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Report No. SRR-91 Final Report DEVELOPMENT OF A RELIABILITY-BASED DESIGN PROCEDURE FOR HIGH-MAST LIGHTING STRUCTURAL SUPPORTS IN COLORADO John W. van de Lindt Jonathan S. Goode March 2006 COLORADO DEPARTMENT OF TRANSPORTATION SAFETY AND TRAFFIC ENGINEERING BRANCH AND STAFF BRIDGE BRANCH

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Page 1: DEVELOPMENT OF A RELIABILITY-BASED DESIGN …s3.amazonaws.com/zanran_storage/ LIGHTING STRUCTURAL SUPPORTS IN COLORADO 5. ... for a specified wind velocity. Within the fatigue analysis,

Report No. SRR-91 Final Report

DEVELOPMENT OF A RELIABILITY-BASED DESIGN PROCEDURE FOR HIGH-MAST LIGHTING STRUCTURAL SUPPORTS IN COLORADO John W. van de Lindt Jonathan S. Goode

March 2006 COLORADO DEPARTMENT OF TRANSPORTATION SAFETY AND TRAFFIC ENGINEERING BRANCH AND STAFF BRIDGE BRANCH

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The contents of this report reflect the views of the

authors, who are responsible for the facts and

accuracy of the data presented herein. The contents

do not necessarily reflect the official views of the

Colorado Department of Transportation. This

report does not consitute a standard, specification,

or regulation. Any information contained herein

should be used at the users own risk.

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Technical Report Documentation Page 1. Report No. Structural Research Report (SRR)-91

2. Government Accession No.

3. CDOT Project Manager Richard Osmun

4. Title and Subtitle DEVELOPMENT OF A RELIABILITY-BASED DESIGN PROCEDURE FOR HIGH-MAST LIGHTING STRUCTURAL SUPPORTS IN COLORADO

5. Report Date March 2006

7. Author(s) John W. van de Lindt and Jonathan S. Goode

6. Performing Organization Code Colorado State University

9. Performing Organization Name and Address Colorado State University Department of Civil Engineering Campus Mail Stop 1372 Fort Collins, CO 80523-1372

8. Performing Org Report No. SRR-91

10. Work Unit No. (TRAIS)

12. Sponsoring Agency Name and Address Colorado Department of Transportation – Safety and Traffic Engineering Branch 4201 E. Arkansas Ave. Denver, CO 80222

11. Contract Number:

13. Type of Report & Period Covered Final Report, 2004-2005

15. Supplementary Notes

14. Sponsoring Agency Code File: 81.30

16. Abstract High mast lighting structures are being used to provide illumination for large intersections, particularly for highways located in rural areas. These structures, ranging from approximately 50 – 130 ft (15 – 40 m) in height, are exposed to high wind forces that in turn produce a tremendous number of loading cycles each year. A recent high mast lighting structural support failure in the high plains of Colorado near Denver International Airport provided the impetus for this study. Specifically, a numerical investigation to determine the nature of the complex dynamic response, estimate the fatigue life, and determine the effect of extreme wind gusts known as micro-bursts on this dynamic response as well as the effect on the resulting fatigue life. These high-mast structures are less than 3.28 ft (1 m) in diameter and are quite flexible relative to many civil engineering structures. This flexibility results in large deformations when compared to their diameter, i.e. when combined with the height of these structures. Furthermore, large forces and moments at the base are produced that result in large stresses and stress reversals during multi-mode excitation. Morison’s equation, which provides relative force for slender bodies as a function of flow velocity, was applied within a dynamic finite element framework in order to account for the relative motion between the wind and the motion of the structure. Then, a well-known random vibrations approach was coupled with Miner’s rule to estimate the fatigue life of the structural support. Six different design parameters as well as mean wind velocities were examined and an approximate reliability-based design procedure was developed based on these results. Several examples are presented to illustrate the new approach. However, in order for the approach to be appropriately applied to high-mast lighting structural supports in Colorado it is strongly recommended that a state-wide wind study be undertaken to provide accurate reliability indices for all traffic and safety structures such as signal poles, overhead signs, and high-mast lights. 17. Key Words: high mast lighting, fatigue, structural

reliability, steel design, wind loading

18. Distribution Statement No restrictions. This document is available to the public through: National Technical Information Service 5825 Port Royal Road Springfield, VA 22161

19. Security Classification (report) None

20. Security Classification (Page) None

21. No of Pages 99

22. Price

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DEVELOPMENT OF A RELIABILITY-BASED DESIGN

PROCEDURE FOR HIGH-MAST LIGHTING

STRUCTURAL SUPPORTS IN COLORADO

by

John W. van de Lindt, Associate Professor

Jonathan S. Goode, Ph.D. Student

Report No. SRR-91

Sponsored by the

Colorado Department of Transportation

March 2006

Colorado Department of Transportation

Safety and Traffic Engineering Branch

4201 E. Arkansas Ave.

Denver, CO 80222

(303) 757-9506

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ACKNOWLEDGEMENTS

This project was funded by the Colorado Department of Transportation (CDOT) – Safety and

Traffic Engineering Branch and Staff Bridge Branch. That support is gratefully acknowledged

by the authors. Dick Osmun, the project manager, provided advice and support during the

project and the authors thank him for his assistance. The second author would also like to thank

the American Institute of Steel Construction (AISC) – Rocky Mountain Region, for providing a

Graduate Fellowship, which provided funding for the latter portion of his participation in this

study.

Opinions expresses in this report are, however, those of the writers and do not necessarily reflect

those of CDOT or AISC.

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EXECUTIVE SUMMARY

High mast lighting structures are being used to provide illumination for large intersections,

particularly for highways located in rural areas. These structures, ranging from approximately

50 – 130 ft (15 – 40 m) in height, are exposed to high wind forces that in turn produce a

tremendous number of loading cycles each year. A recent high mast lighting structural support

failure in the high plains of Colorado near Denver International Airport provided the impetus for

this study. Specifically, a numerical investigation to determine the nature of the complex

dynamic response, estimate the fatigue life, and determine the effect of extreme wind gusts

known as micro-bursts on this dynamic response as well as the effect on the resulting fatigue life.

These high-mast structures are less than 3.28 ft (1 m) in diameter and are quite flexible relative

to many civil engineering structures. This flexibility results in large deformations when

compared to their diameter, i.e. when combined with the height of these structures. Furthermore,

large forces and moments at the base are produced that result in large stresses and stress reversals

during multi-mode excitation. Morison’s equation, which provides relative force for slender

bodies as a function of flow velocity, was applied within a dynamic finite element framework in

order to account for the relative motion between the wind and the motion of the structure. Then,

a well-known random vibrations approach was coupled with Miner’s rule to estimate the fatigue

life of the structural support. Six different design parameters as well as mean wind velocities

were examined and an approximate reliability-based design procedure was developed based on

these results. Several examples are presented to illustrate the new approach.

The procedure for the development of the reliability-based design procedure can be broken into

six steps. These steps constitute the six major components of the general analysis procedure

presented in this report. This general analysis procedure is briefly described as:

Step 1: Construction of the finite element model of the HML structural support.

Step 2: Fatigue analysis performed in order to determine the fatigue life of the structure

for a specified wind velocity. Within the fatigue analysis, Steps 3 – 5 must also

be performed in a repetitive fashion.

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Step 3: Construction of the wind-loading model to determine the loading applied to the

finite element model.

Step 4: Dynamic analysis performed to determine the motion of the system as a function

of time.

Step 5: Resolve non-linearity of the wind-loading model applied to the finite element

model.

Step 6: Reliability analysis performed in order to determine the reliability index for a

specified target fatigue life.

However, in order for the approach to be appropriately applied to high-mast lighting structural

supports in Colorado it is strongly recommended that a state-wide wind study be undertaken to

provide accurate reliability indices for all traffic and safety structures such as signal poles,

overhead signs, and high-mast lights.

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TABLE OF CONTENTS

SECTION PAGE

CHAPTER 1 INTRODUCTION

1.1 Background and Motivation ..........................................................................................1

1.2 Scope of Research Project and Objectives.....................................................................3

1.3 Summary of Current Design Guidelines: AASHTO 2001 ............................................4

1.4 Overview of Report........................................................................................................7

CHAPTER 2 ANALYSIS PROCEDURES AND METHODS

2.1 General Analysis Procedure...........................................................................................8

2.2 Finite Element Model ..................................................................................................10

2.3 Wind Load Model ........................................................................................................14

2.4 Dynamic Analysis........................................................................................................21

2.5 Relative Motion ...........................................................................................................23

2.6 Fatigue Analysis...........................................................................................................25

2.7 Reliability Analysis......................................................................................................31

CHAPTER 3 SENSITIVITY AND RELIABILITY ANALYSES

3.1 Sensitivity Analysis Background.................................................................................34

3.2 The Mean Wind Velocity.............................................................................................38

3.3 Sensitivity Analysis .....................................................................................................39

3.4 Reliability Analysis......................................................................................................47

CHAPTER 4 RELIABILITY-BASED DESIGN METHODOLOGY

4.1 Design Methodology Background ...............................................................................67

4.2 Design Charts – Single Variable..................................................................................68

4.3 Design Method – Single Variable................................................................................68

4.4 Design Charts – Multiple Variables.............................................................................74

4.5 Design Method – Multiple Variables...........................................................................74

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SECTION PAGE

CHAPTER 5 ILLUSTRATIVE DESIGN EXAMPLES FOR FATIGUE PERFORMANCE

5.1 Example 1 – Single Variable .......................................................................................78

5.2 Example 2 – Multiple Variables ..................................................................................79

CHAPTER 6 SUMMARY, CONCLUSIONS AND RECOMMENDATIONS..........................81

REFERENCES ..............................................................................................................................83

APPENDIX A

A.1 Vortex-Induced-Vibration......................................................................................... A-1

A.2 Selected Mean Wind Velocities................................................................................ A-3

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LIST OF FIGURES

FIGURE PAGE

1-1 HML Structure in Colorado .....................................................................................1

1-2 Base-Line Reliability Indices for HML Structural Support.....................................7

2-1 General Analysis Procedure.....................................................................................9

2-2 Finite Element Model Procedure ...........................................................................11

2-3 Boundary Support Conditions Model ....................................................................13

2-4 Wind Velocity Time Series Procedure ..................................................................15

2-5 In-Line Wind Velocity Power Spectrum ...............................................................16

2-6 In-Line Wind Velocity Time Series.......................................................................18

2-7 Wind Loading Procedure .......................................................................................18

2-8 Logarithmic Wind Velocity Profile .......................................................................19

2-9 Drag Coefficient for a Smooth Cylinder................................................................21

2-10 Dynamic Analysis Procedure.................................................................................22

2-11 Relative Motion Procedure ....................................................................................24

2-12 Relative Velocity of Wind and HML Structure.....................................................25

2-13 Fatigue Analysis Procedure ...................................................................................26

2-14 Lognormal PDF .....................................................................................................30

2-15 Lognormal PDF Bins .............................................................................................30

2-16 Reliability Analysis Procedure ..............................................................................31

3-1 Benchmark HML Structural Support in Colorado.................................................35

3-2 Wind Velocity Parent Distribution ........................................................................39

3-3 Fatigue Life Sensitivity – Pole Outside Diameter .................................................40

3-4 Fatigue Life Sensitivity – Pole Wall Thickness.....................................................41

3-5 Fatigue Life Sensitivity – Pole Length ..................................................................42

3-6 Fatigue Life Sensitivity – Luminaire Structure Weight.........................................42

3-7 Fatigue Life Sensitivity – Luminaire Structure Projected Area.............................43

3-8 Fatigue Life Sensitivity – Structure Damping .......................................................44

3-9 Fatigue Life Sensitivity – Wind Velocity COV.....................................................45

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FIGURE PAGE

3-10 Fatigue Life Sensitivity – Wind Gust ....................................................................45

3-11 Reliability Analysis – Pole Outside Diameter .......................................................48

3-12 Reliability Analysis – Pole Wall Thickness...........................................................51

3-13 Reliability Analysis – Pole Length ........................................................................54

3-14 Reliability Analysis – Luminaire Structure Weight...............................................57

3-15 Reliability Analysis – Luminaire Structure Projected Area ..................................60

3-16 Reliability Analysis – Structure Damping .............................................................63

3-17 Reliability Analysis – Wind Velocity COV...........................................................65

5-1 Example 1 – Single Variable .................................................................................78

5-2 Example 2 – Multiple Variables ............................................................................80

A-1 Selected Locations in Colorado .......................................................................... A-4

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LIST OF TABLES

TABLE PAGE

2-1 Common Reliability Indices, β ..............................................................................33

3-1 HML Structural Support Properties – Pole Sections .............................................36

3-2 HML Structural Support Properties – Joint Sections.............................................37

3-3 HML Structural Support Properties – Boundary Support Conditions ...................37

3-4 HML Structural Support Properties – Luminaire Structure Properties .................38

4-1 Benchmark HML Structural Support Properties....................................................69

4-2 Pole Outside Diameter Properties..........................................................................70

4-3 Pole Wall Thickness Properties .............................................................................70

4-4 Pole Section Length Properties..............................................................................71

4-5 Luminaire Structure Projected Area Properties .....................................................71

4-6 Design Method Confirmation Examples – Single Variable ..................................72

4-7 Design Method Confirmation Summary – Single Variable...................................72

4-8 Design Method Confirmation Properties – Single Variable ..................................73

4-9 Design Method Confirmation Percent Changes – Single Variable .......................73

4-10 Design Method Confirmation Examples – Multiple Variables .............................75

4-11 Design Method Confirmation Summary – Multiple Variables..............................76

4-12 Design Method Confirmation Properties – Multiple Variables.............................76

4-13 Design Method Confirmation Percent Changes – Multiple Variables ..................77

A-1 Wind Speed and Vibration Mode Combinations at which Lock-In was

Numerically Identified ........................................................................................ A-3

A-2 Mean Wind Velocities for Selected Locations in Colorado ............................... A-4

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1

CHAPTER 1

INTRODUCTION

1.1 Background and Motivation

The Colorado Department of Transportation (CDOT) maintains a large number of high mast

lighting (HML) structures in the state of Colorado. These structures, as shown in Figure 1-1, are

primarily used to illuminate large intersections along major arterials and in rural areas. Quite

often, HML structures have heights ranging from 50 – 130 ft (15 – 40 m) with base diameters of

approximately 1.5 ft (460 mm). The main advantage of using HML structures, as opposed to

standard luminaire structures, is the substantial reduction in the total number of structures

required for a specified area.

Figure 1-1: HML Structure in Colorado

On April 11, 2004, two HML structures located at the intersection of E-470 (a toll road) and

Pena Boulevard near Denver International Airport (DIA) failed. These failures resulted in

several HML structures being retrofitted and many more being constantly monitored in that area.

As a result, a substantial economic investment by the E-470 Authority has been required

following these collapses. As always, the safety of the general public is a primary concern since

many HML structures in Colorado, as well as other states, are relatively close to the roadway.

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This combination of economic factors and safety concerns has provided the impetus for this

study.

An investigation conducted by the Advanced Technology for Large Structural Systems (ATLSS)

Engineering Research Center at Lehigh University (Kaufmann, 2005) revealed several

possibilities for the failure of these structures. Conclusions concerning one of the collapsed

structures indicated failure primarily due to the initiation and propagation of fatigue cracks

occurring under high stress cycles. Further investigation of the collapsed structure showed little

evidence of significant corrosion on the crack surface. Reasons for this could be due to the

evidence of high crack propagation rates. Thus, the failure of the structure was likely due to a

short time period event. Indeed, during the hours preceding the failure, there were reports of a

high wind weather event in the area near DIA.

During the investigation, Kaufmann (2005) also conducted chemical and strength property

analyses of the structural steel tubing comprising the HML structural support. The chemical

composition and tensile properties were similar and consistent with Grade 60 steel utilized in

fabricating structural steel tubing. The investigation concluded that the properties of the

structural steel tubing did not directly contribute to the development of the fatigue cracks.

Kaufmann’s investigation also made note of several quality assurance issues that may have

contributed to the failure of these structures. Concerning the collapsed structure, the specified

wall thickness of the structural steel tubing according to design documents was to be 0.25 in

(6.35 mm). However, the actual wall thickness was measured as 0.235 in (5.97 mm), or 6% less

than specified requirements. The sensitivity of fatigue life to wall thickness is significant, as will

be shown in Chapter 3 of the current report. Other structures sent to ATLSS, none of which

collapsed but did show signs of fatigue cracking, had specified wall thicknesses of 0.1875 in

(4.76 mm). Actual measurements indicated wall thicknesses of 0.189 in (4.80 mm), or 0.8%

above specified requirements. One final structure was also tested that did not show any signs of

fatigue cracking. The specified wall thickness was given as 0.25 in (6.35 mm). The actual wall

thickness was determined to be 0.230 in (5.84 mm), or 8% less than specified requirements.

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The American Society for Testing Materials (ASTM) Standard A595 (ASTM, 2002), Standard

Specification for Steel Tubing, Low-Carbon, Tapered for Structural Use, specifies dimensions

and tolerances related to the HML structural supports. The specification covers three grades of

seam-welded, tapered steel tubes for structural use with diameters ranging from 2.375 – 30 in

(60.325 – 762.0 mm) and wall thicknesses ranging from 0.1046 – 0.375 in (2.657 – 9.525 mm).

Tolerances for wall thickness are given as +10% to –5% of the specified wall thickness exclusive

of the weld area. Based on Kaufmann’s investigation, the collapsed structure, with an actual

wall thickness of 6% less than specified requirements, falls outside the acceptable tolerance

based on the ASTM standard. The structure that showed no signs of fatigue cracking also falls

outside the acceptable range of tolerance. Finally, the structures that did show signs of fatigue

cracking, with actual wall thicknesses 0.8% greater than specified, did fall within the ASTM

tolerance range.

1.2 Scope of Research Project and Objectives

Due to the overwhelming evidence of fatigue damage being the primary cause for the failure of

the aforementioned HML structural supports, the focus of this project is on fatigue damage

induced by cyclic loading. The American Association of State Highway and Transportation

Officials (AASHTO, 2001) define fatigue as “damage resulting in fracture caused by stress

fluctuations”. Due primarily to wind fluctuations, HML structures are subjected to a tremendous

number of loading cycles each year. These wind fluctuations in combination with the height of

these structures result in large forces and moments at their bases. Adding to the large number of

potential loading cycles is the possibility of higher modes of vibration. For slender structures of

this height, a common occurrence can be the presence of higher modes of vibration thus

substantially increasing an already large number of loading cycles. There is also the possibility

of vortex-induced vibration, commonly referred to as vortex shedding, which results in a

phenomenon known as lock-in. A preliminary investigation into HML structure lock-in

frequencies is included in this report for completeness.

This project will develop a semi-prescriptive design procedure for HML structural supports in

Colorado. This design procedure will statistically provide a minimum, or target, structural

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reliability index, as prescribed by CDOT. The design procedure will consider many factors

affecting HML structural supports. At the front of this effort are wind-engineering principles

concerning fluid/structure interaction that will help to determine the dynamic response of the

structure to a simulated wind event. Using a finite element approach, the resulting forces and

stresses produced at the base of the structure can then be determined. A linear damage

accumulation model will predict the fatigue life of the HML structural support. Probabilistic

methods will be used to determine reliability indices and then transformed into appropriate

design guidelines. Base-line reliability indices for existing structural supports will also be

determined.

1.3 Summary of Current Design Guidelines: AASHTO 2001

AASHTO 2001 Standard Specifications for Structural Supports for Highway Signs, Luminaires

and Traffic Signals is the national standard for the current design guidelines for HML structural

supports. This section considers the current design guidelines, AASHTO 2001, applied to the

benchmark HML structural support outlined in Chapter 3. AASHTO considers two wind-

loading cases for fatigue design for HML structural supports. The intent of the fatigue design is

that the connection detail or structural member, defining a detail category, will have infinite

fatigue life and, as such, stresses produced will remain below a threshold limit. The detail

category used for the HML structural support is questionable. Based on the attachment of the

HML structural support to the base plate with a 0.25 in (6.35 mm) thick backing ring attached to

both the HML structural support and the base plate with seam welds, the detail category is E′ if

the backing ring is not removed accordingly. However, this detail category is very undesirable

in terms of fatigue design. Thus, it is possible that a detail category of E could be achieved by

removing the backing ring after the initial placement of the HML structural support and welding

the pole to the base plate. For completeness, this report will consider both detail categories.

AASHTO defines fatigue importance factors for the two wind-loading cases. Assuming that all

HML structural supports are located on major highways and are critical structures, an importance

factor category of I is assigned. Thus, for the two wind-loading cases, the fatigue importance

factor, IF, is 1.0.

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Natural Wind Gust

The equivalent static natural wind gust pressure, PNW, is defined as,

(Pa)I250CP

(psf)I5.2CP

FdNW

FdNW

=

= (1-1)

where IF is 1.0 and the drag coefficient, Cd, is determined as a function of a conversion factor, Cv

= 1 for a 3-second 50-year wind gust, the 50-year wind velocities of 90 MPH (144.84 km/hr),

100 MPH (160.93 km/hr), and 110 MPH (177.03 km/hr), and the average diameter of each

section, d. The drag coefficient is determined to be 0.45 for all sections and all wind velocities.

The luminaire structure has a drag coefficient of 1.0 as given by CDOT design specifications

referenced in Chapter 3 of this report. The equivalent static natural wind gust pressure along the

height of the pole is calculated as 2.34 psf (112.5 Pa) for all three wind velocities above and the

resulting pressure on the luminaire structure is calculated as 5.2 psf (250 Pa). Applying this

pressure along the height of the pole, making note of the reduction in outside diameter as height

increases, and on the luminaire structure, the overturning moment at the base of the structure is

calculated to be 345 k-in (38.98 kN-m). The stress due to this overturning moment at the base of

the structure is finally calculated to be 1.81 ksi (12.41 MPa).

For detail category E, AASHTO indicates that the constant-amplitude fatigue threshold is given

as 4.5 ksi (31 MPa). Thus, the stress due to the overturning moment produced by the equivalent

static natural wind gust is lower than the threshold indicated. For detail category E′, AASHTO

indicates that the constant-amplitude fatigue threshold is given as 2.6 ksi (18 MPa). Thus, the

stress due to the overturning moment produced by the equivalent static natural wind gust is also

lower than the threshold indicated.

Vortex-Shedding

The second wind-loading case for fatigue that AASHTO requires HML structural supports to be

checked is vortex shedding. A more complete discussion of this topic is provided in the

appendix of this report. AASHTO indicates that the critical wind velocity, Vc, at which vortex

shedding lock-in can occur is,

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n

nc S

V df= (1-2)

where fn is the first transverse natural frequency of the structure in cyc/sec, d is the diameter of the

structure in ft (or m), and Sn is the Strouhal number given as 0.18 for circular sections. From a

finite element program written by the authors, fn is determined to be 0.5275 cyc/sec and d is taken

as the average diameter of the structure, 1.5075 ft (0.4595 m). Thus, the critical wind velocity at

which vortex shedding lock-in can occur is calculated to be 4.4178 ft/s (1.3465 m/s) or 3.01

MPH (4.848 km/hr). The vortex shedding model discussed in the appendix for the first

transverse mode confirms this same velocity for the HML.

Using the critical wind velocity, the equivalent static vortex shedding pressure, PVS, can be

calculated as,

(Pa)2ξ

IC0.613VP

(psf)2ξ

IC0.00118VP

Fd2C

VS

Fd2C

VS

=

=

(1-3)

where ξ is the damping ratio given as 0.005 by AASHTO. Using the critical wind velocity as

4.4178 ft/s (1.3465 m/s), the drag coefficient as 1.10 updated for a wind velocity of 3.01 MPH

(4.848 km/hr), and the importance factor as 1.0, the equivalent static vortex shedding pressure is

calculated as 2.53 psf (121.14 Pa). Noting that this pressure is not an appreciable increase over

the pressure caused by a natural wind gust, 2.34 psf (112.5 Pa), it is concluded that the stress due

to the overturning moment at the base of the structure will not exceed the constant-amplitude

fatigue threshold for detail category E of 4.5 ksi (31 MPa) or E′ of 2.6 ksi (18 MPa).

Base-Line Reliability Indices

The benchmark HML structural support considered in this study, further discussed in Chapter 3,

has a reliability index for a given wind velocity and target fatigue life. Figure 1-2 depicts the

base-line reliability indices for this benchmark HML structural support in Colorado for target

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fatigue life’s of 25 years, 50 years, and 75 years for detail category E, figure (a), and detail

category E′, figure (b). As will be discussed in Chapter 3 of this report, wind velocities in Figure

1-2 remain as mean or average wind velocities over the life of the structure. Also in Chapter 3 of

this report, several characteristics of this benchmark structure will be varied and analyzed.

(a): Detail Category E (b): Detail Category E′

Figure 1-2: Base-Line Reliability Indices for HML Structural Support

1.4 Overview of Report

Chapters 2 – 5 consist of the development of the design procedure as previously discussed.

Chapter 2 illustrates an outline of the general procedure used in modeling the HML structural

support. Each step of the general procedure is further broken into individual procedures that

contribute to the end result. The approach used in this study regarding the mathematical

formulation is also presented to explain the theoretical derivation encompassing each step of the

procedure. Chapter 3 presents a sensitivity analysis of the fatigue life for given wind-loading

events with respect to variations in properties such as structure height, pole diameter, and pole

wall thickness among others. Reliability indices for various cases are also presented. Chapter 4

presents design guidelines as a result of the analyses shown in Chapter 3. Using the results of

Chapter 4, two illustrative design examples for fatigue performance are presented in Chapter 5.

A step-by-step method is given for both examples considered. Chapter 6 summarizes the design

procedure as given in Chapter 4 and illustrated in Chapter 5 of this study. Conclusions based on

this study are offered. Recommendations for future work and consideration are also given.

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CHAPTER 2

ANALYSIS PROCEDURES AND METHODS

2.1 General Analysis Procedure

The procedure for the development of the reliability-based design procedure can be broken into

six steps. These steps, as outlined in the flowchart shown in Figure 2-1, constitute the six major

components of the general analysis procedure presented in this report. This general analysis

procedure is briefly described as:

Step 1: Construction of the finite element model of the HML structural support.

Step 2: Fatigue analysis performed in order to determine the fatigue life of the structure

for a specified wind velocity. Within the fatigue analysis, Steps 3 – 5 must also

be performed in a repetitive fashion.

Step 3: Construction of the wind-loading model to determine the loading applied to the

finite element model.

Step 4: Dynamic analysis performed to determine the motion of the system as a function

of time.

Step 5: Resolve non-linearity of the wind-loading model applied to the finite element

model.

Step 6: Reliability analysis performed in order to determine the reliability index for a

specified target fatigue life.

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Construct FiniteElement Model(Section 2.2)

Apply FatigueAnalysis

(Section 2.6)

Construct WindLoading Model(Section 2.3)

Resolve Non-LinearWind Load

(Section 2.5)

Solve DynamicAnalysis of the

System(Section 2.4)Apply Reliability

Analysis(Section 2.7)

Figure 2-1: General Analysis Procedure

As indicated in Figure 2-1, each step corresponds to a section in Chapter 2 of this report.

Sections 2.2 – 2.7 further explain each of these steps. The theoretical details behind the models

and analyses used are discussed. This project only considered in-line wind velocity and the in-

line motion produced. As such, all details presented herein will be for two-dimensional analysis.

Changes to the finite element model, wind loading model, and stress combination would only be

needed for three-dimensional analysis. A discussion on vortex-induced-vibration, transverse

motion produced by an in-line wind velocity, is included in Appendix A of this report.

Section 2.2 discusses the finite element model and the procedure used in its construction. The

types of elements used are further explained for both stiffness and mass matrices. Application of

the boundary support and luminaire structure conditions is also discussed. Finally, the details on

the derivation of the structure damping matrix are presented. Section 2.3 discusses the wind-

loading model and the procedure used in its construction. The in-line wind velocity power

spectrum is presented. The procedure for determining the artificial wind velocity time series is

given. Finally, the details on the logarithmic profile and Morison’s equation are presented.

Section 2.4 details the dynamic analysis procedure as well as the theoretical details for its use.

The Newmark-Beta method is further discussed giving a step-by-step procedure for its use in this

project. Section 2.5 details the relative motion procedure. The calculation of the relative

velocity and application of Morison’s equation to obtain the updated forcing function to be used

in the dynamic analysis are presented. Section 2.6 details the fatigue analysis procedure. The

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method proposed by Crandall and Mark (1963), using the Palmgren-Miner rule, is derived. The

division of the lognormal probability density function (PDF) for wind velocity used to describe

the loading event is presented. Finally, Section 2.7 details the reliability analysis procedure.

Determination of the probability of failure and reliability index is also presented.

2.2 Finite Element Model

The procedure for constructing the finite element model of the HML structural support is

presented in Figure 2-2. The purpose for using a finite element approach is to determine the

properties of the structure in a discretized manner. These properties are then directly related to

solving the dynamic motion of the system using the equation of motion, which can be expressed

as,

[ ]{ } [ ]{ } [ ]{ } { })(tFxKxCxM =++ (2-1)

where the three matrices, M, C, and K, are the mass, damping, and stiffness matrices,

respectively. The forcing function, F(t), is nonlinear due to the relative motion between the wind

flow and the structure, and is discussed further in Section 2.3. The vectors, x, x , and x ,

represent the position, velocity, and acceleration, respectively, of the nodal points, or discretized

points representing the continuous system, of the structure.

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Loop throughNumber of Finite

Elements

Determine ElementStiffness Matrix

Determine ElementMass Matrix

End Loop

Apply BoundarySupport Conditions

Apply LuminaireStructure Conditions

Determine StructureDamping Matrix

Assemble StructureStiffness Matrix

Assemble StructureMass Matrix

Figure 2-2: Finite Element Model Procedure

The procedure presented in Figure 2-2 begins with the assembly of K and M. Each element of

the discretized structure has its own stiffness and mass matrix. These matrices are referred to as

the element stiffness and mass matrices. The elements used to construct the finite element model

are six degree-of-freedom beam elements (twelve degree-of-freedom beam elements for three-

dimensional analysis). Each end of the element has 3 degrees-of-freedom: axial deformation,

shear deformation, and bending-moment rotation. The element stiffness matrix can be expressed

as (Paz, 2004),

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[ ]

⎥⎥⎥⎥⎥⎥⎥⎥⎥⎥⎥⎥⎥

⎢⎢⎢⎢⎢⎢⎢⎢⎢⎢⎢⎢⎢

−−−

=

3232

22

3232

22

12061206

0000

604602

12061206

0000

602604

LEI

LEI

LEI

LEI

LEA

LEA

LEI

LEI

LEI

LEI

LEI

LEI

LEI

LEI

LEA

LEA

LEI

LEI

LEI

LEI

K e (2-2)

where E is the modulus of elasticity of the material comprising the element, A is the constant

cross-sectional area of the element, I is the constant moment of inertia of the element, and L is

the length of the element. The element mass matrix can be expressed as (Paz, 2004),

[ ]

⎥⎥⎥⎥⎥⎥⎥⎥

⎢⎢⎢⎢⎢⎢⎢⎢

−−−−

=

156022540130140007002204130354013156022070001400

13032204

420 22

22

LL

LLLLLL

LLLL

M HMLe

ρ (2-3)

where ρHML is the mass density per volume of the material comprising the element. Using a

transformation matrix, T, from local coordinate directions to global coordinate directions, the

stiffness and mass matrices used in Equation (2-1) are formed by,

[ ] [ ] [ ] [ ]

[ ] [ ] [ ] [ ]TMTM

TKTK

eT

eT

=

= (2-4)

Finally, all element stiffness and mass matrices are assembled into the structure stiffness and

mass matrices. This is accomplished based on a numbering or indexing scheme assigned to the

degrees-of-freedom for the structure.

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Boundary support conditions are applied to model the attachment of the HML structural support

to its foundation. These support conditions are represented by linear translational and rotational

springs placed at the base of the HML structural support, as shown in Figure 2-3, and are a

function of the foundation type and soil properties under the foundation. Because these springs

are considered to have no mass, only changes to the structure stiffness matrix are required.

RotationalSpring

TranslationalSpring

x

y

Figure 2-3: Boundary Support Conditions Model

Application of this type of model allows for experimental research to be conducted on actual

foundation connections. For this project, however, the foundation was modeled as a rigid

support. A rigid support is a conservative assumption whereas a foundation that allowed some

movement would actually increase the fatigue life of the structure.

Luminaire structure conditions are applied to model the luminaire structure attached at the top of

the HML structural support. The luminaire is considered to have a specified mass and projected

area for determining wind load. The mass is evenly distributed to translational degrees-of-

freedom to the top point of the structure mass. No contribution to the structure stiffness is

assumed.

The last step as indicated by Figure 2-2 is to determine the structure damping matrix, C. This

matrix is a linear combination of the structure stiffness and mass matrices and is given as

(Chopra, 2001),

[ ] [ ] [ ]KMC βα += (2-5)

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where the parameters, α and β, are determined as,

⎥⎦

⎤⎢⎣

⎡+

=

⎥⎦

⎤⎢⎣

⎡+

=

21

21

21

2

2

ωωξβ

ωωωωξα

(2-6)

where ω1 and ω2 are the first two circular natural frequencies of vibration for the restrained

structure, boundary support conditions applied, with the luminaire structure. The damping ratio,

ξ, is also used to determine the parameters for Rayleigh damping.

2.3 Wind Load Model

The procedure for applying the wind load model consists of two distinct parts. First, the wind

velocity time series for a specific height must be determined. Included in this part is the use of

an approximation of the in-line wind velocity power spectrum, which is essentially the energy

density as a function of frequency. Second, the wind velocity time series is then extruded along

the height of the structure following ASCE-7 (2005) and thus producing a wind velocity profile

through time. Using this wind velocity profile, the loading due to wind velocity is determined

based on drag force theory, or specifically a relative force equation known as Morison’s

equation.

The procedure for determining the wind velocity time series is presented in Figure 2-4.

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Loop throughFrequency

Determine FrequencyInterval

Calculate PowerSpectral Density

End Loop

Loop through Time

Assemble WindVelocity Time Series

End Loop

Start

Figure 2-4: Wind Velocity Time Series Procedure

The in-line wind velocity power spectrum, S(z,n), is given by (Simiu, 1996),

3/52* )501(

200),(ff

unznS

+= (2-7)

where n is frequency, u* is wind shear velocity, and f is given by,

( )zunzf = (2-8)

where z is height above ground and u(z) is the wind velocity at height z. By stepping through

frequency values, the in-line wind velocity power spectrum is calculated for a given wind

velocity at a specific, or characteristic, height. Using the international standard for wind velocity

measurements, and consistent with ASCE-7 (2005), the characteristic height is always assumed

to be 33 ft (10 m) for the calculation of the in-line wind velocity power spectrum.

A graphical representation of Equation (2-7) is presented in Figure 2-5. The velocity considered

in this representation is 20 MPH (32.19 km/hr) at a height of 33 ft (10 m). It is important to note

that wind velocities having a low frequency contain most of the energy in the power spectrum. It

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must also be noted that the power spectrum is dependent on the height above ground, z. As

noted, all power spectrums are generated for a height of 33 ft (10 m) above ground level.

Figure 2-5: In-Line Wind Velocity Power Spectrum

The artificial wind velocity time series can then be generated via the use of the second loop

shown in Figure 2-4. The dynamic analysis must be divided into time increments or time steps.

Thus, for each time step a wind velocity must be generated to compose the wind velocity time

series. This process involves summation of the energy contained within a frequency interval by

generating a large number of sinusoids having the desired amplitudes and frequencies. This is

repeated for all time steps needed for the wind velocity time series.

The process begins by dividing the power spectrum into equal frequency intervals. The

incremental frequency interval and midpoint frequency is determined by,

imid

ii

nnn

nnn

+∆

=

−=∆ +

2

1

(2-9)

where ni, ni+1, and nmid are the frequencies at the lower bound of the frequency interval, the upper

bound of the frequency interval, and the mid-point of the frequency interval, respectively. The

power spectrum located at the midpoint frequency interval can then be calculated using linear

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interpolation. This approximation is valid only if the frequency interval is small enough such

that the power spectrum at the lower and upper bounds of the frequency interval is

approximately linear. This approximation is given as,

21

1 nnnSSSS

ii

iiimid

∆⎟⎟⎠

⎞⎜⎜⎝

⎛−−

+=+

+ (2-10)

where Si, Si+1, and Smid are the power spectrum values at the lower bound of the frequency

interval, the upper bound of the frequency interval, and the mid-point of the frequency interval,

respectively. For each frequency interval, the results of Equations (2-9) and (2-10) are used to

obtain the wind velocity at a given time step, t. For each time step, the entire power spectrum is

considered. The mean wind velocity, u , is added to the summation to generate a wind velocity

time series with this mean value. A random phase angle, φ , is also applied to the summation.

The wind velocity time series is calculated as,

( ) ( )∑∆

−∆+=nAll

midmid tnnSutu φπ2cos2 (2-11)

Figure 2-6 provides an example of a generated wind velocity time series record of 3-minutes or

180-seconds. This time series, or record, was generated using a reference velocity, mean wind

velocity, of 20 MPH (32.19 km/hr). Notice that the mean wind velocity of this record, indicated

by the horizontal solid line, is given as nearly 20 MPH (32.19 km/hr) or the reference velocity.

The actual mean wind velocity of this record is calculated as 19.8 MPH (31.87 km/hr), which is

within 1% of the reference velocity. Notice the wind gusts (and wind relaxation, i.e. wind speeds

well below the mean value), which are characteristic of a random Gaussian process.

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Figure 2-6: In-Line Wind Velocity Time Series

The procedure for determining the loading due to the wind velocity time series is presented in

Figure 2-7.

Start Loop

Fit Wind Velocity toLogarithmic Profile

Evaluate LogarithmicProfile at Nodal Points

Determine Wind Loadat Nodal Points

End Loop

Figure 2-7: Wind Loading Procedure

The wind velocity time series generated from the procedure outlined in Figure 2-4 is for a single

point at the characteristic height. Thus, if perfect spatial correlation is assumed along the height

of the structure, each single wind velocity point in the time series can be fit to a profile such that

wind velocities at other points may be easily determined. The profile used in this project is the

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logarithmic profile. This profile, common in wind engineering studies, is given as (Simiu,

1996),

)ln()(0

*

zz

kuzu = (2-12)

where u* is the wind shear velocity, k is the von Karman constant (≈ 0.4), z is the height above

the ground, z0 is the roughness coefficient, and u(z) is the wind velocity at height z. The wind

shear velocity, u*, is assumed to be constant along the height of the structure. This assumption is

often valid for a height up to approximately 150 ft (45.7 m) above the ground (Simiu, 1996). For

this study, a roughness coefficient, z0, was chosen conforming to an area similar to grassy areas,

z0 equal to 0.787 in (2 cm). An example of the logarithmic profile is provided in Figure 2-8 for a

wind velocity of 20 MPH (32.19 km/hr) at a height of 33 ft (10 m).

Figure 2-8: Logarithmic Wind Velocity Profile

From Equation (2-1), the forcing function, F(t), must be specified at all nodal points. Thus,

using the height of each nodal point, the wind velocity along the height of the structure is

obtained. Morison’s equation, relating fluid flow past an object to determine force, is used to

obtain the wind loading produced by the in-line wind velocity at nodal points as (Morison,

1950),

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windwinddair uuACF ρ21

= (2-13)

where ρair is the mass density of air, A is the tributary projected area for the nodal point, Cd is the

drag coefficient, uwind is the wind velocity at the nodal point, and F is the force produced by the

wind velocity. In heavier fluids an inertial term is also present, but is neglected here due to the

low mass density of air. The mass density of air, ρair, is determined as a function of altitude and

air temperature. It can be determined by using the following relations,

( )

KkgJ

RsluglbftR

zzz

RTgzPP

RTP

basealtalt

altsealevel

air

−=

°−−

=

+=

⎥⎦

⎤⎢⎣

⎡⎟⎠⎞

⎜⎝⎛ −=

=

05.2871716

exp

ρ

(2-14)

where P is the pressure at the height where the mass density is desired, R is the universal gas

constant, and T is the absolute temperature in degrees Rankin or Kelvin. Other variables are

defined as: Psealevel is the standard pressure at sea level, g is acceleration due to gravity, z is the

height above ground where the mass density is desired, zbasealt is the altitude of the base of the

structure above sea-level, and zalt is the altitude above sea-level where the mass density is

desired.

The drag coefficient, Cd, is determined experimentally and is, in general, a function of the

Reynolds number, projected area of the object normal to flow, and other factors such as surface

roughness. For flow past a smooth cylinder, Cd can be obtained from Figure 2-9. This figure

was a result of experimental results for flow past a smooth cylinder. For this project, a drag

coefficient for the HML structural support was assumed to be 0.45 for all wind velocities. A

drag coefficient of 1.0 was assumed for the luminaire structure at the top. These values are

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consistent with example design calculations provided by CDOT and a study by the report’s

authors using published values for flow past a smooth cylinder.

Figure 2-9: Drag Coefficient for a Smooth Cylinder (Wilcox, 2000)

2.4 Dynamic Analysis

The procedure for solving the dynamic analysis of the system is presented in Figure 2-10. The

method chosen for this project was the Newmark-Beta method (Newmark, 1959; Paz, 2004).

This method provides a means to numerically integrate the equation of motion, Equation (2-1),

incrementally over a very small time interval, ∆t. It is assumed that the deformations of the

system remain in the linear elastic range for the material of the HML structure, steel, and thus

relatively small. Because of this assumption, a time step of 0.1 seconds was assumed. However,

as will be discussed in Section 2.5, the forcing function due to wind velocity becomes non-linear

as the structure begins to move with some velocity. Therefore, a procedure was also written to

check for unstable solutions. If a specified number of peak displacements continue to grow, an

unstable condition is noted and the dynamic analysis procedure is repeated with a time step equal

to half of the previous time step. This assumes proper convergence and subsequently accurate

results at all wind velocities.

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Start Loop

Determine EffectiveStiffness and

Equivalent ForceChange

Determine IncrementalPosition and Velocity

Change

DetermineAcceleration

Resolve Non-LinearWind Load

(Section 2.5)

End Loop

Figure 2-10: Dynamic Analysis Procedure

Initial values at time equal to 0 seconds are assumed for position, x, and velocity, x . Initial

acceleration, x , is obtained as,

[ ] { } [ ]{ } { }{ }{ }xKxCtFMx −−= − )(1 (2-15)

where all terms have been previously defined. A static equivalent method is used to obtain the

incremental position and velocity over time step i. The effective stiffness of the structure, Keq, is,

[ ] [ ] [ ] [ ]Ct

Mt

KKN

N

Neq ∆

+∆

+=βγ

β 2

1 (2-16)

where βN and γN are parameters for the Newmark-Beta method. The parameter γN is assumed to

be ½. Values of γN other than ½ may introduce unintended damping effects into the system (Paz,

2004). A range of values for βN is suggested as 1/6 ≤ βN ≤ 1/2 (Newmark, 1959). For this project,

βN was assumed to be ¼, corresponding to the constant acceleration method. The equivalent

force change, Feq, over time step i is,

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{ } { } [ ] [ ]{ } [ ] [ ] { }iN

N

Ni

N

N

Neq xCtMxCM

tFF ⎥

⎤⎢⎣

⎡∆⎟⎟⎠

⎞⎜⎜⎝

⎛−−++

∆+∆=

βγ

ββγ

β 21

211 (2-17)

where ∆F is the force change over time step i. The incremental position, ∆x, and velocity

change, x∆ , over time step i are then,

{ } [ ] { }

{ } { } { } { }iN

Ni

N

N

N

N

eqeq

xtxxt

x

FKx

∆⎟⎟⎠

⎞⎜⎜⎝

⎛−+−∆

∆=∆

=∆ −

βγ

βγ

βγ

21

1

(2-18)

The position, xi+1, and velocity, 1+ix , at the end of the time step, i+1, are then calculated as,

{ } { } { }

{ } { } { }xxx

xxx

ii

ii

∆+=

∆+=

+

+

1

1 (2-19)

Using the equation of motion, Equation (2-1), and forcing dynamic equilibrium, the acceleration,

1+ix , at the end of the time step is calculated as,

{ } [ ] { } [ ]{ } [ ]{ }{ }1111

1 +++−

+ −−= iiii xKxCFMx (2-20)

Thus, by stepping through time the position, velocity, and acceleration at each point along the

height of the HML structure can be determined.

2.5 Relative Motion

The procedure for resolving the non-linear wind load forcing function due to relative motion is

presented in Figure 2-11. The cause for this non-linearity is due to Morison’s equation that is

used to determine the force from the wind velocity in Equation (2-13). As the HML structural

support, herein referred to as the pole, moves, each point on the pole has some velocity, positive

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or negative depending on the motion. The wind is also moving with some velocity, positive or

negative. The true forcing function must be computed from the relative velocity between the

pole and the wind.

Loop for Convergence

Determine In-LinePole Velocity

at Nodal Points

DetermineRelative Velocity

Update Wind Loadat Nodal Points

SolveDynamic Analysis

of the System(Section 2.4)

Check forConvergence

End Loop

Figure 2-11: Relative Motion Procedure

To check the forcing function, the pole velocity before and after the forcing function is updated

and the new relative velocity must be considered. First, the in-line pole velocity at each nodal

point is extracted. These pole velocities, obtained at the end of the time step being considered,

are combined with the wind velocity at the appropriate time to obtain the relative velocity given

as,

{ } { } { }HMLwindrel uuu −= (2-21)

where urel is the relative velocity between the wind velocity, uwind, and the pole velocity, uHML.

Figure 2-12 illustrates the use of Equation (2-21). Here, positive velocities are assumed to be in

the positive x-direction. The wind velocity is moving with some velocity, uwind, in the positive

direction. The pole is also moving with some velocity, uHML, in the positive direction. Thus, the

net or relative velocity, urel, is the difference between the wind velocity and pole velocity.

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uwind uHML urel

_ =

x

y

Figure 2-12: Relative Velocity of Wind and HML Structure

Using the relative velocity between the pole and wind, an updated forcing function using a

modified version of Morison’s equation is determined for each nodal point as,

relreldair uuACF ρ21

= (2-22)

where urel is the relative velocity determined from Equation (2-21). Dynamic analysis using the

Newmark-Beta method from Section 2.4 is completed to reevaluate the position, velocity, and

acceleration of each node of the pole at the end of each time step. In-line pole velocities are

again extracted. Comparisons are made between the previously extracted pole velocities and

these new pole velocities at each node. If a set tolerance is exceeded, this procedure is repeated

until convergence is reached. If the tolerance is not exceeded, convergence is achieved and the

relative motion for the particular time step is completed.

2.6 Fatigue Analysis

The procedure for applying the fatigue analysis to determine the fatigue life for a given wind

speed is presented in Figure 2-13. This procedure makes use of the steps also presented in

Sections 2.3 – 2.5 of this report as noted in Figure 2-13. These steps will only be noted with no

further explanation given.

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The fatigue analysis assumes that the response of the HML structural support is linear elastic, i.e.

no permanent deformations caused by the loading. The derivation to calculate or estimate the

fatigue life of the structure follows the random vibration approach developed by Crandall and

Mark (1963). According to the Palmgren-Miner rule, each stress cycle causes some amount of

damage over some time duration. At some point, the accumulated damage reaches unity,

indicating failure of the system. Divide Wind Velocity

PDF into Bins

Loop throughBins of PDF

Assign Wind Velocityto Bin Value

Construct WindLoading Model(Section 2.3)

SolveDynamic Analysis

of the System(Section 2.4)

End Loop

Extract StressTime History

Resolve Non-LinearWind Load

(Section 2.5)

DetermineExpected Damage

from Bin

DetermineFatigue Life

Figure 2-13: Fatigue Analysis Procedure

First, it is assumed that +0v is the mean up-crossing rate (i.e., the number of mean stress crossings

with a positive slope over one second for the stress time history) such that during a time period

the number of stress cycles is +0v . The fraction of these cycles that would have amplitudes

between some value a and a+da would be p(a)da where p(a) is the probability density function

(PDF) of the peaks of the stress time history. The expected number of peaks, n(a), between these

values is then calculated as,

( ) ( )daaTpvan += 0 (2-23)

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where T is the time duration of the stress time history. According to the Palmgren-Miner rule, a

single peak a causes an incremental damage of,

( )aNdD 1

= (2-24)

where N(a) is the number of cycles to failure at the stress amplitude a for that material from test

data. For all cycles between a and a+da over time, the expected damage is determined as,

( )( )

( )( )aN

daaTpvaNan +

= 0 (2-25)

To account for all possible values of a and to determine the total expected damage, integration

over the entire possible range from zero to infinity yields,

( )[ ] ( )( )∫

∞+=0

daaNapTvTDE o (2-26)

where ( )[ ]TDE is the total expected damage. Assuming that the stress process is a Gaussian

process, a process that fits a normal distribution, then the peaks follow a special case of the

Weibull distribution known as the Rayleigh distribution (shape parameter = 2.0). The PDF for

the Rayleigh distribution is given as,

( ) ⎟⎟⎠

⎞⎜⎜⎝

⎛−= 2

2

2 2exp

yy

aaapσσ

(2-27)

where a is the stress amplitudes and 2yσ is the variance of the stress process as a function of

time. Substitution of Equation (2-27) into (2-26) produces,

( )[ ] ∫∞ +

+

⎟⎟⎠

⎞⎜⎜⎝

⎛−=

0 2

21

20

2exp daaa

cTvTDE

y

b

y σσ (2-28)

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where b and c are fatigue constants related to the material (in the present case steel) of the

structure. These constants, b and c, are determined from,

cNS b = (2-29)

where N is the number of cycles at stress amplitude S. As noted previously, b and c are the

parameters that define the fatigue (S-N) curve for a particular stress category. Integrating the

expected damage from Equation (2-28) yields,

( )[ ] ( ) ⎟⎠⎞

⎜⎝⎛ +Γ=

+

21220 b

cvTDE

b

yσ (2-30)

where σy is the standard deviation of stress process as a function of time and the gamma function

is defined as,

( ) ∫∞ −−=Γ

0

11 dtetx x (2-31)

Finally, setting ( )[ ]ii TDEF = for the ith wind speed (from the PDF of wind velocity) the fatigue

life can be calculated according to the Palmgren-Miner rule as,

∑=

= n

iii

life

PFF

10

1 (2-32)

where P0i is the probability of occurrence of the wind force for the ith wind speed and causing the

associated damage in Equation (2-30).

In order to estimate the fatigue life using Crandall and Mark’s (1963) method, it is necessary to

procure the wind statistical distribution information. Statistics for locations along the Front

Range are not readily available and, therefore, a lognormal distribution was assumed. This

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corresponds to a reasonable fit for data developed by the National Oceanographic and

Atmospheric Administration (NOAA) for the contiguous United States. The PDF for the

lognormal distribution of wind velocity, u, can be expressed as,

( )⎥⎥⎦

⎢⎢⎣

⎡⎟⎟⎠

⎞⎜⎜⎝

⎛ −−=

2ln

21exp

21

ζλ

ζπu

uufU (2-33)

where the parameters ζ and λ are defined as,

2

2

22

21ln

1ln

ζµλ

µσζ

−=

⎟⎟⎠

⎞⎜⎜⎝

⎛+=

(2-34)

and the parameters µ and σ are defined as the mean wind velocity and standard deviation of wind

velocity, respectively. The mean wind velocity and standard deviation of wind velocity are

related by the coefficient of variation (COV) as,

µσ

=COV (2-35)

Figure 2-14 illustrates Equation (2-33), the PDF, for a mean velocity of 20 MPH (32.19 km/hr)

and COV of 25%.

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Figure 2-14: Lognormal PDF

The dynamic response of the structure was determined for each of twenty-five different wind

velocities. This required the lognormal PDF to be divided into twenty-five bins of equal width

and each having a probability of occurrence, P0i, equal to their area. Figure 2-15 illustrates the

bins that would be used for the PDF in Figure 2-14.

Figure 2-15: Lognormal PDF Bins

The area under each bin represents the probability of occurrence of a wind velocity having a

magnitude between the upper and lower bounds of the bin. The probability of occurrence is

paired with the wind velocity occurring at the midpoint of that bin for analysis. As the wind

velocities increase beyond the mean value, the area within each bin typically decreases.

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However, although their occurrence probability is very small, high wind velocities must be

considered as they may cause extensive damage to the structure, decreasing its fatigue life even

with a low probability of occurrence.

2.7 Reliability Analysis

The procedure used for determining the reliability index, β, for a given target fatigue life is

presented in Figure 2-16. The reliability approach used in this study makes use of a numerically

traditional approach to determine the probability of failure of a complex system. The Monte

Carlo Simulation (MCS) method consists of a repetitive procedure in which a large number

(>10,000) of data points are needed to obtain an accurate assessment of the probability of failure.

Upon completion, the reliability index, β, can also be determined.

Determine COVfor Each Fatigue

Parameter

Monte CarloSimulation Loop

Generate RandomNumbers and

Fit to StatisticalDistribution

EvaluateFatigue Life

EvaluateLimit State Function

End Monte CarloSimulation Loop

Evaluate Probabilityof Failure and

Reliability Index

Figure 2-16: Reliability Analysis Procedure

This procedure utilizes Equations (2-30) and (2-32) from the fatigue analysis procedure and thus

requires all of the values indicated in those equations. It does not require, however, that the

entire fatigue analysis be repeated. For this project, the S-N curve is assumed to possess the

model and time uncertainty in the fatigue estimation. Specifically, the fatigue, or S-N

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parameters, constants b and c in Equation (2-29), used to describe the S-N curve for steel are

considered as random variables and account for all other randomness.

The parameters used to describe the S-N curve are considered to have a combined COV of 40%

(Assakkaf and Ayyub, 2000). The COV for each S-N parameter is assumed to be equal and can

thus be determined as,

22 COVCOVCOV CBF += (2-36)

where COVF is the combined COV of 40%, COVB and COVC are the COV for each S-N

parameter. This assumption is only valid if statistical independence between the parameters is

assumed. Furthermore, the parameters are assumed to behave as log-normally distributed

random variables for reliability analysis purposes.

The MCS method requires several steps to be performed. The method, specific to this project, is

outlined as and is repeated i times:

Step 1: Generate two uniformly distributed random numbers within the range –1 ≤ x ≤ 1

where x is the random number.

Step 2: Fit uniformly distributed random numbers to standard normal distributed random

numbers where the standard normal distribution has mean of zero and standard

deviation of one.

Step 3: Fit standard normal distributed random numbers to lognormal distributed random

numbers with given mean values and standard deviations determined from the

COV calculated from Equation (2-36).

Step 4: Re-evaluate expected damage for each bin using Equation (2-30).

Step 5: Re-evaluate fatigue life using Equation (2-32).

Step 6: Evaluate limit state function given in Equation (2-37).

target lifeg F F= − (2-37)

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where g is the limit state function, Flife is the fatigue life calculated for simulation i, and Ftarget is

the target fatigue life as prescribed by CDOT. Thus, we seek the probability that the limit state

function, g, is less than zero, P(g < 0). Counting the number of failures, g < 0, for all simulations

i, the probability of failure, Pf, is calculated as,

simulation

failure

NNPf = (2-38)

where Nfailure is the number of failures and Nsimulation is the total number of simulations or data

points generated. The reliability index, β, can be calculated directly from the probability of

failure as,

( )fP−Φ= − 11β (2-39)

where Φ-1 is the inverse of the standard normal distribution function. Some common values, i.e.

a range typically seen in civil engineering problems, are presented in Table 2-1.

Pf β 0.16 1 0.023 2 0.0013 3 0.000032 4 0.00000029 5

Table 2-1: Common Reliability Indices, β

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CHAPTER 3

SENSTIVITY AND RELIABILITY ANALYSES

3.1 Sensitivity Analysis Background

The approach used to determine the reliability-based design procedure for HML structural

supports procedure can be used to identify the key factors (design parameters and loading

parameters) that contribute to its fatigue life. To accomplish this, a sensitivity analysis

considering six primary physical and two primary wind velocity factors was performed. The six

primary physical factors focused on the physical characteristics of the HML structural supports,

herein referred to as the pole, and how these factors affect the fatigue life. These included the

outside diameter of the pole, the wall thickness of the pole, the height or length of the pole, the

weight of the luminaire structure, the projected area of the luminaire structure, and the damping

ratio of the structure. The two primary wind velocity factors considered the sensitivity of the

fatigue life to wind velocity factors. First, the assumed coefficient of variation (COV) for the

lognormal distribution describing the wind velocity was considered. Second, the probability of

strong wind gusts associated with periodic weather events in Colorado were considered.

To conduct the sensitivity analysis, a benchmark, or representative, HML structural support was

needed. Structural drawings were provided by CDOT. This submittal was in reference to the I-

25 / Broadway Viaduct Phase II project and prepared by Dynalectric Company. Figure 3-1

illustrates a benchmark HML structural support used in this project. For each section shown in

Figure 3-1, a corresponding table of properties for that given section is given in Tables 3-1 – 3-4.

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120 ft

Luminaire Structure(Table 3-4)

Section 3(Table 3-1)

Joint Section 2(Table 3-2)

Section 2(Table 3-1)

Joint Section 1(Table 3-2)

Section 1(Table 3-1)

Structural Foundation(Table 3-3)

Figure 3-1: Benchmark HML Structural Support in Colorado

Table 3-1 provides the properties for pole sections 1 – 3 from Figure 3-1. Properties for each

section were directly obtained from the specification submittals obtained from CDOT.

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Property Section 1 Section 2 Section 3

Total Length 53.49 ft (16.30 m)

52.52 ft (16.01 m)

20.16 ft (6.14 m)

Bottom Outside Diameter

26.00 in (660.40 mm)

19.50 in (495.30 mm)

13.00 in (330.20 mm)

Top Outside Diameter

18.51 in (470.15 mm)

12.15 in (308.61 mm)

10.18 in (258.57 mm)

Taper 0.14 in/ft (11.67 mm/m)

0.14 in/ft (11.67 mm/m)

0.14 in/ft (11.67 mm/m)

Wall Thickness 0.375 in (9.525 mm)

0.250 in (6.350 mm)

0.2391 in (6.0731 mm)

Material Code S22-65 S22-65 S105-55

Yield Strength 65 ksi (448 MPa)

65 ksi (448 MPa)

55 ksi (379 MPa)

Modulus of Elasticity

29,000 ksi (200 GPa)

29,000 ksi (200 GPa)

29,000 ksi (200 GPa)

Mass Density 15.235 slug/ft3

(7850 kg/m3)

15.235 slug/ft3

(7850 kg/m3)

15.235 slug/ft3

(7850 kg/m3)

Poisson’s Ratio 0.3 0.3 0.3

Table 3-1: HML Structural Support Properties – Pole Sections

Table 3-2 provides the properties for joint sections 1 and 2 from Figure 3-1. As indicated in the

specifications, these joint sections are characterized as lap-splices, one section overlapping the

other section. Thus, all section properties are identical to those given in Table 3-1. These joints

do however affect the stiffness of the structure due to the overlapping of the sections as indicated

with the effective wall thickness given in Table 3-2. Properties for each joint section were

directly obtained from the specification submittals obtained from CDOT.

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Property Joint Section 1 Joint Section 2

Section Type Lap-Splice Lap-Splice

Sections Joined 1 – 2 2 – 3

Effective Wall Thickness

0.625 in (15.875 mm)

0.4891 in (12.4231 mm)

Overlap Length

3.492 ft (1.064 m)

2.683 ft (0.818 m)

Height of Overlap

53.49 ft (16.30 m)

102.59 ft (31.25 m)

Table 3-2: HML Structural Support Properties – Joint Sections

Table 3-3 provides the properties for the structural foundation. Recall from Chapter 2 that this

foundation is modeled as a set of translational and rotational springs. For this project, springs

were assumed to have a stiffness representing a fixed structural boundary condition for the

foundation. A fixed structural boundary condition is a conservative assumption in determining

the fatigue life of the structure.

Property Spring Stiffness

Axial Stiffness

1 x 1030 lb/in (1.75 x 1029 kN/m)

Lateral Stiffness

1 x 1030 lb/in (1.75 x 1029 kN/m)

Overturning Stiffness

1 x 1030 lb*in/rad (1.75 x 1029 kN*m/rad)

Table 3-3: HML Structural Support Properties – Boundary Support Conditions

Table 3-4 provides the properties for the luminaire structure mounted at the top of the HML

structural support. Properties for the luminaire structure were directly obtained from the

specification submittals obtained from CDOT.

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Property Luminaire Structure

Mounting Height

120 ft (36.576 m)

Weight 666 lbs (302 kg)

Projected Area 11.50 ft2 (1.0684 m2)

Table 3-4: HML Structural Support Properties – Luminaire Structure Properties

3.2 The Mean Wind Velocity

ASCE-7 (2005) provides design wind velocities for consideration in the design process of a

structure. These design wind velocities represent 3-second wind gusts that have an annual

probability of exceedance of 2%, or a mean recurrence interval (MRI) of 50 years. These design

wind velocities are obtained from the consideration of many years of data recorded at stations

such as airports. Extreme value statistics are then used to determine the 3-second wind gusts

associated with the desired MRI.

For this study, however, the fatigue analysis requires the use of the wind velocity parent

distribution for a given area. As given in Chapter 2, the lognormal PDF is assumed as the

statistical distribution describing the loading event, or in this case the wind velocity. It has been

shown that Weibull distribution is typically a better fit for the parent distribution. However, the

Weibull distribution was not considered at this time due to the lack of knowledge concerning the

characteristics of the wind along the Front Range of Colorado. The lognormal parent

distribution is illustrated again in Figure 3-2 for a mean wind velocity of 10 MPH (16.09 km/hr)

and COV of 25% at a height of 33 ft (10 m). Attempts have been made in the past to predict the

design, or extreme, wind velocities, as used in ASCE-7 (2005), from these parent wind

distributions. These attempts have proven to be unsuccessful (Holmes, 2001).

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Figure 3-2: Wind Velocity Parent Distribution

Thus, the remainder of this study will only consider the mean wind velocity obtained from the

parent wind distribution at 33 ft (10 m). Furthermore, this mean wind velocity is only an

assumed value and not associated with any obtained data. The procedure to be developed will

take this into consideration. The appendix of this report provides some initial consideration of

mean wind velocities within the state of Colorado at 33 ft (10 m). A more detailed statistical

study of the wind along the Front Range of Colorado is needed to accurately determine the

appropriate parent distribution and mean wind velocity. With the completion of this statistical

study, the determination of the design wind velocities along the Front Range of Colorado would

also be capable of being accomplished.

3.3 Sensitivity Analysis

The sensitivity analysis considers eight total factors and their affect on the fatigue life of the

HML structural support for a particular wind-loading event. Among these factors are six

associated with the physical properties or characteristics of the HML structural support or pole.

The other two factors consider the properties of the wind velocity and, in particular, the

statistical distribution used to describe the in-line wind velocity used in the fatigue analysis

computations. Based on Section 1.3, AASHTO 2001, both detail categories E and E′ are used as

the basis for all sensitivity analysis results presented herein.

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Considering first the six factors related to the physical properties of the HML structural support,

the fatigue life is determined for varying values of these properties. For five of the six factors,

outside diameter, wall thickness, section length, luminaire weight, and luminaire projected area,

variations consist of percentage reductions or increases to determine the variation in calculated

fatigue life. If a 30% reduction is considered, indicated by –30%, then all values associated with

that factor are reduced by 30% along all points of the pole. For the sixth factor, damping ratio,

various values are assumed to determine the variation in calculated fatigue life.

Pole Outside Diameter

Figure 3-3 illustrates the sensitivity of the fatigue life for variations in the outside diameter of the

pole. Large changes in the outside diameter of the pole substantially affect the fatigue life of the

structure. Though a decrease in outside diameter yields less cross-sectional material at the base

of the structure and therefore higher stresses, the loading caused by the wind velocity is also

reduced. An increase in outside diameter yields higher loads due to wind velocity, but there is

also more cross-sectional area to resist the forces caused at the base of the structure.

(a): Detail Category E (b): Detail Category E′

Figure 3-3: Fatigue Life Sensitivity – Pole Outside Diameter

Pole Wall Thickness

Figure 3-4 illustrates the sensitivity of the fatigue life for variations in the wall thickness of the

pole. As can be seen, there is substantial variability in fatigue life for decreases in wall

thickness. This, however, is not the case for increases in wall thickness. This result compares

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well with the investigation recently conducted by Kaufmann (2005) concerning the exact

measurements as compared to the design specifications. As a result of this analysis, the

sensitivity due to changes in wall thickness must be carefully monitored.

(a): Detail Category E (b): Detail Category E′

Figure 3-4: Fatigue Life Sensitivity – Pole Wall Thickness

Pole Length

Figure 3-5 illustrates the sensitivity of the fatigue life due to changes in the length of each

section comprising the total height of the structure. Recall from Figure 3-1, the pole is

comprised of 3 sections. Sections 1 and 2 overlap to form the lap-splice at Joint Section 1.

Sections 2 and 3 overlap to form Joint Section 2. As expected, reductions in the height of the

structure yield a higher fatigue life. However, dramatic increases do not have an equivalent

effect in regards to reducing the fatigue life drastically different from the original height or no

change.

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(a): Detail Category E (b): Detail Category E′

Figure 3-5: Fatigue Life Sensitivity – Pole Length

Luminaire Structure Weight

Figure 3-6 illustrates the sensitivity of the fatigue life due to changes in the weight or mass of the

luminaire structure mounted to the top of the pole. Changes in the luminaire structure weight

only effect the applied concentrated nodal mass and the subsequent degrees-of-freedom in the

structure mass matrix. As can be seen, changes to the luminaire structure weight do not effect or

create large variability in the calculated fatigue life of the structure.

(a): Detail Category E (b): Detail Category E′

Figure 3-6: Fatigue Life Sensitivity – Luminaire Structure Weight

Luminaire Structure Projected Area

Figure 3-7 illustrates the sensitivity of the fatigue life due to changes in the projected area of the

luminaire structure mounted to the top of the pole. Changes in the projected area only affect the

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load created by the wind velocity as determined by Morison’s equation. It is rational to assume

that increases in the area would also correlate well with changes in the luminaire structure

weight. However, to determine if either of these variables affects the fatigue life, they were

considered separately. As can be seen, changes in the projected area of the luminaire structure

do not produce as much variability as changes in the wall thickness of the pole.

(a): Detail Category E (b): Detail Category E′

Figure 3-7: Fatigue Life Sensitivity – Luminaire Structure Projected Area

Structure Damping

Figure 3-8 illustrates the sensitivity of the fatigue life due to changes in the damping ratio, ξ, of

the entire structure. The damping ratio of the structure, however, is somewhat of an unknown

quantity. For a structure of this height and slenderness it would be appropriate to assume a

damping ratio of approximately 1%, which has been used in previous studies on similar

structures. However, this value could vary as the fatigue life certainly does vary for changes in

the damping ratio. For purposes of this project, it will be assumed that the damping ratio is

always 1%. Further experimental verification is needed to ensure this assumption is correct.

Finally, it should be noted that variations in damping ratio values did exhibit a wide deviation in

fatigue life.

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(a): Detail Category E (b): Detail Category E′

Figure 3-8: Fatigue Life Sensitivity – Structure Damping

Wind Velocity COV

Finally, the last two factors considered are related to the wind velocity. Figure 3-9 illustrates the

sensitivity of the fatigue life due to changes in the assumed coefficient of variation (COV) for the

statistical distribution describing the in-line wind velocity. This distribution is instrumental in

determining the expected damage from each bin of the distribution. Recent studies have

indicated a COV of 25% is appropriate for wind velocity, 35% for wind-loading. A 25% COV

represents a high degree of uncertainty in wind velocities and thus wind-loading. As shown, a

higher COV produces a lower fatigue life for the structure. This unknown quantity cannot be

resolved without extensive statistical studies of wind velocities along the Front Range of

Colorado. Thus, it is assumed that a COV of 25% is appropriate.

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(a): Detail Category E (b): Detail Category E′

Figure 3-9: Fatigue Life Sensitivity – Wind Velocity COV

Wind Gust

Figure 3-10 illustrates the sensitivity of the fatigue life due to simulated wind gusts. The mean

wind velocity was assumed to be 10 MPH (16.09 km/hr) with a COV of 25%. Wind gusts

varying from 50 MPH (80.47 km/hr) to 100 MPH (160.93 km/hr) were chosen with varying

probabilities of occurrence as indicated in Figure 3-10. It should be noted that these occurrence

rates, even 1%, are extremely high and are used here to examine sensitivity only. As a result of

this analysis, it can be seen that the fatigue life is extremely sensitive to wind gusts, as one might

expect. Further development of this realization is needed.

(a): Detail Category E (b): Detail Category E′

Figure 3-10: Fatigue Life Sensitivity – Wind Gust

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The sensitivity analysis yielded several factors that directly contribute to the loss of desired

fatigue life. The luminaire structure weight and luminaire structure projected area did not

contribute to large variations in fatigue life. Variations in luminaire structure weight appear to

affect the fatigue life less than variations in luminaire structure projected area. Thus, based on

these two parameters, it would be appropriate to state that the projected area of the luminaire

structure is more important to the resulting fatigue life of the HML structural support.

Sensitivity of the fatigue life to structural damping did have an effect on the fatigue life.

However, this quantity cannot be exactly determined without experimental verifications. Thus, a

damping ratio of 1% is consistent with dynamic investigations of traffic and lighting structures.

Variations in the assumed COV for describing the wind velocity distribution did contribute

significantly to the fatigue life. However, as noted earlier, an extensive statistical study of wind

velocities along the Front Range of Colorado is recommended to determine the appropriate

COV. Thus, a COV of 25% is assumed at this point in time and is approximately consistent with

COV’s in North America.

Sensitivity of fatigue life to wind gusts did contribute to high degrees of variability in fatigue

life. The details behind appropriate gusts and occurrence probabilities associated with those

gusts would need to be determined. This could be accomplished with the same study to

determine the appropriate COV for wind velocity. This analysis is beyond the scope of the

present project but exacerbates the need for a conclusive wind study along the Front Range of

Colorado, where it is known that there are sometimes extreme wind conditions.

The primary factors that contributed to fatigue life that are under the control of the designer are

pole outside diameter, pole wall thickness, and pole length. Due to these observations, the

design method must consider these three factors with respect to wind velocity. The design

method will also include the effects of the luminaire structure attached to the top the HML

structural supports. Only the projected area of the luminaire structure will be considered in this

regard. As shown, the other luminaire structure factor did not display a wide range of fatigue life

values based on variations in its weight.

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3.4 Reliability Analysis

The reliability analysis considers the results from the sensitivity analysis and their effect on the

reliability of the HML structural support for a particular wind-loading event. From the

sensitivity analysis, all variations in outside diameter, wall thickness, section length, luminaire

weight, and luminaire projected area are considered in the reliability analysis. All variations in

structure damping are considered for the reliability analysis. Fatigue life results are only given

for the assumed damping ratio of 1%. Additionally, all variations in wind velocity COV are

considered for the reliability analysis. Fatigue life results are only given for the assumed wind

velocity COV of 25% and wind gusts are not considered.

All reliability analyses are conducted for 50,000 simulations using the Monte Carlo method. The

limit state function, given in Equation (2-37), is evaluated using a target fatigue life of 50 years.

It should be noted that this target fatigue life was selected somewhat arbitrarily to illustrate the

methods and can be any value in future studies. Failure of the HML structural support is thus

indicated by a calculated fatigue life for a particular wind-loading event as being less than the

target fatigue life or 50 years. The probability of failure is calculated in accordance with

Equation (2-38) where the total number of simulations is 50,000. Finally, the reliability index, β,

is calculated using Equation (2-39) that uses the results from Equation (2-38), the probability of

failure. Using 50,000 simulations, reliability indices of β ≈ 4 are capable of being estimated.

This is a direct result of the minimum probability of failure capable of being obtained using

50,000 simulations.

Pole Outside Diameter

Figures 3-11 (a) – (c) illustrate the fatigue life for 30% reduction, no change, and 30% increase

in pole outside diameter, respectively, for detail category E (designated by E in the figure

subtitle). The solid line illustrates the mean fatigue life for the variation considered. Plus and

minus one standard deviation with respect to the mean fatigue life are given as dashed lines. In

cases where the mean minus one standard deviation becomes negative, these values are not

plotted and hence the appearance of incomplete data sets.

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(a): Fatigue Life (E) – 30% Reduction (b): Fatigue Life (E) – No Change

(c): Fatigue Life (E) – 30% Increase

Figure 3-11: Reliability Analysis – Pole Outside Diameter

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Figures 3-11 (d) and (e) illustrate the probability of failure and reliability index for all variations

considered for changes in pole outside diameter, respectively, for detail category E (designated

by E in the figure subtitle). These figures are determined based on a target fatigue life of 50

years. As can be seen, an increase in outside diameter correlates well with a decrease in

probability of failure and an increase in reliability index.

(d): Probability of Failure (E) (e): Reliability Index (E)

Figure 3-11 (cont.): Reliability Analysis – Pole Outside Diameter

Figures 3-11 (f) – (j) provide the same results given in (a) – (e) except for detail category E′

(designated by E′ in the figure subtitle).

(f): Fatigue Life (E′) – 30% Reduction (g): Fatigue Life (E′) – No Change

Figure 3-11 (cont.): Reliability Analysis – Pole Outside Diameter

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(h): Fatigue Life (E′) – 30% Increase

(i): Probability of Failure (E′) (j): Reliability Index (E′)

Figure 3-11 (cont.): Reliability Analysis – Pole Outside Diameter

Pole Wall Thickness

Figures 3-12 (a) – (c) illustrate the fatigue life for 30% reduction, no change, and 30% increase

in pole wall thickness, respectively, for detail category E (designated by E in the figure subtitle).

The solid line illustrates the mean fatigue life for the variation considered. Plus and minus one

standard deviation with respect to the mean fatigue life are given as dashed lines. In cases where

the mean minus one standard deviation becomes negative, these values are not plotted and hence

the appearance of incomplete data sets.

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(a): Fatigue Life (E) – 30% Reduction (b): Fatigue Life (E) – No Change

(c): Fatigue Life (E) – 30% Increase

Figure 3-12: Reliability Analysis – Pole Wall Thickness

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Figures 3-12 (d) and (e) illustrate the probability of failure and reliability index for all variations

considered for changes in pole wall thickness, respectively, for detail category E (designated by

E in the figure subtitle). These figures are determined based on a target fatigue life of 50 years.

As can be seen, an increase in wall thickness correlates well with a decrease in probability of

failure and an increase in reliability index.

(d): Probability of Failure (E) (e): Reliability Index (E)

Figure 3-12 (cont.): Reliability Analysis – Pole Wall Thickness

Figures 3-12 (f) – (j) provide the same results given in (a) – (e) except for detail category E′

(designated by E′ in the figure subtitle).

(f): Fatigue Life (E′) – 30% Reduction (g): Fatigue Life (E′) – No Change

Figure 3-12 (cont.): Reliability Analysis – Pole Wall Thickness

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(h): Fatigue Life (E′) – 30% Increase

(i): Probability of Failure (E′) (j): Reliability Index (E′)

Figure 3-12 (cont.): Reliability Analysis – Pole Wall Thickness

Pole Length

Figures 3-13 (a) – (c) illustrate the fatigue life for 30% reduction, no change, and 30% increase

in pole section length, respectively, for detail category E (designated by E in the figure subtitle).

The solid line illustrates the mean fatigue life for the variation considered. Plus and minus one

standard deviation with respect to the mean fatigue life are given as dashed lines. In cases where

the mean minus one standard deviation becomes negative, these values are not plotted and hence

the appearance of incomplete data sets.

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(a): Fatigue Life (E) – 30% Reduction (b): Fatigue Life (E) – No Change

(c): Fatigue Life (E) – 30% Increase

Figure 3-13: Reliability Analysis – Pole Length

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Figures 3-13 (d) and (e) illustrate the probability of failure and reliability index for all variations

considered for changes in pole section length, respectively, for detail category E (designated by

E in the figure subtitle). These figures are determined based on a target fatigue life of 50 years.

As can be seen, a decrease in section length correlates well with a decrease in probability of

failure and an increase in reliability index.

(d): Probability of Failure (E) (e): Reliability Index (E)

Figure 3-13 (cont.): Reliability Analysis – Pole Length

Figures 3-13 (f) – (j) provide the same results given in (a) – (e) except for detail category E′

(designated by E′ in the figure subtitle).

(f): Fatigue Life (E′) – 30% Reduction (g): Fatigue Life (E′) – No Change

Figure 3-13 (cont.): Reliability Analysis – Pole Length

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(h): Fatigue Life (E′) – 30% Increase

(i): Probability of Failure (E′) (j): Reliability Index (E′)

Figure 3-13 (cont.): Reliability Analysis – Pole Length

Luminaire Structure Weight

Figures 3-14 (a) – (c) illustrate the fatigue life for 30% reduction, no change, and 30% increase

in luminaire structure weight, respectively, for detail category E (designated by E in the figure

subtitle). The solid line illustrates the mean fatigue life for the variation considered. Plus and

minus one standard deviation with respect to the mean fatigue life are given as dashed lines. In

cases where the mean minus one standard deviation becomes negative, these values are not

plotted and hence the appearance of incomplete data sets.

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(a): Fatigue Life (E) – 30% Reduction (b): Fatigue Life (E) – No Change

(c): Fatigue Life (E) – 30% Increase

Figure 3-14: Reliability Analysis – Luminaire Structure Weight

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Figures 3-14 (d) and (e) illustrate the probability of failure and reliability index for all variations

considered for changes in luminaire structure weight, respectively, for detail category E

(designated by E in the figure subtitle). These figures are determined based on a target fatigue

life of 50 years. As can be seen, changes in weight do not appear to greatly affect the probability

of failure or reliability index of the structure.

(d): Probability of Failure (E) (e): Reliability Index (E)

Figure 3-14 (cont.): Reliability Analysis – Luminaire Structure Weight

Figures 3-14 (f) – (j) provide the same results given in (a) – (e) except for detail category E′

(designated by E′ in the figure subtitle).

(f): Fatigue Life (E′) – 30% Reduction (g): Fatigue Life (E′) – No Change

Figure 3-14 (cont.): Reliability Analysis – Luminaire Structure Weight

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(h): Fatigue Life (E′) – 30% Increase

(i): Probability of Failure (E′) (j): Reliability Index (E′)

Figure 3-14 (cont.): Reliability Analysis – Luminaire Structure Weight

Luminaire Structure Projected Area

Figures 3-15 (a) – (c) illustrate the fatigue life for 30% reduction, no change, and 30% increase

in luminaire structure projected area, respectively, for detail category E (designated by E in the

figure subtitle). The solid line illustrates the mean fatigue life for the variation considered. Plus

and minus one standard deviation with respect to the mean fatigue life are given as dashed lines.

In cases where the mean minus one standard deviation becomes negative, these values are not

plotted and hence the appearance of incomplete data sets.

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(a): Fatigue Life (E) – 30% Reduction (b): Fatigue Life (E) – No Change

(c): Fatigue Life (E) – 30% Increase

Figure 3-15: Reliability Analysis – Luminaire Structure Projected Area

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Figures 3-15 (d) and (e) illustrate the probability of failure and reliability index for all variations

considered for changes in luminaire structure projected area, respectively, for detail category E

(designated by E in the figure subtitle). These figures are determined based on a target fatigue

life of 50 years. As can be seen, changes in projected area do not appear to greatly affect the

probability of failure or reliability index of the structure.

(d): Probability of Failure (E) (e): Reliability Index (E)

Figure 3-15 (cont.): Reliability Analysis – Luminaire Structure Projected Area

Figures 3-15 (f) – (j) provide the same results given in (a) – (e) except for detail category E′

(designated by E′ in the figure subtitle).

(f): Fatigue Life (E′) – 30% Reduction (g): Fatigue Life (E′) – No Change

Figure 3-15 (cont.): Reliability Analysis – Luminaire Structure Projected Area

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(h): Fatigue Life (E′) – 30% Increase

(i): Probability of Failure (E′) (j): Reliability Index (E′)

Figure 3-15 (cont.): Reliability Analysis – Luminaire Structure Projected Area

Structure Damping

Figure 3-16 (a) illustrates the fatigue life for an assumed damping ratio of 1% for detail category

E (designated by E in the figure subtitle). The solid line illustrates the mean fatigue life. Plus

and minus one standard deviation with respect to the mean fatigue life are given as dashed lines.

In cases where the mean minus one standard deviation becomes negative, these values are not

plotted and hence the appearance of incomplete data sets.

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(a): Fatigue Life (E) – 1% Damping

Figure 3-16: Reliability Analysis – Structure Damping

Figures 3-16 (b) and (c) illustrate the probability of failure and reliability index for all variations

considered for changes in structure damping, respectively, for detail category E (designated by E

in the figure subtitle). These figures are determined based on a fatigue life of 50 years. As can

be seen, an increase in structure damping correlates well with a decrease in probability of failure

and an increase in reliability index.

(b): Probability of Failure (E) (c): Reliability Index (E)

Figure 3-16 (cont.): Reliability Analysis – Structure Damping

Figures 3-16 (d) – (f) provide the same results given in (a) – (c) except for detail category E′

(designated by E′ in the figure subtitle).

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(d): Fatigue Life (E′) – 1% Damping

(e): Probability of Failure (E′) (f): Reliability Index (E′)

Figure 3-16 (cont.): Reliability Analysis – Structure Damping

Wind Velocity COV

Figure 3-17 (a) illustrates the fatigue life for an assumed wind velocity COV of 25% for detail

category E (designated by E in the figure subtitle). The solid line illustrates the mean fatigue

life. Plus and minus one standard deviation with respect to the mean fatigue life are given as

dashed lines. In cases where the mean minus one standard deviation becomes negative, these

values are not plotted and hence the appearance of incomplete data sets.

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(a): Fatigue Life (E) – 25% COV

Figure 3-17: Reliability Analysis – Wind Velocity COV

Figures 3-17 (b) and (c) illustrate the probability of failure and reliability index for all variations

considered for changes in wind velocity COV, respectively, for detail category E (designated by

E in the figure subtitle). These figures are determined based on a fatigue life of 50 years. As can

be seen, an increase in the COV correlates well with an increase in probability of failure and a

decrease in reliability index.

(b): Probability of Failure (E) (c): Reliability Index (E)

Figure 3-17 (cont.): Reliability Analysis – Wind Velocity COV

Figures 3-17 (d) – (f) provide the same results given in (a) – (c) except for detail category E′

(designated by E′ in the figure subtitle).

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(d): Fatigue Life (E′) – 25% COV

(e): Probability of Failure (E′) (f): Reliability Index (E′)

Figure 3-17 (cont.): Reliability Analysis – Wind Velocity COV

The results of the reliability analysis yielded interesting results in regard to the selected target

fatigue life of 50 years. As will be seen with the presentation of the design methodology, a target

fatigue life of 50 years at this point appears to be reasonable for mean wind velocities of 15 MPH

(24.14 km/hr) or less for detail category E and 12 MPH (19.31 km/hr) or less for detail category

E′. Due to the variability in wind events along the Front Range of Colorado, these results may be

of concern. However, these results could also be a combination of the two major assumptions

regarding the HML structural support itself and the statistics related to the wind velocity

distribution. As was seen from the sensitivity analysis, structure damping and wind velocity

COV variations produced relatively large variations in fatigue life. These results were

reciprocated in the reliability analysis for both parameters.

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CHAPTER 4

RELIABILITY-BASED DESIGN METHODOLOGY

4.1 Design Methodology Background

The method consists of several design charts for each of the design parameters considered in the

sensitivity and reliability analyses of Chapter 3. Included among these parameters are variations

in outside diameter, wall thickness, section length or height of the structure, and luminaire

structure projected area. Excluded are two of the more sensitive parameters, structure damping

and wind velocity coefficient of variation (COV). Thus, at this time, a damping ratio for the

structure is assumed to be 1% and the wind velocity COV is assumed to be 25%. Recall,

however, that other studies have concluded that an appropriate COV for wind-loading is 35%,

thus yielding an approximate COV of 25% for wind velocity, if all other variables in Morison’s

equation are considered deterministic, i.e. not random. The luminaire structure weight is not

considered as a parameter in the design charts. As shown in Chapter 3, the luminaire structure

weight was shown to not severely affect the fatigue life or reliability of the HML structural

support. The luminaire projected area was more critical in this aspect. Any luminaire structure

that would be used would have a given weight and projected area. Thus, from these two

parameters it is concluded that the projected area of the luminaire structure is more important.

The first set of design charts, for single parameter variations, were developed in a similar fashion

to the reliability index figures in Section 3.4. However, in this case, the target fatigue life was

varied for 25 years, 50 years, and 75 years. As a result of this, reliability indices were calculated

for each variation of a particular parameter and mean wind velocity for a given target fatigue life.

As noted previously in Chapter 3, 50-year wind velocities, or design wind velocities, were

unable to be produced based on the sole knowledge of the parent wind velocity distribution.

Thus, the use of the single parameter design charts requires the knowledge of the mean, or

average, wind velocity for a particular site in Colorado. The appendix of this report does provide

an initial summary of mean wind velocities for various sites in Colorado. However, the data

used to compile this summary is limited and should not be used exclusively. Use of the single

parameter design charts, based on a given factor or parameter value such as outside diameter,

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target fatigue life and mean wind velocity produces a reliability index. A summary of the design

method used in conjunction with the single parameter design charts is presented in Section 4.3.

The first set of design charts were developed based on the assumption that only a single

parameter, such as wall thickness, is changing from the benchmark HML structure given in

Figure 3-1 and described in Tables 3-1 through 3-4. As this is likely never the case, a second set

of design charts for multiple parameter variations have been developed for multiple parameter

variations. The multiple parameter design charts do not require the use of the single parameter

design charts. A summary of the design method used in conjunction with the multiple parameter

design charts is presented in Section 4.5.

4.2 Design Charts – Single Variable

The design charts for a single variable are provided in the supplemental reports for detail

categories E and E′. These design charts were determined based on varying only the parameter

for which it is given: pole outside diameter, pole wall thickness, pole length, or luminaire

structure projected area. Thus, it is assumed that, for example, changes in outside diameter and

changes in wall thickness are independent. Or, changing one parameter does not require that

another parameter be changed.

4.3 Design Method – Single Variable

The design charts for a single variable were developed based on the assumption that only a single

parameter, or factor such as outside diameter, is changing from the benchmark HML structure

given in Figure 3-1 and described in Tables 3-1 through 3-4. If, however, it is known that only

one parameter is being varied from the benchmark HML structure, then the design procedure for

determining the single parameter based on a target reliability index, βHML, can be summarized as:

Step 1: Determine detail category at the base of the HML structural support based on

AASHTO specifications: E or E′.

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Step 2: Select single parameter to be varied: pole outside diameter, pole wall thickness,

pole length, or luminaire structure projected area.

Step 3: Determine the appropriate mean wind velocity, target fatigue life, and target

reliability index, βHML.

Step 4: Using the appropriate design chart based on the single parameter and target

fatigue life, determine the single parameter value based on mean wind velocity

and target reliability index, βHML.

Step 5: Determine all physical properties of HML structural support.

Step 5 requires that the properties of the benchmark HML structural support be modified. Table

4-1 provides the properties for this benchmark structure based on the four design parameters.

Tables 4-2 through 4-4 provide further details for pole outside diameter, pole wall thickness, and

pole section length. Table 4-5 provides further details for luminaire structure projected area. If

the single parameter varied is the pole outside diameter, pole wall thickness, or pole section

length then modification of the parameter must be done for all points along the height of the

pole. For example, if from Step 4, the pole outside diameter was found to be 20.8 in (528.32

mm), which corresponds to a 20% reduction from the original pole outside diameter, for a

particular mean wind velocity, target fatigue life, and target reliability index then the

corresponding reduction in all outside diameters along the height of the pole would be 20%.

Thus, reading from Table 4-2, all other outside diameters for the three sections that comprise the

pole could be easily determined. For cases in which the percent reduction or increase is not

given in the tables, linear interpolation is permitted.

Property Benchmark HML Structural Support

Outside Diameter (Base of Structure)

26.00 in (660.40 mm)

Wall Thickness (Base of Structure)

0.375 in (9.525 mm)

Total Length 120 ft (36.576 m)

Luminaire Structure Projected Area

11.50 ft2 (1.0684 m2)

Table 4-1: Benchmark HML Structural Support Properties

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Pole Outside Diameter Benchmark Properties

(No Change) -30% -20% -10% +10% +20% +30%

Bottom of Section

26.00 in (660.40 mm)

18.2 in (462.28 mm)

20.8 in (528.32 mm)

23.4 in (594.36 mm)

28.6 in (726.44 mm)

31.2 in (792.48 mm)

33.8 in (858.52 mm)

Sect

ion

1

Top of Section

18.51 in (470.15 mm)

12.957 in (329.11 mm)

14.808 in (376.12 mm)

16.659 in (423.14 mm)

20.361 in (517.17 mm)

22.212 in (564.18 mm)

24.063 in (611.20 mm)

Bottom of Section

19.50 in (495.30 mm)

13.65 in (346.71 mm)

15.6 in (396.24 mm)

17.55 in (445.77 mm)

21.45 in (544.83 mm)

23.4 in (594.36 mm)

25.35 in (643.89 mm)

Sect

ion

2

Top of Section

12.15 in (308.61 mm)

8.505 in (216.03 mm)

9.72 in (246.89 mm)

10.935 in (277.75 mm)

13.365 in (339.47 mm)

14.58 in (370.33 mm)

15.795 in (401.19 mm)

Bottom of Section

13.00 in (330.20 mm)

9.1 in (231.14 mm)

10.4 in (264.16 mm)

11.7 in (297.18 mm)

14.3 in (363.22 mm)

15.6 in (396.24 mm)

16.9 in (429.26 mm)

Sect

ion

3

Top of Section

10.18 in (258.57 mm)

7.126 in (181.00 mm)

8.144 in (206.86 mm)

9.162 in (232.71 mm)

11.198 in (284.43 mm)

12.216 in (310.29 mm)

13.234 in (336.14 mm)

Table 4-2: Pole Outside Diameter Properties

Pole Wall Thickness Benchmark Properties

(No Change) -30% -20% -10% +10% +20% +30%

Section 1 0.375 in (9.525 mm)

0.2625 in (6.6675 mm)

0.3 in (7.62 mm)

0.3375 in (8.5725 mm)

0.4125 in (10.478 mm)

0.45 in (11.43 mm)

0.4875 in (12.383 mm)

Section 2 0.250 in (6.350 mm)

0.175 in (4.445 mm)

0.2 in (5.08 mm)

0.225 in (5.715 mm)

0.275 in (6.985 mm)

0.3 in (7.62 mm)

0.325 in (8.255 mm)

Section 3 0.2391 in (6.0731 mm)

0.16737 in (4.2512 mm)

0.19128 in (4.8585 mm)

0.21519 in (5.4658 mm)

0.26301 in (6.6805 mm)

0.28692 in (7.2878 mm)

0.31083 in (7.8951 mm)

Table 4-3: Pole Wall Thickness Properties

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Pole Section Length Benchmark Properties

(No Change) -30% -20% -10% +10% +20% +30%

Section 1 53.49 ft (16.30 m)

37.443 ft (11.4126 m)

42.792 ft (13.0430 m)

48.141 ft (14.6734 m)

58.839 ft (17.9341 m)

64.188 ft (19.5645 m)

69.537 ft (21.1949 m)

Section 2 52.52 ft (16.01 m)

36.764 ft (11.2057 m)

42.016 ft (12.8065 m)

47.268 ft (14.4073 m)

57.772 ft (17.6089 m)

63.024 ft (19.2097 m)

68.276 ft (20.8105 m)

Section 3 20.16 ft (6.14 m)

14.112 ft (4.3013 m)

16.128 ft (4.9158 m)

18.144 ft (5.5303 m)

22.176 ft (6.7592 m)

24.192 ft (7.3737 m)

26.208 ft (7.9882 m)

Total Length 120 ft (36.576 m)

84 ft (25.6032 m)

96 ft (29.2608 m)

108 ft (32.9184 m)

132 ft (40.2336 m)

144 ft (43.8912 m)

156 ft (47.5488 m)

Table 4-4: Pole Section Length Properties

Luminaire Structure Projected Area

Benchmark Properties

(No Change) -30% -20% -10% +10% +20% +30%

Projected Area 11.50 ft2 (1.0684 m2)

8.05 ft2 (0.74787 m2)

9.2 ft2 (0.85471 m2)

10.35 ft2 (0.96155 m2)

12.65 ft2 (1.1752 m2)

13.8 ft2 (1.2821 m2)

14.95 ft2 (1.3889 m2)

Table 4-5: Luminaire Structure Projected Area Properties

Verification of the design method for a single variable is provided for four examples as outlined

in Table 4-6 for detail categories E and E′. Table 4-7 provides a summary of the results of these

examples. In Table 4-7, the column marked “Full Simulation” indicates that a full analysis using

the computer simulation program written by the authors was used to determine the reliability

index. The columns contained by the heading “Design Chart Method” makes use of the design

charts provided in the supplemental report for detail categories E and E′. Tables 4-8 and 4-9

provide the resulting properties and percent change from the benchmark HML structural support

from the examples considered in Table 4-6 respectively. The reader is also referred to Chapter 5

for an additional detailed example of the design method for a single variable.

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Example Number

Outside Diameter at Bottom of Structure

Wall Thickness at Bottom

of Structure

Total Length

Luminaire Structure Projected

Area

Mean Wind Velocity

Target Fatigue

Life

AASHTO Detail

Category

Example 1 Variable No Change No Change No Change 12 MPH (19.31 km/hr) 50 Years E

Example 2 No Change Variable No Change No Change 14 MPH (22.53 km/hr) 25 Years E

Example 3 No Change No Change Variable No Change 14 MPH (22.53 km/hr) 75 Years E′

Example 4 No Change No Change No Change Variable 12 MPH (19.31 km/hr) 75 Years E′

Table 4-6: Design Method Confirmation Examples – Single Variable

Full Simulation Design Chart Method

Example Number

β Unknown Parameter Target β

β Ratio

Example 1 2.998 Outside Diameter 3.0 0.999

Example 2 2.687 Wall Thickness 2.5 1.075

Example 3 2.511 Total Height 2.5 1.004

Example 4 2.851 Projected Area 3.0 0.950

Table 4-7: Design Method Confirmation Summary – Single Variable

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Example Number

Outside Diameter at Bottom of Structure

Wall Thickness at Bottom of

Structure Total Length

Luminaire Structure

Projected Area

Example 1 20.8 in (528.32 mm)

0.375 in (9.525 mm)

120 ft (36.576 m)

11.5 ft2 (1.0684 m2)

Example 2 26 in (660.4 mm)

0.2625 in (6.668 mm)

120 ft (36.576 m)

11.5 ft2 (1.0684 m2)

Example 3 26 in (660.4 mm)

0.375 in (9.525 mm)

108 ft (32.918 m)

11.5 ft2 (1.0684 m2)

Example 4 26 in (660.4 mm)

0.375 in (9.525 mm)

120 ft (36.576 m)

14.375 ft2 (1.335 m2)

Table 4-8: Design Method Confirmation Properties – Single Variable

Example Number

Outside Diameter at Bottom of Structure

Wall Thickness at Bottom of

Structure Total Length

Luminaire Structure

Projected Area

Example 1 -20% No Change No Change No Change

Example 2 No Change -30% No Change No Change

Example 3 No Change No Change -10% No Change

Example 4 No Change No Change No Change +25%

Table 4-9: Design Method Confirmation Percent Changes – Single Variable

Based on the summary given in Table 4-7, the design charts for a single variable are, on average,

approximately 1% conservative. Example 4, however, does provide a reliability index from the

design charts that is higher than the reliability index calculated from the full computer

simulation. The design chart is thus approximately 5.2% higher than the computer simulation.

This result is not unexpected due to the complexity of the analysis. Furthermore, the results are

still reasonably accurate.

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4.4 Design Charts – Multiple Variables

The design charts for multiple variables are provided in the supplemental reports for detail

categories E and E′. These design charts were determined based on assumed values for pole

outside diameter, pole length, and luminaire structure projected area. Reasonable values were

assumed for these three variables. Pole wall thickness values were varied for several

combinations of the three assumed variables.

4.5 Design Method – Multiple Variables

The design charts for multiple variables were developed based on assumed values for pole

outside diameter, pole length, and luminaire structure projected area. Reasonable values were

assumed for these three variables. Pole wall thickness values were varied for several

combinations of the three assumed variables. Prior conversations with CDOT personnel

conveyed the desire to select the pole outside diameter and pole wall thickness for a given pole

length and luminaire structure. Thus, the design procedure for determining the parameters based

on a target reliability index, βHML, can be summarized as:

Step 1: Determine detail category at the base of the HML structural support based on

AASHTO specifications: E or E′.

Step 2: Select pole length, or height of the HML structural support, from three choices:

100 ft (30.48 m), 120 ft (36.576 m), or 140 ft (42.672 m).

Step 3: Select luminaire structure projected area from three choices: 7.5 ft2 (0.6968 m2),

9.5 ft2 (0.8826 m2), or 11.5 ft2 (1.0684 m2).

Step 4: Determine the appropriate mean wind velocity, target fatigue life, and target

reliability index, βHML.

Step 5: Select an appropriate pole outside diameter from three choices: 23.4 in (594.36

mm), 26 in (660.4 mm), or 28.6 in (726.44 mm).

Step 6: Using the appropriate design chart based on the pole outside diameter, mean wind

velocity, and target fatigue life, determine the pole wall thickness based on the

pole length, luminaire structure projected area, and target reliability index, βHML.

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Step 7: Determine all physical properties of HML structural support.

Step 7 requires that the properties of the benchmark HML structural support be modified. As

before, Table 4-1 provides the properties for this typical structure based on the four design

parameters. Tables 4-2 through 4-4 provide further details for pole outside diameter, pole wall

thickness, and pole section length. Table 4-5 provides further details for luminaire structure

projected area. The same procedure as was explained for Step 5 of the design method for a

single variable is applicable to Step 7 for the design method for multiple variables.

Verification of the design method for multiple variables is provided for four examples as

outlined in Table 4-10 for detail categories E and E′. Table 4-7 provides a summary of the

results of these examples. In Table 4-11, the column marked “Full Simulation” indicates that a

full analysis using the computer simulation program written by the authors was used to

determine the reliability index. The columns contained by the heading “Design Chart Method”

makes use of the design charts provided in the supplemental report for detail categories E and E′.

Tables 4-12 and 4-13 provide the resulting properties and percent change from the benchmark

HML structural support from the examples considered in Table 4-10 respectively. The reader is

also referred to Chapter 5 for an additional detailed example of the design method for a single

variable.

Example Number

Outside Diameter at Bottom of Structure

Wall Thickness at Bottom

of Structure

Total Length

Luminaire Structure Projected

Area

Mean Wind Velocity

Target Fatigue

Life

AASHTO Detail

Category

Example 1 Assumed:

28.6 in (726.44 mm)

Variable Assumed:

140 ft (42.672 m)

Assumed: 11.5 ft2

(1.0684 m2)

12 MPH (19.31 km/hr) 75 Years E

Example 2 Assumed:

26 in (660.4 mm)

Variable Assumed:

120 ft (36.576 m)

Assumed: 9.5 ft2

(0.8826 m2)

14 MPH (22.53 km/hr) 50 Years E

Example 3 Assumed:

23.4 in (594.36 mm)

Variable Assumed:

120 ft (36.576 m)

Assumed: 7.5 ft2

(0.6968 m2)

12 MPH (19.31 km/hr) 25 Years E′

Example 4 Assumed:

26 in (660.4 mm)

Variable Assumed:

140 ft (42.672 m)

Assumed: 9.5 ft2

(0.8826 m2)

14 MPH (22.53 km/hr) 50 Years E′

Table 4-10: Design Method Confirmation Examples – Multiple Variables

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Full Simulation Design Chart Method

Example Number

β Unknown Parameter Target β

β Ratio

Example 1 3.187 Wall Thickness 3.0 1.062

Example 2 2.524 Wall Thickness 2.5 1.010

Example 3 2.763 Wall Thickness 2.75 1.005

Example 4 2.037 Wall Thickness 2.0 1.019

Table 4-11: Design Method Confirmation Summary – Multiple Variables

Example Number

Outside Diameter at Bottom of Structure

Wall Thickness at Bottom of

Structure Total Length

Luminaire Structure

Projected Area

Example 1 28.6 in (726.44 mm)

0.345 in (8.763 mm)

140 ft (42.672 m)

11.5 ft2 (1.0684 m2)

Example 2 26 in (660.4 mm)

0.3 in (7.62 mm)

120 ft (36.576 m)

9.5 ft2 (0.8826 m2)

Example 3 23.4 in (594.36 mm)

0.25 in (6.35 mm)

120 ft (36.576 m)

7.5 ft2 (0.6968 m2)

Example 4 26 in (660.4 mm)

0.445 in (11.303 mm)

140 ft (42.672 m)

9.5 ft2 (0.8826 m2)

Table 4-12: Design Method Confirmation Properties – Multiple Variables

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Example Number

Outside Diameter at Bottom of Structure

Wall Thickness at Bottom of

Structure Total Length

Luminaire Structure

Projected Area

Example 1 +10% -8% +16.7% No Change

Example 2 No Change -20% No Change -17.4%

Example 3 -10% -33.33% No Change -34.8%

Example 4 No Change +18.67% +16.7% -17.4%

Table 4-13: Design Method Confirmation Percent Changes – Multiple Variables

Based on the summary given in Table 4-11, the design charts for multiple variables are, on

average, approximately 2% conservative. As with the design charts for a single variable, these

results are not unexpected due to the complexity of the analysis. Furthermore, the results are still

reasonably accurate for all four examples.

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CHAPTER 5

ILLUSTRATIVE DESIGN EXAMPLES FOR FATIGUE PERFORMANCE

5.1 Example 1 – Single Variable

Illustrative example 1 considers an HML structural support design for a mean wind velocity of

12 MPH (19.31 km/hr) with a target fatigue life of 50 years and detail category E. A target

reliability index, βHML, of 3.0 is desired for the HML structural support. Only pole wall

thickness is considered to vary from the benchmark HML structural support used in this study.

All other factors, pole outside diameter, pole length, and luminaire structure projected area, are

considered to be consistent with the benchmark HML structural support. Therefore, there values

are 26 in (660.4 mm), 120 ft (36.576 m), and 11.5 ft2 (1.0684 m2) respectively.

Using the design charts for a single variable from the supplemental report for detail category E

with a mean wind velocity of 12 MPH (19.31 km/hr), a target fatigue life of 50 years, and a

target reliability index of 3.0, the pole wall thickness is determined as shown in Figure 5-1.

Figure 5-1: Example 1 – Single Variable

Based on the results from Figure 5-1, the wall thickness has been reduced 25% to 0.28125 in

(7.144 mm) compared to the benchmark HML structure wall thickness of 0.375 in (9.525 mm) at

the base of the structure.

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The target reliability index for the structure is 3.0. A full analysis using the computer simulation

program written by the authors determined that the reliability index of the structure used in this

example was 2.972. Recall that the design method proposed for a single variable produces, on

average, designs that are approximately 1% conservative. For this example, the target reliability

index of 3.0 is 0.9% higher than the calculated reliability index of 2.972.

The final step in the design process that must be completed is the adjustment of the physical

properties of the HML structural support, or Step 5 in the design process for a single variable.

The wall thickness of the entire structure must be reduced by 25% at all points. There were no

changes to the outside diameter, length, or luminaire structure projected area. Therefore, their

values remain at 26 in (660.4 mm), 120 ft (36.576 m), and 11.5 ft2 (1.0684 m2) respectively.

5.2 Example 2 – Multiple Variables

Illustrative example 2 considers an HML structural support design for a mean wind velocity of

14 MPH (22.53 km/hr) with a target fatigue life of 50 years and detail category E′. A target

reliability index, βHML, of 2.5 is desired for the HML structural support. Initial requirements for

pole length and luminaire structure projected area are 100 ft (30.48 m) and 9.5 ft2 (0.8826 m2)

respectively. Values for pole outside diameter and pole wall thickness are thus needed for the

desired target reliability index. It is assumed that the pole outside diameter is set at 23.4 in

(594.36 mm). Thus, the pole wall thickness is considered to vary.

Using the design charts for multiple variables from the supplemental report for detail category E′

with a mean wind velocity of 14 MPH (22.53 km/hr), a target fatigue life of 50 years, a pole

outside diameter of 23.4 in (594.36 mm), and a target reliability index of 2.5, the pole wall

thickness is determined as shown in Figure 5-2.

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Figure 5-2: Example 2 – Multiple Variables

Based on the results from Figure 5-2, the wall thickness has been decreased 15.33% to 0.3175 in

(8.065 mm) compared to the benchmark HML structure wall thickness of 0.375 in (9.525 mm) at

the base of the structure. Furthermore, the pole outside diameter has been reduced 10% to 23.4

in (594.36 mm) compared to the benchmark HML structure outside diameter of 26 in (660.4

mm) at the base of the structure. The pole length has been decreased 16.7% to 100 ft (30.48 m)

compared to the benchmark HML structure length of 120 ft (36.576 m). Finally, the luminaire

structure projected area has been decreased 17.4% to 9.5 ft2 (0.8826 m2) compared to the

benchmark luminaire structure projected area of 11.5 ft2 (1.0684 m2).

The target reliability index for the structure is 2.5. A full analysis using the computer simulation

program written by the authors determined that the reliability index of the structure used in this

example was 2.472. Recall that the design method proposed for multiple variables produces, on

average, designs that are approximately 2% conservative. For this example, the target reliability

index of 2.5 is 1.1% higher than the calculated reliability index of 2.472.

Again, one final step in the design process that must be completed is the adjustment of the

physical properties of the HML structural support, or Step 7 in the design process for multiple

variables. The outside diameter and wall thickness of the entire structure must be decreased by

10% and 15.33%, respectively, at all points.

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81

CHAPTER 6

SUMMARY, CONCLUSIONS AND RECOMMENATIONS

In this report the method and results for the development of a reliability-based design procedure

for high-mast lighting structural supports in Colorado were presented. A computational fluid

dynamics (CFD) approach was coupled with finite element theory in order to model the in-line

dynamic motion of high mast lighting structural supports. Common frequencies and wind

velocity combinations associated with vortex shedding were also examined and presented in the

appendix of the report. Six structural and two wind-related parameters were varied and their

sensitivity on fatigue life examined. Based on these sensitivities, design charts were developed

for single and multiple variable variations and are given in the supplemental reports for detail

categories E and E′ defining the AASHTO connection type at the base of the HML structural

support. The design charts for the multiple variable variations were developed based on

conversations with CDOT personnel. Results determined from the design charts compared well

with those obtained from a full computer simulation. The two wind-related parameters in this

study were based on expert judgment, but will require verification beyond the present study’s

scope, prior to implementation of the methodology around the state of Colorado.

The approach presented herein is general and can be applied to virtually any type of high mast

lighting structure that has a reasonable number of design parameters. Tabulated values could

also be generated rather than plots, when it is sought to implement the methodology. It can be

concluded based on the results of the two examples that for the general population of high mast

lighting structural supports in Colorado, the methodology will work well provided that accurate

wind statistics can be developed.

Thus, it is highly recommended that CDOT consider a wind study along Colorado’s Front Range

(and other locations, if desired), thus mapping any inconsistencies with ASCE-7 mapped values,

which are known to be quite coarse. Additionally, this study must also create a link between the

mean wind velocities used in this report and appropriate 50-year wind velocities along

Colorado’s Front Range. Further, current 50-year wind velocities used in the state of Colorado

by CDOT, which range from 90 to 110 MPH (144.84 to 177.03 km/hr) may or may not be

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82

justified. The answer to this question is unknown both at the state and national level and is

deserving of the amount of attention that would be required to solve this important problem.

Such a study would have immediate implications on all traffic-related structures, such as signal

poles and arms, whose numbers are far greater than high mast lighting structural supports.

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83

REFERENCES

AASHTO (2001). With interims. “Standard Specifications for Structural Supports for Highway Signs, Luminaires and Traffic Signals”, 4th Edition. American Association of State Highway and Transportation Officials, Washington, D.C.

Ang, A.H-S. and W.H. Tang (1975). Probability Concepts in Engineering Planning and Design,

Volume 1. John Wiley and Sons, New York. ASCE 7-05 (2005). “Minimum Design Loads for Buildings and Other Structures”. American

Society of Civil Engineers, Reston, VA. Assakkaf, I., and Ayyub (2000), B.M., “Load and Resistance Factor Design Approach for

Fatigue of Marine Structures”, 8th ASCE Specialty Conference on Probabilistic Mechanics and Structural Reliability, ASCE, University of Notre Dame, South Bend, IN.

Chopra, A.K. (2001). Dynamics of Structures, 2nd Edition. Prentice Hall, Upper Saddle River,

NJ. Crandall, S.H. and W.D. Mark (1963). Random Vibration of Mechanical Systems. Academic

Press, New York and London. Holmes, J.D. (2001). Wind Loading of Structures. Spon Press, New York. Kaufmann, E.J. (2005). “Investigation of Cracking in High-Mast Light Poles at E-470 and Pena

Boulevard, Denver, Colorado”. ATLSS, Lehigh University, Bethlehem, PA. Kwon, Y.W. and H. Bang (2000). The Finite Element Method Using MATLAB, 2nd Edition. CRC

Press, New York. Miner, M.A. (1945). “Cumulative Damage in Fatigue”. Journal of Applied Mechanics, 12, A159. Morison, J.R., O’Brien, M.P., Johnson, J.W. and S.A. Schaaf (1950). “The Force Exerted by

Surface Waves on Piles”. AIME Petroleum Transactions, 189, 149-157. Newmark, N.M. (1959). “A Method of Computation for Structural Dynamics”. Trans. ASCE,

American Society of Civil Engineers, 109(111). Paz, M. and W. Leigh (2004). Structural Dynamics, 5th Edition. Kluwer Academic Publishers,

Boston. Simiu, E. and R.H. Scanlan (1996). Wind Effects on Structures, 3rd Edition. John Wiley and

Sons, New York. Wilcox, D.C. (2003). Basic Fluid Mechanics, 2nd Edition. DCW Industries, La Cañada, CA.

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A-1

APPENDIX A

A.1 Vortex-Induced-Vibration

One major type of loading that slender structures are subjected to during wind loading is a

phenomenon known as vortex shedding. Vortex shedding occurs when vortices are formed and

shed in the wake just behind the cylinder, i.e. the mast of the HML. This section presents the

results of an investigation into vortex-induced-vibration (VIV) of HML structural supports.

Finite Element Model

In order to determine the fundamental period of vibration, Tn, and the harmonics, 1 2, , , nT T T , a

finite element model (FEM) that utilized twelve degree-of-freedom beam elements was

employed. The FEM details were presented in Chapter 2 of this report

Vortex Shedding Model

It has been reasoned that an empirical linear model for VIV provides significant and accurate

information for many engineering structures (Simiu, 1996). In order to derive this approach, we

begin with the forced equation of motion of a cylinder in fluid flow,

( )2

1sin2 LDmx cx kx C K sm

ρ θ+ + = − (A-1)

where m is the mass, c is the damping coefficient, and k is the structure stiffness. The value x is

the displacement and a dot indicates a time derivative, ρ is the mass density of air, D is the

diameter of the cylinder, θ is the phase angle, LC is an experimentally determined lift

coefficient, and

1nDK

= (A-2)

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A-2

where nω is the natural cyclic frequency of the structure, and U is the velocity of the wind flow,

and

UtsD

= (A-3)

where t is time. According to Simiu (1996) solving closed form for the steady state response of

the oscillator described by equations (A-1) and (A-2) yields an amplitude of

( ) ( )

2

2 22 21 1

2

2L

n n

D C m

K c K

ρηω ω

=− +

(A-4)

Notice that all quantities are known except the lift coefficient, CL. However, extensive

experiments have been performed on cylinders in fluids with uniform flow. Again, utilizing the

data provided in Simiu (1996), one can express the amplitude given in equation (A-4) as a

function of K1. In order to solve for CL one can rearrange equation (A-4) as

( ) ( )2 22 21 12

2 2L n nmC K c K

Dη ω ωρ

= − + (A-5)

Then, fitting the appropriate polynomial for the experimental data gives

( ) ( )1

2 20 2 21 12

22

nn i n

iL n n

m a KC K c K

Dω ω

ρ

=

⎧ ⎫⎨ ⎬⎩ ⎭= − +∑

(A-6)

where n is the order of the polynomial and i is simply the index in the summation.

For the illustration presented in this appendix it is only desired to determine if lock in occurs at

one or more of the three fundamental transverse frequencies. Because there were slight

variations in the wall thickness of the poles this will be varied as well. Table A-1 presents the

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A-3

results of the vortex induced vibration lock-in study described above. An “×” was placed in the

table when lock-in was identified by the numerical model.

First Transverse Mode Second Transverse Mode Third Transverse Mode Wall Thickness

Wind Speed MPH

(km/hr) -30% NC +30% -30% NC +30% -30% NC +30% 5

(8.05) × × × 10

(16.09) 15

(24.14) × × × 20

(32.19) × × × 25

(40.23) × × × 30

(48.28) 35

(56.33) × 40

(64.37) × × × 45

(72.42) × × × 50

(80.47) × × × 55

(88.51) × × × 60

(96.56) × × × 65

(104.61) × × 70

(112.65)

Table A-1: Wind Speed and Vibration Mode Combinations at which Lock-In was Numerically Identified

Interestingly, notice that some type of lock-in occurs at almost every wind speed. However, it is

very important to note that no taper of the HML structural support was considered here and these

results are presented for consideration of VIV sensitivity only.

A.2 Selected Mean Wind Velocities

A preliminary survey of readily available data for locations within Colorado was conducted to

determine mean wind velocities at the characteristic height of 33 ft (10 m). This data was

obtained from the Plains Organization for Wind Energy Resources (POWER) and Energy and

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A-4

Environmental Research Center (EERC) at the University of North Dakota. This data is

available online with the Internet address provided under the caption of the table. Data was

recorded hourly. Table A-2 summarizes the data obtained and Figure A-1 provides the locations

given in the table.

Location Record Length Mean Wind Velocity MPH (km/hr)

Mean Standard Deviation

MPH (km/hr)

Mean Turbulence Intensity (COV)

%

Boulder 4 years 8.38 (13.49)

1.57 (2.53) 18.68

Calhan 1 year 13.03 (20.97)

2.39 (3.85) 18.34

Cheyenne Wells 1 year 13.29 (21.39)

2.34 (3.77) 17.59

Genoa 1 year 13.72 (22.08)

2.38 (3.83) 17.31

Gobblers Knob (East) 1 year 13.45

(21.65) 2.25

(3.62) 16.74

Gobblers Knob (West) 1 year 12.90

(20.76) 2.29

(3.69) 17.73

Livermore 1 year 14.93 (24.03)

2.94 (4.73) 19.71

Mesa de Maya 1 year 12.08 (19.44)

2.31 (3.72) 19.09

Pawnee Buttes 1 year 16.21 (26.09)

2.48 (3.99) 15.31

Peetz 1 year 14.34 (23.08)

2.49 (4.01) 17.37

Wauneta 1 year 15.04 (24.20)

2.50 (4.02) 16.62

Table A-2: Mean Wind Velocities for Selected Locations in Colorado

Figure A-1: Selected Locations in Colorado

(Table A-2 and Figure A-1: http://www.undeerc.org/wind/winddb/COwindsites.asp)