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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________________
Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 95
DESIGN AND ANALYSIS OF STRESS RIBBON BRIDGES
Siddhartha Ray1, D. M. Joshi2, Rahul Chandrashekar3
1
M. E. student, Department of Civil Engineering, S. C. O.E., Kharghar, Maharashtra, India
2
Assistant Professor., Department of Civil Engineering, S. C. O.E., Kharghar, Maharashtra, India
3
Design Engineering, Precast, L & T Construction, Maharashtra, India
Abstract
A stressed ribbon bridge (also known as stress-ribbon bridge or catenary bridge) is primarily a structure under tension. The
tension cablesform the part of the deck which follows an inverted catenary between supports. The ribbon is stressed such that it is
in compression, thereby increasing the rigidity of the structure where as a suspension spans tend to sway and bounce. Such
bridges are typically made RCC structures with tension cables to support them. Such bridges are generally not designed for
vehicular traffic but where it is essential, additional rigidity is essential to avoid the failure of the structure in bending. A stress
ribbon bridge of 45 meter span is modelled and analyzed using ANSYS version 12. For simplicity in importing civil materials a nd
civil cross sections, CivilFEM version 12 add-on of ANSYS was used. A 3D model of the whole structure was developed and
analyzed and according to the analysis results, the design was performed manually.
Keywords: Stress Ribbon, Precast Segments, Prestressing, Dynamic Analysis, Pedestrian Excitation.
--------------------------------------------------------------------***----------------------------------------------------------------------
1. INTRODUCTION
Stress-ribbon bridge is the term that has been created to
describe on which pedestrians can directly walk and is in the
shape of an inverted arch. The structure consists of
tensioned cables which have slight sag in them, embedded
in a concrete deck which is very slender when compared
with the span. This deck serves the purpose of distributing
the loads and to maintain the continuous nature of the deck,.
It is a type of a suspended structure where the cables are
tensioned so tightly that the pedestrian load can be placed
directly on the concrete deck in which the cables are
embedded. It’s a very simple structure when compared to
other complex structures like suspension bridges. The only
drawback of these bridges is the very fact that the tensioning
force is so high in the cables that one has to anchor its
abutments which makes the bridge expensive.
A stressed ribbon bridge is a structure primarily in tension
which is very similar structurally to suspension bridges. The
design of such bridges is very rare in the world. Very few
engineers as such understand its form and behaviour and
hence such bridges are not common in the world. Unlike a
simple suspension bridge, the ribbon is stressed in
compression which increases the stiffness of the structure.
Such bridges are typically made RCC structures with
tension cables to support them. They are primarily used for
pedestrians but bicycles may be allowed based on design.
Such bridges, generally are maintenance free, architecturally
appeasing and economical when compared with their spans.
The slender deck allows them to make the minimum use of
construction material. In the current scenario, research is
being carried out to find the most viable variation of the
structure by combining it with arches.
Fig. 1 Redding Pedestrian stress ribbon bridge.
There are 3 types of stress ribbon bridges, namely
traditional, stress ribbon bridges supported on an arch and
stress ribbon bridge suspended on an arch. Fig. 1 is an
example of a traditional stress ribbon bridge.
For stress ribbon bridges supported on arches, the arch acts
as a temporary support wherein the deck can rise during and
fall during various loading states and temperature
fluctuations. The Fig. 2a shows the general structural
arrangement of a stress ribbon bridge supported on arches.
In its initial stages, it resembles its behaviour as a two-span
cable, supported by the central support that is anchored to
the end abutments (ref. Fig.2b). The supporting arch is
stressed by its own weight in addition to that of the deck,
the self-weight of the support members and the radial forces
exerted by the tensioned cables (ref. Fig.2c) [4]. After post-
tensioning the entire structure behaves as one.
The thrust forces in the stress ribbon HSR and the arch HA
play a critical role since they have to be chosen in such a
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________________
Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 96
manner that they are equal. If the aforementioned criteria are
met, the stress ribbon and the arch can be connected by and
inclined strut which shall primarily be in compression. An
overturning moment shall be created by cable thrust HSR*h
which shall be balanced by the arch reaction ΔV*LP. Hence
a self-balancing mechanism is created (ref Fig.2d) [4].
Another alternative is to suspend the stress-ribbon fromthe
arch. Self-balancing systems can be made for the same as
well.
Fig. 3a, shows a fixed arch at the end anchorages of a
slender prestressed concrete deck. The loadings on the arch
is its ownself weight in addition to the self-weight of the
stress-ribbon combined with the radial forces of the
tensioning cables. Fig. 3bpresents a statically similar
structure as represented in Fig. 2d. Fig. 3 c presents a
condition wherein the thin prestressed deck with additional
flexural rigidity in the unsupported section of the structure
[[4]].
Fig. 2 Stress ribbon supported by arch.
Fig. 3 Stress ribbon suspended on arch.
The aim of the present study is to analyse a traditional stress
ribbon for a span of 45 meters for IRC loading conditions
and a safety check for pedestrian excitation.
2.MODELING AND ANALYSIS RESULTS
The deck segment selected was 4 meters wide, 250 mm
thick and 1 meter long. The bridge would consist of 45 such
segments supported on bearing cables. The meshing was
performed according to the length of segments. The deck
had to be given a sag by the formula 𝑓 = 0.02 ∗ 𝐿 where L
is the length of the bridge [3]. The final geometric model of
the bridge is shown in Fig. 4.
Fig. 4 Final geometric model.
The structure was loaded with live, wind and temperature
loads as per IRC 6-2010. Wind and temperature loads were
calculated for Mumbai region. The force in the bearing
cable was calculated as per 𝑃 =
𝑤∗𝐿2
8∗𝑓
, where w is the self
weight intensity of the bridge deck [3]. The cable forces
come to 7320 kN which will require 4 12K15 prestressing
cables to transfer the load to the abutment. The structure was
analyzed in ANSYS for the individual load cases and load
combinations as per IRC 6-2010. The results are shown in
table 1.
Table 1. Loading Results
Sr.
No.
Load Case
Bending
Moment
(kNm)
Maximum
Deflection
(mm)
Sag Hog
1 Live Load 104 212 65.66
2
Transverse Wind
Load
- - 0.3
3 Vertical Wind Load 36 72 22.36
4 Temperature Load (+) 80 158 49.26
5 Temperature Load (-) 158 80
49.26
(upward)
6 Normal Combination 104 212 65.66
7
Temperature
Combination
184 370 115
8
Wind & Temperature
Combination
219 443 137.3
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________________
Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 97
The critical load combination in terms of prestressing steel
comes out to the temperature combination which also proves
that stress ribbons are critical to temperature [3]. It was for
this combination the design was carried out as per IRC 18-
2000 manually and 6, 4K15 cables stressed at a force of 800
kN each, including losses was found out as the post
tensioned steel requirement.
The structure was then analyzed for the different critical
prestressing conditions in ANSYS and the deflection for the
structure in the final state under temperature combination
and prestress is shown in Fig. 5. Also since stress is an
important parameter under prestressing conditions the
maximum stress results under temperature combination and
prestress are also shown in Fig. 6. The table 2 shows the
results due to prestress under transfer and temperature
combination. Non critical cases and bending moments are
not mentioned in table 2. Minimum reinforcement in the
form of untensioned steelhas to be provided in the segments
for safety against temperature.
Fig. 5 Deflection due to temperature combination and
prestress in meters.
Fig. 6 Stress due to temperature combination and prestress
in kN/m2.
Table 2. Prestressing Results
Sr.
No.
Load
Case
Bending
Moment
(kNm)
Maximum
Deflection
(mm)
Stress
(N/mm2)
Sag Hog
1 Dead
Load &
Prestress
217 106 67.08
(upward)
10.16
(Comp)
& 0.233
(Tensile)
2 Prestress
&
Temperat
ure
Combinati
on
- - 47.84 4.06
(Comp)
& 3.31
(Tensile)
The initial approach was to design a standard abutment that
is generally used for bridges with the proportioning of its
dimensions as given in standard books used for bridge
engineering. The drawback however was that the horizontal
deflection of the abutment due to the cable forces was very
high, almost 400 mm deflection for 5 meter height of the
abutment. Hence a stepped abutment was taken into
consideration whose deflections were much lesser than the
standard abutment. The cross sectional dimensions of the
stepped abutment are shown below in Fig. 7. The top width
of the abutment is 4 m which is the width of the deck of the
bridge. A gradually decreasing drop of around 300 mm is
provided so as to accommodate the first segment of the deck
having a depth of 250 mm and an extra 50 mm for the
provisions of elastomeric bearings while maintaining the
slope of the deck. The bottom width of the abutment
provided is 9 m so as to satisfy the S.B.C. conditions of the
strata below. The stratumbelow is assumed as rock having a
S.B.C. value of 900 kN/m2.
Fig. 7 Abutment cross section.
The most critical loading condition for the abutment is the
cable forces acting on it [3] and structural engineers around
the world design the abutment for cable forces only. The
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________________
Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 98
abutment was analyzed for cable forces in ANSYS and the
bending moment results for the same are shown in Fig. 8.
The design was performed manually as per IRC 21-2000
and the untensioned reinforcement for the top part of the
abutment comes out to 20 tor bars @125 mm c/c and for the
bottompart comes out to 32 tor bars @ 100 mm c/c.
Fig. 8 Bending moment in abutment due to cable force in
kNm.
While most bridge abutments have only compressive forces
on the soil, a stress ribbon bridge abutment will also have
tension on its abutment base. The soil pressure results are
shown in Fig. 9 under normal working conditions without
any soil improvement methods. It is due these high tension
forces on the abutment, rock anchoring is generally
suggested to keep the abutment in place.
Fig. 9 Soil pressure results.
3. DYNAMIC ANALYSIS AND PEDESTRIAN
EXCITATION
There are three primary mode shapes for the deck, namely,
vertical, lateral and torsion modes. The first three modes are
vertical. The first lateral mode is the fourth mode and the
first torsional mode is the seventh mode.
The first two vertical modes have a frequencies f1=1.379 Hz
and f2=1.788 Hz respectively and the mode shapes are
shown in Fig. 10 and Fig. 11 respectively. Normal practice
suggests that that the second mode f2shape should actually
be the first mode shape but, this mode requires an elongation
of the cable, hence the corresponding frequency in some
cases is higher and mode shape of f1 becomes the first mode
[3].
The first lateral mode is the fourth mode of the structure
with a frequency f4=3.959 Hz. Due to the vertical curvature
of the prestressed band, a horizontal movement is always
combined with torsion and it is therefore difficult to find a
pure torsional mode [3]. The first torsional mode is the
seventh mode for the structure with a frequency of
f4=7.129Hz. Both the mode shapes are shown in Fig. 12 and
Fig. 13 respectively.
Fig. 10Mode shape for frequency f1=1.379 Hz.
Fig. 11 Mode shape for frequency f2=1.788 Hz.
Fig. 12 Mode shape for frequency f4=3.959 Hz.
Fig. 13 Mode shape for frequency f7=7.129 Hz.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________________
Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 99
Stress ribbon bridges are very slender in nature and have a
natural frequency very close to the pedestrian walking
frequency of 2 Hz [1], [4], [5]. The codes of choice for
structural engineers around the world for pedestrian
excitation analysis are The British Standard BS 5400 Part 2
and Ontario Highway Bridge Design Code OHBDCONT 83
[3], [6]. For this article, I have used fib 32 guidelines and BS
5400 limiting criteria.
The fib 32 has a calculation method which determines the
maximum vertical acceleration resulting from the passage of
one pedestrian walking / running with a pace rate equal to
the fundamental natural frequency of the bridge. Therefore,
it is modelled as an equivalent single degree-of-freedom
oscillator. The formula is given below,
𝑎 = 4 ∗ 𝜋2
∗ 𝑓2
∗ 𝑦 ∗ 𝛼 ∗ ∅
Where, a= Acceleration in m/s2,
f= Vertical natural frequency of the bridge in Hz,
y= Static deflection at mid span in m for a force of 700N,
α = Fourier coefficient of the relevant harmonic of the
walking or running rate,
∅ = Dynamic amplification factor for one pedestrian moving
across simple span (See Fig. 14).
Fig. 14 Dynamic amplification factor.
For given conditions, the value of α would be 0.4 for a step
frequency of 2 Hz for the first natural frequency and number
of cycles per span for a 45 m span bridge is 60 [2]. BS 5400
Part 2 also considers the higher order harmonics of the
structure and hence it has a limiting value of frequencies to
be considered till 5 Hz. However research has shown that
higher order harmonics (frequency above 2.4 Hz) will not
produce important oscillations in a structure due to the lower
force component of higher harmonics [2]. The permissible
vertical acceleration is, 𝑎 𝑉,𝑚𝑎𝑥 = 0.5 ∗ √ 𝑓. The results of
pedestrian excitation is given in table 3.
Table 3 Pedestrian Excitation Results
Frequency
(Hz)
y (m) α 
a (m/ss
)
aV,max(m/ss
)
f1=1.379 0.000508 0.4 25 0.381682 0.587154
f2=1.788 0.000508 0.1 25 0.160416 0.668581
The above table shows that the vertical accelerations of the
bridge deck for the first two frequencies are well within the
permissible limits and hence the pedestrians will not feel
discomfort while walking on the bridge. Hence the bridge
will be safe from pedestrian excitation at its critical
frequencies.
4. CONCLUSION
The basic objective of this study is to elaborate on what a
stress ribbon bridge is, its types and its advantages over
conventional pedestrian bridges. This study elaborates on
the various parameters essential before the actual design or
analysis and the sources from which they are obtained. It
also briefly explains the process of modelling, loading and
analysis of a stress ribbon bridge in ANSYS. The critical
conditions were identified and designed for manually. In this
study a model of a stress ribbon bridge of 45 meter span is
modelled and analyzed using ANSYS version 12. the
following conclusions can be made:
 Design of stress ribbon structures have confirmed that a
slender concrete deck supported by an internal and/or
external cables can be very efficient.
 Their designs have to be based on understanding of the
cable tension, bending stiffness and on the
understanding of the function of the prestressed
concrete deck.
 The bending moment in a stress ribbon bridge is much
lesser when compared to a beambecause of its inverted
arch shape.
 Temperature is a critical condition in a stress ribbon
bridge due to its slender deck and flexible nature.

The abutment has to transfer high cable forces due to which
it requires a very good stratumbelow it (preferably rock).
REFERENCES
[1] D. E. Newland, 2004. “Pedestrian excitation of
bridges”, Institution of Mechanical Engineers
(IMechE), Volume 218, Part C, 477-492.
[2] Jiri Strasky, et al., 2005. “Guidelines for the design of
footbridges”, federation internationale du béton (fib),
Bulletin 32.
[3] Jiri Strasky, 2006. “Stress Ribbon and Cable Supported
Pedestrian Bridges”, Academy of Sciences of the Czech
Republic, Brno, Czech Republic.
[4] Jiri Strasky, 2008. “Stress Ribbon Pedestrian Bridges
Supported or Suspended on Arches”, Chinese-Croatian
joint colloquium, Long Arch Bridges, Brijuni Islands,
Croatia, 135-147.
[5] Jiri Strasky, 2010. “Stress Ribbon and Arch Pedestrian
Bridges”, 6th International Conference on Arch
Bridges, Fuzhou, China, 38-45.
[6] Dr. Chung C. Fu, “Dynamic Response of Pedestrian
Bridges”, Research Professor, University of Maryland.

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Design and analysis of stress ribbon bridges

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________________ Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 95 DESIGN AND ANALYSIS OF STRESS RIBBON BRIDGES Siddhartha Ray1, D. M. Joshi2, Rahul Chandrashekar3 1 M. E. student, Department of Civil Engineering, S. C. O.E., Kharghar, Maharashtra, India 2 Assistant Professor., Department of Civil Engineering, S. C. O.E., Kharghar, Maharashtra, India 3 Design Engineering, Precast, L & T Construction, Maharashtra, India Abstract A stressed ribbon bridge (also known as stress-ribbon bridge or catenary bridge) is primarily a structure under tension. The tension cablesform the part of the deck which follows an inverted catenary between supports. The ribbon is stressed such that it is in compression, thereby increasing the rigidity of the structure where as a suspension spans tend to sway and bounce. Such bridges are typically made RCC structures with tension cables to support them. Such bridges are generally not designed for vehicular traffic but where it is essential, additional rigidity is essential to avoid the failure of the structure in bending. A stress ribbon bridge of 45 meter span is modelled and analyzed using ANSYS version 12. For simplicity in importing civil materials a nd civil cross sections, CivilFEM version 12 add-on of ANSYS was used. A 3D model of the whole structure was developed and analyzed and according to the analysis results, the design was performed manually. Keywords: Stress Ribbon, Precast Segments, Prestressing, Dynamic Analysis, Pedestrian Excitation. --------------------------------------------------------------------***---------------------------------------------------------------------- 1. INTRODUCTION Stress-ribbon bridge is the term that has been created to describe on which pedestrians can directly walk and is in the shape of an inverted arch. The structure consists of tensioned cables which have slight sag in them, embedded in a concrete deck which is very slender when compared with the span. This deck serves the purpose of distributing the loads and to maintain the continuous nature of the deck,. It is a type of a suspended structure where the cables are tensioned so tightly that the pedestrian load can be placed directly on the concrete deck in which the cables are embedded. It’s a very simple structure when compared to other complex structures like suspension bridges. The only drawback of these bridges is the very fact that the tensioning force is so high in the cables that one has to anchor its abutments which makes the bridge expensive. A stressed ribbon bridge is a structure primarily in tension which is very similar structurally to suspension bridges. The design of such bridges is very rare in the world. Very few engineers as such understand its form and behaviour and hence such bridges are not common in the world. Unlike a simple suspension bridge, the ribbon is stressed in compression which increases the stiffness of the structure. Such bridges are typically made RCC structures with tension cables to support them. They are primarily used for pedestrians but bicycles may be allowed based on design. Such bridges, generally are maintenance free, architecturally appeasing and economical when compared with their spans. The slender deck allows them to make the minimum use of construction material. In the current scenario, research is being carried out to find the most viable variation of the structure by combining it with arches. Fig. 1 Redding Pedestrian stress ribbon bridge. There are 3 types of stress ribbon bridges, namely traditional, stress ribbon bridges supported on an arch and stress ribbon bridge suspended on an arch. Fig. 1 is an example of a traditional stress ribbon bridge. For stress ribbon bridges supported on arches, the arch acts as a temporary support wherein the deck can rise during and fall during various loading states and temperature fluctuations. The Fig. 2a shows the general structural arrangement of a stress ribbon bridge supported on arches. In its initial stages, it resembles its behaviour as a two-span cable, supported by the central support that is anchored to the end abutments (ref. Fig.2b). The supporting arch is stressed by its own weight in addition to that of the deck, the self-weight of the support members and the radial forces exerted by the tensioned cables (ref. Fig.2c) [4]. After post- tensioning the entire structure behaves as one. The thrust forces in the stress ribbon HSR and the arch HA play a critical role since they have to be chosen in such a
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________________ Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 96 manner that they are equal. If the aforementioned criteria are met, the stress ribbon and the arch can be connected by and inclined strut which shall primarily be in compression. An overturning moment shall be created by cable thrust HSR*h which shall be balanced by the arch reaction ΔV*LP. Hence a self-balancing mechanism is created (ref Fig.2d) [4]. Another alternative is to suspend the stress-ribbon fromthe arch. Self-balancing systems can be made for the same as well. Fig. 3a, shows a fixed arch at the end anchorages of a slender prestressed concrete deck. The loadings on the arch is its ownself weight in addition to the self-weight of the stress-ribbon combined with the radial forces of the tensioning cables. Fig. 3bpresents a statically similar structure as represented in Fig. 2d. Fig. 3 c presents a condition wherein the thin prestressed deck with additional flexural rigidity in the unsupported section of the structure [[4]]. Fig. 2 Stress ribbon supported by arch. Fig. 3 Stress ribbon suspended on arch. The aim of the present study is to analyse a traditional stress ribbon for a span of 45 meters for IRC loading conditions and a safety check for pedestrian excitation. 2.MODELING AND ANALYSIS RESULTS The deck segment selected was 4 meters wide, 250 mm thick and 1 meter long. The bridge would consist of 45 such segments supported on bearing cables. The meshing was performed according to the length of segments. The deck had to be given a sag by the formula 𝑓 = 0.02 ∗ 𝐿 where L is the length of the bridge [3]. The final geometric model of the bridge is shown in Fig. 4. Fig. 4 Final geometric model. The structure was loaded with live, wind and temperature loads as per IRC 6-2010. Wind and temperature loads were calculated for Mumbai region. The force in the bearing cable was calculated as per 𝑃 = 𝑤∗𝐿2 8∗𝑓 , where w is the self weight intensity of the bridge deck [3]. The cable forces come to 7320 kN which will require 4 12K15 prestressing cables to transfer the load to the abutment. The structure was analyzed in ANSYS for the individual load cases and load combinations as per IRC 6-2010. The results are shown in table 1. Table 1. Loading Results Sr. No. Load Case Bending Moment (kNm) Maximum Deflection (mm) Sag Hog 1 Live Load 104 212 65.66 2 Transverse Wind Load - - 0.3 3 Vertical Wind Load 36 72 22.36 4 Temperature Load (+) 80 158 49.26 5 Temperature Load (-) 158 80 49.26 (upward) 6 Normal Combination 104 212 65.66 7 Temperature Combination 184 370 115 8 Wind & Temperature Combination 219 443 137.3
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________________ Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 97 The critical load combination in terms of prestressing steel comes out to the temperature combination which also proves that stress ribbons are critical to temperature [3]. It was for this combination the design was carried out as per IRC 18- 2000 manually and 6, 4K15 cables stressed at a force of 800 kN each, including losses was found out as the post tensioned steel requirement. The structure was then analyzed for the different critical prestressing conditions in ANSYS and the deflection for the structure in the final state under temperature combination and prestress is shown in Fig. 5. Also since stress is an important parameter under prestressing conditions the maximum stress results under temperature combination and prestress are also shown in Fig. 6. The table 2 shows the results due to prestress under transfer and temperature combination. Non critical cases and bending moments are not mentioned in table 2. Minimum reinforcement in the form of untensioned steelhas to be provided in the segments for safety against temperature. Fig. 5 Deflection due to temperature combination and prestress in meters. Fig. 6 Stress due to temperature combination and prestress in kN/m2. Table 2. Prestressing Results Sr. No. Load Case Bending Moment (kNm) Maximum Deflection (mm) Stress (N/mm2) Sag Hog 1 Dead Load & Prestress 217 106 67.08 (upward) 10.16 (Comp) & 0.233 (Tensile) 2 Prestress & Temperat ure Combinati on - - 47.84 4.06 (Comp) & 3.31 (Tensile) The initial approach was to design a standard abutment that is generally used for bridges with the proportioning of its dimensions as given in standard books used for bridge engineering. The drawback however was that the horizontal deflection of the abutment due to the cable forces was very high, almost 400 mm deflection for 5 meter height of the abutment. Hence a stepped abutment was taken into consideration whose deflections were much lesser than the standard abutment. The cross sectional dimensions of the stepped abutment are shown below in Fig. 7. The top width of the abutment is 4 m which is the width of the deck of the bridge. A gradually decreasing drop of around 300 mm is provided so as to accommodate the first segment of the deck having a depth of 250 mm and an extra 50 mm for the provisions of elastomeric bearings while maintaining the slope of the deck. The bottom width of the abutment provided is 9 m so as to satisfy the S.B.C. conditions of the strata below. The stratumbelow is assumed as rock having a S.B.C. value of 900 kN/m2. Fig. 7 Abutment cross section. The most critical loading condition for the abutment is the cable forces acting on it [3] and structural engineers around the world design the abutment for cable forces only. The
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________________ Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 98 abutment was analyzed for cable forces in ANSYS and the bending moment results for the same are shown in Fig. 8. The design was performed manually as per IRC 21-2000 and the untensioned reinforcement for the top part of the abutment comes out to 20 tor bars @125 mm c/c and for the bottompart comes out to 32 tor bars @ 100 mm c/c. Fig. 8 Bending moment in abutment due to cable force in kNm. While most bridge abutments have only compressive forces on the soil, a stress ribbon bridge abutment will also have tension on its abutment base. The soil pressure results are shown in Fig. 9 under normal working conditions without any soil improvement methods. It is due these high tension forces on the abutment, rock anchoring is generally suggested to keep the abutment in place. Fig. 9 Soil pressure results. 3. DYNAMIC ANALYSIS AND PEDESTRIAN EXCITATION There are three primary mode shapes for the deck, namely, vertical, lateral and torsion modes. The first three modes are vertical. The first lateral mode is the fourth mode and the first torsional mode is the seventh mode. The first two vertical modes have a frequencies f1=1.379 Hz and f2=1.788 Hz respectively and the mode shapes are shown in Fig. 10 and Fig. 11 respectively. Normal practice suggests that that the second mode f2shape should actually be the first mode shape but, this mode requires an elongation of the cable, hence the corresponding frequency in some cases is higher and mode shape of f1 becomes the first mode [3]. The first lateral mode is the fourth mode of the structure with a frequency f4=3.959 Hz. Due to the vertical curvature of the prestressed band, a horizontal movement is always combined with torsion and it is therefore difficult to find a pure torsional mode [3]. The first torsional mode is the seventh mode for the structure with a frequency of f4=7.129Hz. Both the mode shapes are shown in Fig. 12 and Fig. 13 respectively. Fig. 10Mode shape for frequency f1=1.379 Hz. Fig. 11 Mode shape for frequency f2=1.788 Hz. Fig. 12 Mode shape for frequency f4=3.959 Hz. Fig. 13 Mode shape for frequency f7=7.129 Hz.
  • 5. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________________ Volume: 05 Issue: 08 | Aug-2016, Available @ http://ijret.esatjournals.org 99 Stress ribbon bridges are very slender in nature and have a natural frequency very close to the pedestrian walking frequency of 2 Hz [1], [4], [5]. The codes of choice for structural engineers around the world for pedestrian excitation analysis are The British Standard BS 5400 Part 2 and Ontario Highway Bridge Design Code OHBDCONT 83 [3], [6]. For this article, I have used fib 32 guidelines and BS 5400 limiting criteria. The fib 32 has a calculation method which determines the maximum vertical acceleration resulting from the passage of one pedestrian walking / running with a pace rate equal to the fundamental natural frequency of the bridge. Therefore, it is modelled as an equivalent single degree-of-freedom oscillator. The formula is given below, 𝑎 = 4 ∗ 𝜋2 ∗ 𝑓2 ∗ 𝑦 ∗ 𝛼 ∗ ∅ Where, a= Acceleration in m/s2, f= Vertical natural frequency of the bridge in Hz, y= Static deflection at mid span in m for a force of 700N, α = Fourier coefficient of the relevant harmonic of the walking or running rate, ∅ = Dynamic amplification factor for one pedestrian moving across simple span (See Fig. 14). Fig. 14 Dynamic amplification factor. For given conditions, the value of α would be 0.4 for a step frequency of 2 Hz for the first natural frequency and number of cycles per span for a 45 m span bridge is 60 [2]. BS 5400 Part 2 also considers the higher order harmonics of the structure and hence it has a limiting value of frequencies to be considered till 5 Hz. However research has shown that higher order harmonics (frequency above 2.4 Hz) will not produce important oscillations in a structure due to the lower force component of higher harmonics [2]. The permissible vertical acceleration is, 𝑎 𝑉,𝑚𝑎𝑥 = 0.5 ∗ √ 𝑓. The results of pedestrian excitation is given in table 3. Table 3 Pedestrian Excitation Results Frequency (Hz) y (m) α  a (m/ss ) aV,max(m/ss ) f1=1.379 0.000508 0.4 25 0.381682 0.587154 f2=1.788 0.000508 0.1 25 0.160416 0.668581 The above table shows that the vertical accelerations of the bridge deck for the first two frequencies are well within the permissible limits and hence the pedestrians will not feel discomfort while walking on the bridge. Hence the bridge will be safe from pedestrian excitation at its critical frequencies. 4. CONCLUSION The basic objective of this study is to elaborate on what a stress ribbon bridge is, its types and its advantages over conventional pedestrian bridges. This study elaborates on the various parameters essential before the actual design or analysis and the sources from which they are obtained. It also briefly explains the process of modelling, loading and analysis of a stress ribbon bridge in ANSYS. The critical conditions were identified and designed for manually. In this study a model of a stress ribbon bridge of 45 meter span is modelled and analyzed using ANSYS version 12. the following conclusions can be made:  Design of stress ribbon structures have confirmed that a slender concrete deck supported by an internal and/or external cables can be very efficient.  Their designs have to be based on understanding of the cable tension, bending stiffness and on the understanding of the function of the prestressed concrete deck.  The bending moment in a stress ribbon bridge is much lesser when compared to a beambecause of its inverted arch shape.  Temperature is a critical condition in a stress ribbon bridge due to its slender deck and flexible nature.  The abutment has to transfer high cable forces due to which it requires a very good stratumbelow it (preferably rock). REFERENCES [1] D. E. Newland, 2004. “Pedestrian excitation of bridges”, Institution of Mechanical Engineers (IMechE), Volume 218, Part C, 477-492. [2] Jiri Strasky, et al., 2005. “Guidelines for the design of footbridges”, federation internationale du béton (fib), Bulletin 32. [3] Jiri Strasky, 2006. “Stress Ribbon and Cable Supported Pedestrian Bridges”, Academy of Sciences of the Czech Republic, Brno, Czech Republic. [4] Jiri Strasky, 2008. “Stress Ribbon Pedestrian Bridges Supported or Suspended on Arches”, Chinese-Croatian joint colloquium, Long Arch Bridges, Brijuni Islands, Croatia, 135-147. [5] Jiri Strasky, 2010. “Stress Ribbon and Arch Pedestrian Bridges”, 6th International Conference on Arch Bridges, Fuzhou, China, 38-45. [6] Dr. Chung C. Fu, “Dynamic Response of Pedestrian Bridges”, Research Professor, University of Maryland.