge remains surrounding the impact of temperature cycles on the mobilised bearing capacity and head displacements of energy piles for a variety of pile and soil properties.

3                Numerical Model

This section outlines the finite element model, defining how it works and verifying it using a back-analysis against existing field data.

3.1          Model Description

A finite element model developed in MATLAB is to be used to conduct a parametric study of an energy pile. This model adopts a  t-z beam spring method where the pile is split into a number of equally sized, linear beam elements connected by nodes, as shown in Figure 9.

Figure 9: T-z Beam Spring Method

Each node has one degree of freedom, due to free vertical movements. The local beam element stiffness matrix, kEL, is based on standard finite element formulation, (Bathe, 2014):

kEL, pile=EALEL1-1-11

(5)

The soil is simplified as a series of nonlinear springs which connect to the beams simulating the pile-soil interaction. Each spring has one degree of freedom, due to free vertical movement, with the stiffness of the spring, kspring, based upon the load transfer (t-z) curve, shown in Figure 10.

kspring=tz

(6)

The t-z curve defines the shaft friction, t, and pile displacements, z, due to the pile-soil interaction. Maximum shaft friction can be calculated for drained and undrained conditions, (Craig & Knappett, 2012):

tm, undrained=αSuAs

(7)

tm, drained=K0σv’tan⁡φ’As

(8)

Where the terms are defined; soil adhesion factor, α; undrained shear strength of soil, Su; area of pile in contact with soil, As; coefficient of earth pressure, K0; effective vertical soil stress,

σv’; soil friction angle, δ’.

Figure 10: T-z Load Transfer Curve

The maximum stiffness for displacement, km, was defined by Randolph and Wroth (1978):

km=Grln2.5L(1-ν)γ

(9)

Where the terms are defined; soil shear modulus, G; pile radius, r; pile length, L; soil Poisson’s ratio, ν; soil unit weight, γ.

The shaft friction along the load transfer curve has subsequently been defined, (Pelecanos, et al., 2018):

t=kmz1+kmztmhdd

(10)

Where the terms are defined; hardening parameter, h; degradation parameter, d.

Substituting into Equation 6 allows the calculation of the local spring stiffness. The global stiffness matrices for the pile, kp, and the soil, ks, can then be formed by combining the local values for each element. Considering the equilibrium of the model an expression for pile displacements can be derived, (Bathe, 2014):

P=ku

(11)

Displacements, u, are calculated by multiplying the applied mechanical loads, P, against the inverse of the combined global stiffness matrix, k. Where

k=kp+ksthe equation can be stated:

P=kp+ksu

(12)

However, in the case of thermomechanical analysis temperature loading, specified by Equation 4, will also need to be included within the equilibrium equation:

P + αcEA∆T=kp+ksu

(13)

Thus, when the properties and loading are specified the finite element model is able to determine the unknown displacement values.

3.2          Validation

The finite element model will now be validated by performing a back-analysis of a known field study and comparing the test results to ensure that the model appropriately simulates energy pile behaviour.

3.2.1         Lambeth College

Bourne-Webb, et al. (2009) conducted one of the first energy pile field tests at the Clapham Centre of Lambeth College, South London. The study was performed prior to construction of a five storey building supported on 143 bored pile foundations all of which were utilised as a GSHP system. The experiment aimed to determine the behaviour of a single test pile for cycles of heating and cooling under a sustained load (Bourne-Webb, et al., 2009).

The 23m test pile, shown in Figure 11, was designed based purely on the geotechnical requirements with a safety factor of 2.5. The pile diameter varied with depth, 0.610m for the first 5m and 0.550m for the subsequent 18m. U-shaped heat exchanger loops were attached to 32mm reinforcement which extended for the full length of the pile. Continuous strain and temperature measurements were supplied by 18 vibrating-wire strain gauges, 6 thermistors and optical fibre sensors (Bourne-Webb, et al., 2009).

Figure 11: Lambeth College Test Pile, (Bourne-Webb, et al., 2009)

Ground conditions are shown in Figure 11, showed 1.5m of made ground and 2.5m of terrace gravel overlying a layer of London clay. The groundwater table was found within the terrace gravel at depth 3m. Throughout testing a mechanical load of 1200kN was sustained through several cycles of heating and cooling. As seen from Figure 12, the temperature change under cooling ~∆T=-18℃ and ~∆T=+10℃ under heating (Bourne-Webb, et al., 2009).

Figure 12: Lambeth College Test Temperature Variation

Testing was conducted in over a three month period in 2007, with the series of tests specified below:

  • 1800kN applied, pile unloaded;
  • 1200kN applied;
  • Cooling cycles;
  • Heating cycles ;
  • Maximum load test to 3600kN, unloaded (Bourne-Webb, et al., 2009).

The study results, displayed in Figure 8a, significantly improved the understanding of energy pile behaviour. The Lambeth College study has subsequently been successfully used to by multiple studies validate numerical models (Ouyang, et al., 2011; Gawecka, et al., 2016; Knellwolf, et al., 2011). Therefore, a back-analysis of this field data will be performed using the finite element model.

3.2.2         Comparison

Three tests were conducted and compared to Lambeth College data, with the parameters based upon data obtained from a previous back-analysis by Ouyang, et al., (2011). The applied loading and model parameters are displayed in the tables below.

Table 1: Verification Model Loading

 Test Mechanical Load Thermal Load
Mechanical 1.2MN ΔT = 0°C
Heating 1.2MN ΔT = +10°C
Cooling 1.2MN ΔT = -18°C

Table 2: Verification Model Pile Properties

Pile Properties Mechanical Load
Length, L (m) 23
Diameter, d (m) 0.610 for  Depth 0-5m

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