SlideShare a Scribd company logo
Soil-pipe Interaction due to Tunneling April 2009
Winkler Elastic Continuum Solutions
Soil–pipe interaction due to tunneling: comparison between
Winkler and elastic continuum solutions
George M. Iskander* - Ramy H. Gabr**
Introduction:
The aim of this paper is to study the effect of tunneling on existing buried pipelines
[Fig.1] by comparing between an elastic continuum solution and a closed-form Winkler
solution with Vesic subgrade modulus.
Tunneling process generates soil settlement deforming the pipe where it suffers
additional bending depends on the distribution of settlement at the pipeline level and the
relative stiffness between the pipe and the surrounding soil.
Conventionally, this problem is solved using Winkler-based models where an
appropriate subgrade modulus is assumed for both linear elastic and non-linear analyses.
In linear elastic analysis the subgrade modulus is usually determined by means of
Vesic’s expression that allows a beam on a Winkler foundation to exhibit similar
displacements and moments to that of a beam on an elastic half-space when loaded with
the same load.
To validate the comparison results, assumptions are given for both solutions (refer to
the original paper for assumptions (a) to (f))
Elastic Continuum Solution:
The pipe behavior and the soil continuum displacement are represented in [Eq.
(2)&(3)], and after introducing compatibility requirements, elastic continuum solution is
obtained in [Eq.(8)]
Constructing the components of [Eq.(8)] uses point loading however; it does not
satisfy displacement at the point of loading.
To solve this inadequacy, a reference displacement value for that point was
considered [Fig.2], where displacement at certain point due to uniform load equal to
average displacement for that load due to equivalent concentrated load at that point.
Normalized solution is proposed which describe maximum sagging bending moments
[Fig.3], where Smax and i (Inflection point) are the maim factors affecting the relation.
[Fig.4] shows when R increase, the normalized Bending moment decrease which
highlights the overestimation of bending moments when assuming the pipe follows the
curvature of the soil.
Closed-Form Solution of the Winkler Problem:
The pipe behavior is represented in [Eq.9] and illustrated mechanically in [Fig.5].The
infinite Winkler beam consider a concentrated load P to creates bending moment at
distance t [Eq.(10)], the continuous loading due to the soil trough settlement can be
replaced by an infinite number of infinitesimal concentrated loads dP(x) [Eq.(11)].
The maximum sagging moment and the moment due to the infinitesimal loads is
normalized afterthought [Eq.(13)to(15)] and a closed-form solution shall be used in [Eq.
(16)].
.
*Professor, Ain Shams University, Geotechnical Engineering Department.
Department of civil engineering
Ain shams university
- 1 -
Soil-pipe Interaction due to Tunneling April 2009
Winkler Elastic Continuum Solutions
**Student, M.Sc, Structural Engineer.
[Fig.6] shows a comparison of the above solution with the numerical values derived
by Attewell that fit their solution with the current closed-form solution.
The Validity of Vesic’s Subgrade Modulus for Soil–Pipe Interaction:
Attewell suggest the use of the Vesic equation for the subgrade modulus (K∞ ) [Eq.
(17)] which physically means if this subgrade modulus is used to define the maximum
moment in an infinite beam under a concentrated load, this moment will be [Eq.(18)] for
the Winkler solution and [Eq.(19)] for the elastic continuum solution.
But [Eq.(19)] refers to a beam resting on the surface of an infinite half-space, thus for
the buried pipes, Attewell suggested taking K=2K∞ which corresponds to the case where
the pipe is buried at infinite depth which is also considered conservative.
Practically it is more likely to be between K∞ & 2K∞ .
Vesic derivation for [Eq.(17)] based on both Winkler and elastic continuum are
loaded by the same external loads. However, in this case, the tunnel effect may be
represented by a force distribution along the pipe that relates to the greenfield settlement.
These force distributions are not generally the same in both Winkler and elastic
continuum solution, and hence the Vesic expression might not necessarily be adequate
for this case.
[Fig.7] shows comparison between the normalized bending moment resulting from
the continuum elastic analysis and the Winkler solution using Vesic’s expression. It can
be shown that when i/ro increases the two solutions close to each other and tend to be
practically identical. However, when i/ro decreases, significant differences are
recognized due to:
1-The simple beam theory would not be accurate for a case where the extent of
deformation is comparable to the pipe radius.
2-Assumption (c) above may not be justifiable because the pipe is located close to the
tunnel, and the diameter of the pipe is similar to or bigger than that of the tunnel.
Then the comparison between the two models may be considered irrelevant unless the
true solution is known.
Because the Winkler method underestimates the solution [Fig.7], continuum solution
is preferred as it always provides conservative estimation and accurate solutions.
An Alternative Analogue for Winkler Solution:
In the Winkler system the normalized bending moment is a function of ºI, whereas in
the elastic continuum it was found to be a function of R, where a relation is given
between them [Eq.(20)].
[Fig.8] shows the comparison between the Winkler solution with the subgrade
modulus of [Eq.(20) and the continuum solution as before [Eq.(16)] showing a good
agreement between the two solutions.
Department of civil engineering
Ain shams university
- 2 -
Soil-pipe Interaction due to Tunneling April 2009
Winkler Elastic Continuum Solutions
It should be noted that the current analysis is based on a linear elastic soil. In reality
soil non-linearity will be involved. However for small displacement, where elastic
behavior dominates, the elastic continuum solution is still valid.
Conclusions:
The problem of tunneling effects on existing pipelines was solved using an elastic
continuum solution and a closed-form solution for the Winkler solution using Vesic’s
subgrade modulus which was found -after comparing the solutions- to be not necessarily
adequate for this problem.
It was noted that the significant difference between the two models was observed in a
region where both models may possibly become inadequate because of potential violation
of the model assumptions, and that a different approach should be considered for solving
the problem.
In the comparison between the proposed continuum and Winkler models, it is
practically safer to use the proposed continuum method rather than Winkler solution, as it
will either be closer to the accurate solution or at least more conservative than Winkler
solution.
Vesic’s spring coefficient would not generally give identical results to that of a
continuum solution because Vesic’s expression is ideal when Winkler and the continuum
systems are loaded by identical external loads, but in the case, same settlement trough
does not necessarily result in the same loads.
For the current case an alternative expression for the subgrade modulus was
suggested to create similar maximum bending moment in the Winkler and elastic
continuum systems.
Department of civil engineering
Ain shams university
- 3 -

More Related Content

What's hot

Splashing mechanism during impact of a hollow droplet on a substrate(156)doc
Splashing mechanism during impact of a hollow droplet on a substrate(156)docSplashing mechanism during impact of a hollow droplet on a substrate(156)doc
Splashing mechanism during impact of a hollow droplet on a substrate(156)doc
amarjitkene
 
Geotechnical Engineering-I [Lec #17: Consolidation]
Geotechnical Engineering-I [Lec #17: Consolidation]Geotechnical Engineering-I [Lec #17: Consolidation]
Geotechnical Engineering-I [Lec #17: Consolidation]
Muhammad Irfan
 
Peer Reviewed CETI 14-044: CO2 Huff-n-Puff for Condensate Blockage Removal
Peer Reviewed CETI 14-044: CO2 Huff-n-Puff for Condensate Blockage RemovalPeer Reviewed CETI 14-044: CO2 Huff-n-Puff for Condensate Blockage Removal
Peer Reviewed CETI 14-044: CO2 Huff-n-Puff for Condensate Blockage Removal
Uchenna Odi, PhD, MBA
 
FIELD AND THEORETICAL ANALYSIS OF ACCELERATED CONSOLIDATION USING VERTICAL DR...
FIELD AND THEORETICAL ANALYSIS OF ACCELERATED CONSOLIDATION USING VERTICAL DR...FIELD AND THEORETICAL ANALYSIS OF ACCELERATED CONSOLIDATION USING VERTICAL DR...
FIELD AND THEORETICAL ANALYSIS OF ACCELERATED CONSOLIDATION USING VERTICAL DR...
P singh
 
1385911597researchpaper_STUDY-OF-GRAVITY-DRIVEN-FILM-FLOW-WITH-VARIABLE-PHYSI...
1385911597researchpaper_STUDY-OF-GRAVITY-DRIVEN-FILM-FLOW-WITH-VARIABLE-PHYSI...1385911597researchpaper_STUDY-OF-GRAVITY-DRIVEN-FILM-FLOW-WITH-VARIABLE-PHYSI...
1385911597researchpaper_STUDY-OF-GRAVITY-DRIVEN-FILM-FLOW-WITH-VARIABLE-PHYSI...
MD AMZAD HOSSAIN
 
Geotechnical Engineering-I [Lec #22A: Consolidation Problem Sheet]
Geotechnical Engineering-I [Lec #22A: Consolidation Problem Sheet]Geotechnical Engineering-I [Lec #22A: Consolidation Problem Sheet]
Geotechnical Engineering-I [Lec #22A: Consolidation Problem Sheet]
Muhammad Irfan
 
Geotechnical Engineering-I [Lec #3: Phase Relationships]
Geotechnical Engineering-I [Lec #3: Phase Relationships]Geotechnical Engineering-I [Lec #3: Phase Relationships]
Geotechnical Engineering-I [Lec #3: Phase Relationships]
Muhammad Irfan
 
Consolidaton
ConsolidatonConsolidaton
Consolidaton
Hasan Imam
 
Nanoscale 2014
Nanoscale 2014Nanoscale 2014
Nanoscale 2014
Jorge Roque de la Puente
 
Consolidation Properties
Consolidation PropertiesConsolidation Properties
Consolidation Properties
Sanchari Halder
 
Chapter 03
Chapter 03Chapter 03
Chapter 03
SantistebanCampos
 
Phase Change Material Based Solar Water Heater
Phase Change Material Based Solar Water HeaterPhase Change Material Based Solar Water Heater
Phase Change Material Based Solar Water Heater
inventionjournals
 
A Note on the Beavers and Joseph Condition for Flow over a Forchheimer Porous...
A Note on the Beavers and Joseph Condition for Flow over a Forchheimer Porous...A Note on the Beavers and Joseph Condition for Flow over a Forchheimer Porous...
A Note on the Beavers and Joseph Condition for Flow over a Forchheimer Porous...
IJRESJOURNAL
 
Dr khalid elhasnaoui 3
Dr khalid elhasnaoui 3Dr khalid elhasnaoui 3
Dr khalid elhasnaoui 3
Khalid El Hasnaoui
 
Phase of soil (Complete Soil Mech. Undestanding Pakage: ABHAY)
Phase of soil (Complete Soil Mech. Undestanding Pakage: ABHAY)Phase of soil (Complete Soil Mech. Undestanding Pakage: ABHAY)
Phase of soil (Complete Soil Mech. Undestanding Pakage: ABHAY)
Abhay Kumar
 
Field and Theoretical Analysis of Accelerated Consolidation Using Vertical Dr...
Field and Theoretical Analysis of Accelerated Consolidation Using Vertical Dr...Field and Theoretical Analysis of Accelerated Consolidation Using Vertical Dr...
Field and Theoretical Analysis of Accelerated Consolidation Using Vertical Dr...
inventionjournals
 
Molecular Fractal Surfaces Analysis ICSE4-ffvi
Molecular Fractal Surfaces Analysis ICSE4-ffviMolecular Fractal Surfaces Analysis ICSE4-ffvi
Molecular Fractal Surfaces Analysis ICSE4-ffvi
fferrieu
 
Unit4 kvv
Unit4 kvvUnit4 kvv
Unit4 kvv
Pavan Kumar N
 
Index property of soil
Index property of soilIndex property of soil
Index property of soil
SARASWATI PATHARIYA
 
Geotechnical Engineering-I [Lec #27A: Flow Calculation From Flow Nets]
Geotechnical Engineering-I [Lec #27A: Flow Calculation From Flow Nets]Geotechnical Engineering-I [Lec #27A: Flow Calculation From Flow Nets]
Geotechnical Engineering-I [Lec #27A: Flow Calculation From Flow Nets]
Muhammad Irfan
 

What's hot (20)

Splashing mechanism during impact of a hollow droplet on a substrate(156)doc
Splashing mechanism during impact of a hollow droplet on a substrate(156)docSplashing mechanism during impact of a hollow droplet on a substrate(156)doc
Splashing mechanism during impact of a hollow droplet on a substrate(156)doc
 
Geotechnical Engineering-I [Lec #17: Consolidation]
Geotechnical Engineering-I [Lec #17: Consolidation]Geotechnical Engineering-I [Lec #17: Consolidation]
Geotechnical Engineering-I [Lec #17: Consolidation]
 
Peer Reviewed CETI 14-044: CO2 Huff-n-Puff for Condensate Blockage Removal
Peer Reviewed CETI 14-044: CO2 Huff-n-Puff for Condensate Blockage RemovalPeer Reviewed CETI 14-044: CO2 Huff-n-Puff for Condensate Blockage Removal
Peer Reviewed CETI 14-044: CO2 Huff-n-Puff for Condensate Blockage Removal
 
FIELD AND THEORETICAL ANALYSIS OF ACCELERATED CONSOLIDATION USING VERTICAL DR...
FIELD AND THEORETICAL ANALYSIS OF ACCELERATED CONSOLIDATION USING VERTICAL DR...FIELD AND THEORETICAL ANALYSIS OF ACCELERATED CONSOLIDATION USING VERTICAL DR...
FIELD AND THEORETICAL ANALYSIS OF ACCELERATED CONSOLIDATION USING VERTICAL DR...
 
1385911597researchpaper_STUDY-OF-GRAVITY-DRIVEN-FILM-FLOW-WITH-VARIABLE-PHYSI...
1385911597researchpaper_STUDY-OF-GRAVITY-DRIVEN-FILM-FLOW-WITH-VARIABLE-PHYSI...1385911597researchpaper_STUDY-OF-GRAVITY-DRIVEN-FILM-FLOW-WITH-VARIABLE-PHYSI...
1385911597researchpaper_STUDY-OF-GRAVITY-DRIVEN-FILM-FLOW-WITH-VARIABLE-PHYSI...
 
Geotechnical Engineering-I [Lec #22A: Consolidation Problem Sheet]
Geotechnical Engineering-I [Lec #22A: Consolidation Problem Sheet]Geotechnical Engineering-I [Lec #22A: Consolidation Problem Sheet]
Geotechnical Engineering-I [Lec #22A: Consolidation Problem Sheet]
 
Geotechnical Engineering-I [Lec #3: Phase Relationships]
Geotechnical Engineering-I [Lec #3: Phase Relationships]Geotechnical Engineering-I [Lec #3: Phase Relationships]
Geotechnical Engineering-I [Lec #3: Phase Relationships]
 
Consolidaton
ConsolidatonConsolidaton
Consolidaton
 
Nanoscale 2014
Nanoscale 2014Nanoscale 2014
Nanoscale 2014
 
Consolidation Properties
Consolidation PropertiesConsolidation Properties
Consolidation Properties
 
Chapter 03
Chapter 03Chapter 03
Chapter 03
 
Phase Change Material Based Solar Water Heater
Phase Change Material Based Solar Water HeaterPhase Change Material Based Solar Water Heater
Phase Change Material Based Solar Water Heater
 
A Note on the Beavers and Joseph Condition for Flow over a Forchheimer Porous...
A Note on the Beavers and Joseph Condition for Flow over a Forchheimer Porous...A Note on the Beavers and Joseph Condition for Flow over a Forchheimer Porous...
A Note on the Beavers and Joseph Condition for Flow over a Forchheimer Porous...
 
Dr khalid elhasnaoui 3
Dr khalid elhasnaoui 3Dr khalid elhasnaoui 3
Dr khalid elhasnaoui 3
 
Phase of soil (Complete Soil Mech. Undestanding Pakage: ABHAY)
Phase of soil (Complete Soil Mech. Undestanding Pakage: ABHAY)Phase of soil (Complete Soil Mech. Undestanding Pakage: ABHAY)
Phase of soil (Complete Soil Mech. Undestanding Pakage: ABHAY)
 
Field and Theoretical Analysis of Accelerated Consolidation Using Vertical Dr...
Field and Theoretical Analysis of Accelerated Consolidation Using Vertical Dr...Field and Theoretical Analysis of Accelerated Consolidation Using Vertical Dr...
Field and Theoretical Analysis of Accelerated Consolidation Using Vertical Dr...
 
Molecular Fractal Surfaces Analysis ICSE4-ffvi
Molecular Fractal Surfaces Analysis ICSE4-ffviMolecular Fractal Surfaces Analysis ICSE4-ffvi
Molecular Fractal Surfaces Analysis ICSE4-ffvi
 
Unit4 kvv
Unit4 kvvUnit4 kvv
Unit4 kvv
 
Index property of soil
Index property of soilIndex property of soil
Index property of soil
 
Geotechnical Engineering-I [Lec #27A: Flow Calculation From Flow Nets]
Geotechnical Engineering-I [Lec #27A: Flow Calculation From Flow Nets]Geotechnical Engineering-I [Lec #27A: Flow Calculation From Flow Nets]
Geotechnical Engineering-I [Lec #27A: Flow Calculation From Flow Nets]
 

Viewers also liked

Pipe Soil Interaction
Pipe Soil InteractionPipe Soil Interaction
Pipe Soil Interaction
Mintu Choudhury
 
Building Service Chapter 2
Building Service Chapter 2Building Service Chapter 2
Building Service Chapter 2
Izam Lukman
 
plumbing
plumbingplumbing
plumbing
Piyush Dhola
 
Building Services Engg. (Electrical installations)
Building Services Engg. (Electrical installations)Building Services Engg. (Electrical installations)
Building Services Engg. (Electrical installations)
Ritesh Ambadkar
 
Plumbing in Architecture
Plumbing in ArchitecturePlumbing in Architecture
Plumbing in Architecture
Sneha Nagarajan
 
Piping training-course
Piping training-coursePiping training-course
Piping training-course
pdmsguy
 
Building services
Building servicesBuilding services
Building services
Siddharth Khanna
 

Viewers also liked (7)

Pipe Soil Interaction
Pipe Soil InteractionPipe Soil Interaction
Pipe Soil Interaction
 
Building Service Chapter 2
Building Service Chapter 2Building Service Chapter 2
Building Service Chapter 2
 
plumbing
plumbingplumbing
plumbing
 
Building Services Engg. (Electrical installations)
Building Services Engg. (Electrical installations)Building Services Engg. (Electrical installations)
Building Services Engg. (Electrical installations)
 
Plumbing in Architecture
Plumbing in ArchitecturePlumbing in Architecture
Plumbing in Architecture
 
Piping training-course
Piping training-coursePiping training-course
Piping training-course
 
Building services
Building servicesBuilding services
Building services
 

Similar to Geotechnical-Report-Final

Turbulence Modeling – The k-ε Turbulence Model.pdf
Turbulence Modeling – The k-ε Turbulence Model.pdfTurbulence Modeling – The k-ε Turbulence Model.pdf
Turbulence Modeling – The k-ε Turbulence Model.pdf
SkTarifAli1
 
Consolidation settlement with sand drains – analytical and numerical approaches
Consolidation settlement with sand drains – analytical and numerical approachesConsolidation settlement with sand drains – analytical and numerical approaches
Consolidation settlement with sand drains – analytical and numerical approaches
Umed Paliwal
 
velocity distribution in diverging Channel.pptx
velocity distribution in diverging Channel.pptxvelocity distribution in diverging Channel.pptx
velocity distribution in diverging Channel.pptx
BodapatiSreeSaiPrasa
 
K012256874
K012256874K012256874
K012256874
IOSR Journals
 
Efficiency of vertical drains using finite element method may 2017
Efficiency of vertical drains using finite element method may 2017Efficiency of vertical drains using finite element method may 2017
Efficiency of vertical drains using finite element method may 2017
Dr Mazin Alhamrany
 
Andreev zhelyazkov embankment_final
Andreev zhelyazkov embankment_finalAndreev zhelyazkov embankment_final
Andreev zhelyazkov embankment_final
Stoyan Andreev
 
Calculation of Fluid Dynamic for Wind Flow around Reinforced Concrete Walls
Calculation of Fluid Dynamic for Wind Flow around Reinforced Concrete WallsCalculation of Fluid Dynamic for Wind Flow around Reinforced Concrete Walls
Calculation of Fluid Dynamic for Wind Flow around Reinforced Concrete Walls
IJERA Editor
 
9979190.pdf
9979190.pdf9979190.pdf
9979190.pdf
ssusercf6d0e
 
Numerical study on free-surface flow
Numerical study on free-surface flowNumerical study on free-surface flow
Numerical study on free-surface flow
miguelpgomes07
 
Slope Stability Evaluation for the New Railway Embankment using Stochastic & ...
Slope Stability Evaluation for the New Railway Embankment using Stochastic & ...Slope Stability Evaluation for the New Railway Embankment using Stochastic & ...
Slope Stability Evaluation for the New Railway Embankment using Stochastic & ...
Dr.Costas Sachpazis
 
Flow Modeling Based Wall Element Technique
Flow Modeling Based Wall Element TechniqueFlow Modeling Based Wall Element Technique
Flow Modeling Based Wall Element Technique
CSCJournals
 
FDSSI.pptx
FDSSI.pptxFDSSI.pptx
FDSSI.pptx
VaibhavPawar130
 
FDSSI.pptx
FDSSI.pptxFDSSI.pptx
FDSSI.pptx
VaibhavPawar130
 
paper_237_theme7_haug&mukherjee
paper_237_theme7_haug&mukherjeepaper_237_theme7_haug&mukherjee
paper_237_theme7_haug&mukherjee
Rahul Mukherjee
 
Vilnay chernincotsovos
Vilnay chernincotsovosVilnay chernincotsovos
Vilnay chernincotsovos
GanapathyramasamyN
 
E04701035045
E04701035045E04701035045
E04701035045
ijceronline
 
Fatigue behavior of high volume fly ash
Fatigue behavior of high volume fly ashFatigue behavior of high volume fly ash
Fatigue behavior of high volume fly ash
IAEME Publication
 
Buckling and Pull-In Instability of Multi-Walled Carbon Nanotube Probes Near ...
Buckling and Pull-In Instability of Multi-Walled Carbon Nanotube Probes Near ...Buckling and Pull-In Instability of Multi-Walled Carbon Nanotube Probes Near ...
Buckling and Pull-In Instability of Multi-Walled Carbon Nanotube Probes Near ...
IJERA Editor
 
ANSYS FLUENT 12.0 Theory Guide - 4.12.1 Overview.pdf
ANSYS FLUENT 12.0 Theory Guide - 4.12.1 Overview.pdfANSYS FLUENT 12.0 Theory Guide - 4.12.1 Overview.pdf
ANSYS FLUENT 12.0 Theory Guide - 4.12.1 Overview.pdf
Álvaro Gil
 
Jwrhe10065 20150204-144509-1366-46826
Jwrhe10065 20150204-144509-1366-46826Jwrhe10065 20150204-144509-1366-46826
Jwrhe10065 20150204-144509-1366-46826
yimer mulate
 

Similar to Geotechnical-Report-Final (20)

Turbulence Modeling – The k-ε Turbulence Model.pdf
Turbulence Modeling – The k-ε Turbulence Model.pdfTurbulence Modeling – The k-ε Turbulence Model.pdf
Turbulence Modeling – The k-ε Turbulence Model.pdf
 
Consolidation settlement with sand drains – analytical and numerical approaches
Consolidation settlement with sand drains – analytical and numerical approachesConsolidation settlement with sand drains – analytical and numerical approaches
Consolidation settlement with sand drains – analytical and numerical approaches
 
velocity distribution in diverging Channel.pptx
velocity distribution in diverging Channel.pptxvelocity distribution in diverging Channel.pptx
velocity distribution in diverging Channel.pptx
 
K012256874
K012256874K012256874
K012256874
 
Efficiency of vertical drains using finite element method may 2017
Efficiency of vertical drains using finite element method may 2017Efficiency of vertical drains using finite element method may 2017
Efficiency of vertical drains using finite element method may 2017
 
Andreev zhelyazkov embankment_final
Andreev zhelyazkov embankment_finalAndreev zhelyazkov embankment_final
Andreev zhelyazkov embankment_final
 
Calculation of Fluid Dynamic for Wind Flow around Reinforced Concrete Walls
Calculation of Fluid Dynamic for Wind Flow around Reinforced Concrete WallsCalculation of Fluid Dynamic for Wind Flow around Reinforced Concrete Walls
Calculation of Fluid Dynamic for Wind Flow around Reinforced Concrete Walls
 
9979190.pdf
9979190.pdf9979190.pdf
9979190.pdf
 
Numerical study on free-surface flow
Numerical study on free-surface flowNumerical study on free-surface flow
Numerical study on free-surface flow
 
Slope Stability Evaluation for the New Railway Embankment using Stochastic & ...
Slope Stability Evaluation for the New Railway Embankment using Stochastic & ...Slope Stability Evaluation for the New Railway Embankment using Stochastic & ...
Slope Stability Evaluation for the New Railway Embankment using Stochastic & ...
 
Flow Modeling Based Wall Element Technique
Flow Modeling Based Wall Element TechniqueFlow Modeling Based Wall Element Technique
Flow Modeling Based Wall Element Technique
 
FDSSI.pptx
FDSSI.pptxFDSSI.pptx
FDSSI.pptx
 
FDSSI.pptx
FDSSI.pptxFDSSI.pptx
FDSSI.pptx
 
paper_237_theme7_haug&mukherjee
paper_237_theme7_haug&mukherjeepaper_237_theme7_haug&mukherjee
paper_237_theme7_haug&mukherjee
 
Vilnay chernincotsovos
Vilnay chernincotsovosVilnay chernincotsovos
Vilnay chernincotsovos
 
E04701035045
E04701035045E04701035045
E04701035045
 
Fatigue behavior of high volume fly ash
Fatigue behavior of high volume fly ashFatigue behavior of high volume fly ash
Fatigue behavior of high volume fly ash
 
Buckling and Pull-In Instability of Multi-Walled Carbon Nanotube Probes Near ...
Buckling and Pull-In Instability of Multi-Walled Carbon Nanotube Probes Near ...Buckling and Pull-In Instability of Multi-Walled Carbon Nanotube Probes Near ...
Buckling and Pull-In Instability of Multi-Walled Carbon Nanotube Probes Near ...
 
ANSYS FLUENT 12.0 Theory Guide - 4.12.1 Overview.pdf
ANSYS FLUENT 12.0 Theory Guide - 4.12.1 Overview.pdfANSYS FLUENT 12.0 Theory Guide - 4.12.1 Overview.pdf
ANSYS FLUENT 12.0 Theory Guide - 4.12.1 Overview.pdf
 
Jwrhe10065 20150204-144509-1366-46826
Jwrhe10065 20150204-144509-1366-46826Jwrhe10065 20150204-144509-1366-46826
Jwrhe10065 20150204-144509-1366-46826
 

Geotechnical-Report-Final

  • 1. Soil-pipe Interaction due to Tunneling April 2009 Winkler Elastic Continuum Solutions Soil–pipe interaction due to tunneling: comparison between Winkler and elastic continuum solutions George M. Iskander* - Ramy H. Gabr** Introduction: The aim of this paper is to study the effect of tunneling on existing buried pipelines [Fig.1] by comparing between an elastic continuum solution and a closed-form Winkler solution with Vesic subgrade modulus. Tunneling process generates soil settlement deforming the pipe where it suffers additional bending depends on the distribution of settlement at the pipeline level and the relative stiffness between the pipe and the surrounding soil. Conventionally, this problem is solved using Winkler-based models where an appropriate subgrade modulus is assumed for both linear elastic and non-linear analyses. In linear elastic analysis the subgrade modulus is usually determined by means of Vesic’s expression that allows a beam on a Winkler foundation to exhibit similar displacements and moments to that of a beam on an elastic half-space when loaded with the same load. To validate the comparison results, assumptions are given for both solutions (refer to the original paper for assumptions (a) to (f)) Elastic Continuum Solution: The pipe behavior and the soil continuum displacement are represented in [Eq. (2)&(3)], and after introducing compatibility requirements, elastic continuum solution is obtained in [Eq.(8)] Constructing the components of [Eq.(8)] uses point loading however; it does not satisfy displacement at the point of loading. To solve this inadequacy, a reference displacement value for that point was considered [Fig.2], where displacement at certain point due to uniform load equal to average displacement for that load due to equivalent concentrated load at that point. Normalized solution is proposed which describe maximum sagging bending moments [Fig.3], where Smax and i (Inflection point) are the maim factors affecting the relation. [Fig.4] shows when R increase, the normalized Bending moment decrease which highlights the overestimation of bending moments when assuming the pipe follows the curvature of the soil. Closed-Form Solution of the Winkler Problem: The pipe behavior is represented in [Eq.9] and illustrated mechanically in [Fig.5].The infinite Winkler beam consider a concentrated load P to creates bending moment at distance t [Eq.(10)], the continuous loading due to the soil trough settlement can be replaced by an infinite number of infinitesimal concentrated loads dP(x) [Eq.(11)]. The maximum sagging moment and the moment due to the infinitesimal loads is normalized afterthought [Eq.(13)to(15)] and a closed-form solution shall be used in [Eq. (16)]. . *Professor, Ain Shams University, Geotechnical Engineering Department. Department of civil engineering Ain shams university - 1 -
  • 2. Soil-pipe Interaction due to Tunneling April 2009 Winkler Elastic Continuum Solutions **Student, M.Sc, Structural Engineer. [Fig.6] shows a comparison of the above solution with the numerical values derived by Attewell that fit their solution with the current closed-form solution. The Validity of Vesic’s Subgrade Modulus for Soil–Pipe Interaction: Attewell suggest the use of the Vesic equation for the subgrade modulus (K∞ ) [Eq. (17)] which physically means if this subgrade modulus is used to define the maximum moment in an infinite beam under a concentrated load, this moment will be [Eq.(18)] for the Winkler solution and [Eq.(19)] for the elastic continuum solution. But [Eq.(19)] refers to a beam resting on the surface of an infinite half-space, thus for the buried pipes, Attewell suggested taking K=2K∞ which corresponds to the case where the pipe is buried at infinite depth which is also considered conservative. Practically it is more likely to be between K∞ & 2K∞ . Vesic derivation for [Eq.(17)] based on both Winkler and elastic continuum are loaded by the same external loads. However, in this case, the tunnel effect may be represented by a force distribution along the pipe that relates to the greenfield settlement. These force distributions are not generally the same in both Winkler and elastic continuum solution, and hence the Vesic expression might not necessarily be adequate for this case. [Fig.7] shows comparison between the normalized bending moment resulting from the continuum elastic analysis and the Winkler solution using Vesic’s expression. It can be shown that when i/ro increases the two solutions close to each other and tend to be practically identical. However, when i/ro decreases, significant differences are recognized due to: 1-The simple beam theory would not be accurate for a case where the extent of deformation is comparable to the pipe radius. 2-Assumption (c) above may not be justifiable because the pipe is located close to the tunnel, and the diameter of the pipe is similar to or bigger than that of the tunnel. Then the comparison between the two models may be considered irrelevant unless the true solution is known. Because the Winkler method underestimates the solution [Fig.7], continuum solution is preferred as it always provides conservative estimation and accurate solutions. An Alternative Analogue for Winkler Solution: In the Winkler system the normalized bending moment is a function of ºI, whereas in the elastic continuum it was found to be a function of R, where a relation is given between them [Eq.(20)]. [Fig.8] shows the comparison between the Winkler solution with the subgrade modulus of [Eq.(20) and the continuum solution as before [Eq.(16)] showing a good agreement between the two solutions. Department of civil engineering Ain shams university - 2 -
  • 3. Soil-pipe Interaction due to Tunneling April 2009 Winkler Elastic Continuum Solutions It should be noted that the current analysis is based on a linear elastic soil. In reality soil non-linearity will be involved. However for small displacement, where elastic behavior dominates, the elastic continuum solution is still valid. Conclusions: The problem of tunneling effects on existing pipelines was solved using an elastic continuum solution and a closed-form solution for the Winkler solution using Vesic’s subgrade modulus which was found -after comparing the solutions- to be not necessarily adequate for this problem. It was noted that the significant difference between the two models was observed in a region where both models may possibly become inadequate because of potential violation of the model assumptions, and that a different approach should be considered for solving the problem. In the comparison between the proposed continuum and Winkler models, it is practically safer to use the proposed continuum method rather than Winkler solution, as it will either be closer to the accurate solution or at least more conservative than Winkler solution. Vesic’s spring coefficient would not generally give identical results to that of a continuum solution because Vesic’s expression is ideal when Winkler and the continuum systems are loaded by identical external loads, but in the case, same settlement trough does not necessarily result in the same loads. For the current case an alternative expression for the subgrade modulus was suggested to create similar maximum bending moment in the Winkler and elastic continuum systems. Department of civil engineering Ain shams university - 3 -