Special edition paper

Similar documents
Fatigue Crack Analysis on the Bracket of Sanding Nozzle of CRH5 EMU Bogie

Centrifuge Shaking Table Tests and FEM Analyses of RC Pile Foundation and Underground Structure

FE-Analysis of Stringer-to-floor-beam Connections in Riveted Railway Bridges

Evaluation of dynamic behavior of culverts and embankments through centrifuge model tests and a numerical analysis

The University of Melbourne Engineering Mechanics

VERIFICATION TEST AND EARTHQUAKE RESPONSE OBSERVATION OF A BASE ISOLATED BUILDING WITH ECCENTRIC ROLLER BEARINGS

Sabah Shawkat Cabinet of Structural Engineering Walls carrying vertical loads should be designed as columns. Basically walls are designed in

HYSTERETIC PERFORMANCE OF SHEAR PANEL DAMPERS OF ULTRA LOW- YIELD-STRENGTH STEEL FOR SEISMIC RESPONSE CONTROL OF BUILDINGS

Title. Author(s)T. MIZUTANI; Y. NARAZAKI; Y. FUJINO. Issue Date Doc URL. Type. Note. File Information

ENG1001 Engineering Design 1

AN EXPERIMENTAL STUDY ON INELASTIC BEHAVIOR AND RESTORING FORCE CHARACTERISTICS OF VIBRATION CONTROL DEVICE AS STEEL SCALING-FRAME

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown.

Special edition paper

TRI-AXIAL SHAKE TABLE TEST ON THE THINNED WALL PIPING MODEL AND DAMAGE DETECTION BEFORE FAILURE

Study of Pile Interval of Landslide Restraint Piles by Centrifuge Test and FEM Analysis

Development of Spherical Sliding Bearing

Where and are the factored end moments of the column and >.

[5] Stress and Strain

FRICTION SLIPPING BEHAVIOR BETWEEN CONCRETE AND STEEL -AIMING THE DEVELOPMENT OF BOLTED FRICTION- SLIPPING JOINT -

Dynamic Analysis of a Reinforced Concrete Structure Using Plasticity and Interface Damage Models

Dynamic analysis of a reinforced concrete shear wall with strain rate effect. Synopsis. Introduction

STRUCTURAL PROPERTIES EVALUATION OF UNIQUE BOAT HOUSE USING OBLIQUE NUKI Part II: Cyclic Loading Test and Shear Force Estimation

Stress Analysis and Validation of Superstructure of 15-meter Long Bus under Normal Operation

EQUIVALENT FRACTURE ENERGY CONCEPT FOR DYNAMIC RESPONSE ANALYSIS OF PROTOTYPE RC GIRDERS

MECHANICS OF STRUCTURES SCI 1105 COURSE MATERIAL UNIT - I

Junya Yazawa 1 Seiya Shimada 2 and Takumi Ito 3 ABSTRACT 1. INTRODUCTION

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS

CWR track vibration characteristics varying with the change of supporting condition

SEISMIC PERFORMANCE EVALUATION METHOD FOR A BUILDING WITH CENTER CORE REINFORCED CONCRETE WALLS AND EXTERIOR STEEL FLAME

SYSTEM IDENTIFICATION & DAMAGE ASSESSMENT OF STRUCTURES USING OPTICAL TRACKER ARRAY DATA

Design of Beams (Unit - 8)

INFLUENCE OF LOADING RATIO ON QUANTIFIED VISIBLE DAMAGES OF R/C STRUCTURAL MEMBERS

Section 19.1: Forces Within Earth Section 19.2: Seismic Waves and Earth s Interior Section 19.3: Measuring and Locating.

Pseudo-dynamic tests in centrifugal field for structure-foundation-soil systems

Brittle Deformation. Earth Structure (2 nd Edition), 2004 W.W. Norton & Co, New York Slide show by Ben van der Pluijm

SHAKING TABLE TEST OF STEEL FRAME STRUCTURES SUBJECTED TO NEAR-FAULT GROUND MOTIONS

A STUDY ON DAMAGE TO STEEL PIPE PILE FOUNDATION ON RECLAIMED LAND DURING HYOGO-KEN-NANBU EARTHQUAKE

EARTHQUAKE SIMULATION TESTS OF BRIDGE COLUMN MODELS DAMAGED DURING 1995 KOBE EARTHQUAKE

CONNECTION DESIGN. Connections must be designed at the strength limit state

FLEXIBILITY METHOD FOR INDETERMINATE FRAMES

Peak Strain and Displacement Sensors for Structural Health Monitoring

APPENDIX G I-BEAM SUMMARIES 0.6-IN. STRAND G-1

SHAKING TABLE TESTS ON SEISMIC RESPONSE REDUCTION EFFECTS OF ROCKING BUILDING STRUCTURAL SYSTEMS

Dynamic Response of Timber-Plywood Joints under Forced Harmonic Vibrations

Tracker Tower 01 Prototype Test & Analysis Overview

Experimental Study and Numerical Simulation on Steel Plate Girders With Deep Section

Rigid and Braced Frames

Entrance exam Master Course

Nonlinear static analysis PUSHOVER

Structural Calculations for Juliet balconies using BALCONY 2 System (Aerofoil) handrail. Our ref: JULB2NB Date of issue: March 2017

Analysis of the Full-scale Seven-story Reinforced Concrete Test Structure

Earthquakes. Forces Within Eartth. Faults form when the forces acting on rock exceed the rock s strength.

Experiment Two (2) Torsional testing of Circular Shafts

CHAPTER 5. T a = 0.03 (180) 0.75 = 1.47 sec 5.12 Steel moment frame. h n = = 260 ft. T a = (260) 0.80 = 2.39 sec. Question No.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each.

QUANTITATIVE ANALYSIS OF ACOUSTIC EMISSION WAVEFORMS AND. M.Ohtsu Department of Civil and Environmental Eng. Kumamoto University Kumamoto 860, Japan

N = Shear stress / Shear strain

COLUMN BASE WEAK AXIS ALIGNED ASYMMETRIC FRICTION CONNECTION CYCLIC PERFORMANCE

Downloaded from Downloaded from / 1

1. A pure shear deformation is shown. The volume is unchanged. What is the strain tensor.

COEFFICIENT OF DYNAMIC HORIZONTAL SUBGRADE REACTION OF PILE FOUNDATIONS ON PROBLEMATIC GROUND IN HOKKAIDO Hirofumi Fukushima 1

TABLE OF CONTENTS SECTION TITLE PAGE 2 PRINCIPLES OF SEISMIC ISOLATION OF BRIDGES 3

Field Investigation and Dynamic Analysis of Damaged Structure on Pile Foundation during the 2011 off the Pacific Coast of Tohoku Earthquake

NAME: Given Formulae: Law of Cosines: Law of Sines:

QUESTION BANK DEPARTMENT: CIVIL SEMESTER: III SUBJECT CODE: CE2201 SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A

Supplement: Statically Indeterminate Trusses and Frames

ASIAN JOURNAL OF CIVIL ENGINEERING (BUILDING AND HOUSING) VOL. 10, NO. 5 (2009) PAGES **-**

Collapse modes of structures under strong motions of earthquake

Effect of Deformation Mode of Cylindrical Tubes with Corrugated Surface Dimensional Errors

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering

Lecture 19. Measurement of Solid-Mechanical Quantities (Chapter 8) Measuring Strain Measuring Displacement Measuring Linear Velocity

Author(s) Sawamura, Yasuo; Kishida, Kiyoshi;

ME 243. Mechanics of Solids

STRUCTURAL ANALYSIS OF THE LIFTING DEVICE DETECTOR SUPPORTS FOR THE LHCb VERTEX LOCATOR (VELO)

Section Forces Within Earth. 8 th Grade Earth & Space Science - Class Notes

SHEAR CAPACITY OF REINFORCED CONCRETE COLUMNS RETROFITTED WITH VERY FLEXIBLE FIBER REINFORCED POLYMER WITH VERY LOW YOUNG S MODULUS

IMPACT RESPONSE ANALYSIS OF LARGE SCALE RC GIRDER WITH SAND CUSHION

A Modified Response Spectrum Analysis Procedure (MRSA) to Determine the Nonlinear Seismic Demands of Tall Buildings

Comparison of Structural Models for Seismic Analysis of Multi-Storey Frame Buildings

CE5510 Advanced Structural Concrete Design - Design & Detailing of Openings in RC Flexural Members-

Chapter 5. Vibration Analysis. Workbench - Mechanical Introduction ANSYS, Inc. Proprietary 2009 ANSYS, Inc. All rights reserved.

Numerical Modelling of Dynamic Earth Force Transmission to Underground Structures

DEVELOPMENT OF SEISMIC ISOLATION TABLE COMPOSED OF AN X-Y TABLE AND WIRE ROPE ISOLATORS

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS

[8] Bending and Shear Loading of Beams

BIAXIAL STRENGTH INVESTIGATION OF CFRP COMPOSITE LAMINATES BY USING CRUCIFORM SPECIMENS

Tension Members. ENCE 455 Design of Steel Structures. II. Tension Members. Introduction. Introduction (cont.)

Finite Element Modelling with Plastic Hinges

Title. Author(s)DONG, Q.; OKAZAKI, T.; MIDORIKAWA, M.; RYAN, K.; SAT. Issue Date Doc URL. Type. Note. File Information BEARINGS

Structural behaviour of traditional mortise-and-tenon timber joints

A study of action point correction factor for L type flanges of wind turbine towers

2012 MECHANICS OF SOLIDS

Seismic design of bridges

ENERGY DIAGRAM w/ HYSTERETIC

PEER/SSC Tall Building Design. Case study #2

Lecture 20. Measuring Pressure and Temperature (Chapter 9) Measuring Pressure Measuring Temperature MECH 373. Instrumentation and Measurements

ΙApostolos Konstantinidis Diaphragmatic behaviour. Volume B

FURTHER RESEARCH ON CHORD LENGTH AND BOUNDARY CONDITIONS OF CHS T- AND X-JOINTS

Estimation of the characteristic of contact line uplift and strain in the neighborhood of a tunnel inlet by computer simulation

Seismic Response Analysis of Structure Supported by Piles Subjected to Very Large Earthquake Based on 3D-FEM

Transcription:

Development of New Aseismatic Structure Using Escalators Kazunori Sasaki* Atsushi Hayashi* Hajime Yoshida** Toru Masuda* Aseismatic reinforcement work is often carried out in parallel with improvement work for barrier-free access. Generally, braces have been installed in conventional aseismatic reinforcement. Based on the idea that substituting escalators installed in improvement work for addition of new braces can minimize obstruction to existing buildings, we have decided to undertake development of a new aseismatic mechanism using escalators. In this study, we confirmed behavior by analysis of escalator truss frames and behavior and performance of escalators using a full size aseismatic escalator. The confirmation results have proved that the developed aseismatic escalator has sufficient performance as an aseismatic member for structures such as over-track station buildings. Keywords Over-track station building, Aseismatic escalator, Aseismatic reinforcement, Three-dimensional FEM analysis, Full size model experiment 1 Introduction Aseismatic reinforcement projects are proceeding at many places in the JR East jurisdiction. Up to now, we have adopted the method by which we increase bearing force by adding braces, as shown in Fig. 1 (a). In this method, however, there are major restrictions because the work is done on buildings in use. Some works also involve compensation for business in commercial areas where construction takes place. Furthermore, placing wall-type aseismatic mechanisms is undesirable in terms of construction planning as that narrows usable space range. There is thus demand for a reinforcement method to solve those problems by effectively improving aseismatic performance while minimizing obstruction to existing buildings. Reinforcement work is often carried out in parallel with improvement work for barrier-free access involving installing escalators or elevators. As we usually do not regard escalators or elevators as construction members, we had not considered having them bear horizontal force. But, if we can regard those, escalators in particular, as components of aseismatic mechanisms, we can effectively improve aseismatic performance while keeping obstruction to existing buildings at a minimum. We thus have decided to undertake development of new aseismatic structure using escalators. In this article, we call escalators that resist horizontal force aseismatic escalators. We have designed the structure of such aseismatic escalators to be able to reduce the number of reinforcement members such as braces by making them bear part of horizontal force at earthquakes in the longitudinal direction, as shown in Fig. 1 (b). The premise is that steps, motors and other mechanical parts of such escalators are not damaged, even when bearing horizontal seismic load. 2 Specifications of Aseismatic Escalators and Three-Dimensional FEM Analysis 2.1 Specifications of Aseismatic Escalators Taking into account the premise that mechanical parts of aseismatic escalators such as steps and motors will not be damaged, we * Frontier Service Development Laboratory, Research and Development Center of JR East Group ** Tokyo Construction Office (Previously at Frontier Service Development Laboratory) General floors Track floor (a) Conventional method (b) Developed Method Bearing seismic force determined spec targets of the developed aseismatic escalators. Those are that the structure components of the escalator truss show stress within the elasticity range when the maximum horizontal force is applied to them. At the same time, we decided to drive piles under the escalator pit for horizontal resistance. And no damage is done to mechanical parts of the escalator even when bearing horizontal force at earthquakes. Based on understanding of performance of a standard escalator frame without reinforcement by three-dimensional FEM analysis, we developed a reinforcement method to make that frame a sufficient aseismatic member. 2.2 Reinforcement Method for Standard Escalator Frames We calculated the shear force that an aseismatic escalator bears from the total of horizontal resistance of piles and pit frame, and we assumed the maximum seismic horizontal force that affects the aseismatic escalator to be 682.5 kn. In the analysis by applying that load to a standard escalator frame, we gained the stress contour figure shown in Fig. 2. The figure shows that larger stress than yield stress ESC ESC Bearing seismic force Reinforcement by braces Use of escalator truss as brace Fig. 1 Images of Conventional Method and Newly Developed Method Pile Pit Pit Pile 21

was generated near the upper and lower bends where the escalator truss frame changes from horizontal to sloped direction, and that stress is beyond the elasticity range. That means that upper and lower bends are weak parts (circled with dashed line). Analysis conditions Horizontal input Equal distribution at upper support beam panel points Support conditions Bonded in X and Z directions (upper support beam) Equally distributed load of Bonded in X and Z directions 682.5 kn/65 (nodes) (intermediate support) Fully bonded (lower support beam) (1) Upper bend reinforcement (3) (1) Upper bend reinforcement (2) (1) Upper bend reinforcement (4) (3) Intermediate panel reinforcement (1) Upper bend reinforcement (1) (8) Upper support beam (9) Frame end support Support point (2) Upper panel reinforcement (4) Lower bend reinforcement (2) (3) Intermediate panel reinforcement (4) Lower bend (7) Bottom horizontal reinforcement (1) truss (13) Lower support (10) Intermediate support beam (6) Intermediate horizontal truss (11) Lower slope support reinforcement (1) Longitudinal/diagonal (11) Lower slope support reinforcement (2) (5) Lower panel reinforcement (12) Frame end support Support point (7) Bottom horizontal truss (General parts) (Under upper bend) Total stress distribution * (1) - (7) New reinforcement structure (9) (11) (12) New support structure (8) (10) (13) Conventional structure Fig. 3 Frame Reinforcement Structure Plan Distribution of larger stress than yield stress Fig. 2 Stress Distribution Contour Figure of Standard Escalator Frame 682.5 kn/88.6 x 88.6 (area) x 4 (support points) Analysis conditions surface pressure Horizontal input Even distribution at supports of upper frame end Support condition Bonded in X and Z directions (upper support beam, intermediate support, upper frame end) Fully bonded (lower slope, lower frame end, lower support beam) Accordingly, some countermeasures to meet target specs are necessary. We thought up two measures (i) reinforcement of escalator frame components, and (ii) change of escalator frame support mechanism. Then, we studied details of aseismatic escalators with those measures combined. In countermeasure (i), we reinforced weak parts ((1) to (7) in Fig. 3) to improve cross-sectional performance of each component. In countermeasure (ii), we examined the support method that involves no major change of upper and lower fit of the standard escalator pit ((9), (10) and (11) in Fig. 3). In this development, we examined three-section escalators of story height 6 m, which are actually deployed in many stations, and added an intermediate support at 2.4 m story height. No stress larger than yield stress is distributed. Fig. 4 Stress Contour Figure of Aseismatic Escalator Frame by Three-Dimensional FEM Analysis 682.5 kn/88.6 x 88.6 (area) x 4 (support points) surface pressure 2.3 Three-Dimensional FEM Analysis of Aseismatic Escalator Frames In the model analyzed and given support structures as introduced in the previous section (Fig. 3), we applied 682.5 kn seismic horizontal force as equally distributed pressure at the escalator upper end support. We used it to check behavior such as stress and deformation at each point. Fig. 4 indicates the stress contour figure of that frame by three-dimensional FEM analysis. In Fig. 4, we confirmed that the reinforcement shown in Fig. 3 successfully reduced stress of every component including upper and lower bends of a standard escalator frame (the weak parts) to less than the yield stress. We further applied three-dimensional FEM analysis under the same analysis conditions in the case where the lower full-surface panel reinforcement shown in Fig. 3 (5) is divided into upper and lower panels. Stress and deformation figure by this analysis is shown in Fig. 5 and 6. Fig. 5 proved that stress of components is still less than the yield stress, even when the lower full-surface panel reinforcement is omitted. Fig. 6 also shows that deflection of the aseismatic escalator δ is 3.8 mm for the maximum span of 7.2 m (interval between intermediate support and upper bend) and that the maximum displacement at the ESC upper end is 6.1 mm. Deformation is thus minimal for both. Based on those analysis results, we have determined the escalator frame shown in Fig. 5 and 6 as the finalized design detail of the aseismatic escalator frame. Fig. 5 Contour Figure of Finalized Aseismatic Escalator Frame by Three-Dimensional FEM Analysis 3 Intermediate support 30 times deformation magnification Loading Test and Simulation of Aseismatic Escalator Upper bend 682.5 kn/88.6 x 88.6 (area) x 4 (support points) surface pressure Fig. 6 Deformation Contour Figure of Finalized Aseismatic Escalator Frame by Three-Dimensional FEM Analysis 3.1 Purpose In the previous section, we proposed a detailed aseismatic escalator frame, and we demonstrated by methods such as three-dimensional FEM analysis that such an escalator frame could remain within the elasticity range at the assumed seismic force. However, aseismatic escalators should have basic performance as escalators, and further function as an aseismatic component. Thus, we produced a fullsize aseismatic escalator, to perform final evaluation as an aseismatic escalator by analyzing loading test results. 22

3.2 Experiment Overview In order to identify features of an aseismatic escalator alone when receiving horizontal force, we produced an aseismatic escalator of 2.65 m story height shown in Fig. 7, and then carried out static loading tests and dynamic vibration tests. (Displacement scale) 1 mm 100 kn compression Left rail Glass Right rail Stainless steel ESC frame Reaction wall Fig. 9 Y and Z Direction Displacement Measurement Results at 100 kn Compression Pit reinforcement Base Fig. 7 Aseismatic Escalator Test Model 3.5.2 Escalator Frame Analysis Model Tests clarified that displacement occurred at support beam fixing points and pit reinforcement. In order to evaluate that displacement, we created an analysis model with beam model for the base and reflected that in analysis. Fig. 10 shows that model. Lower frame fixture Reaction wall ESC body Reaction wall Reaction floor Installation ESC frame Base 8540 100 kn vibration exciter Reaction wall Sill plate Anchor bolt Strain gauge (stress indication in Fig. 12) Equivalent rigid beam ESC frame 2650 ESC body Support beam and base beam welded to each other Rigid Reaction floor Rigid Pit reinforcement Fig. 8 Aseismic Escalator Loading Test Overview 3.3 Static Loading Test In static loading test, we fixed the lower part of the test model to the base (Fig. 7 and 8) fixed to the reaction wall and reaction floor. Then, we measured deformation and stress of the test model frame when ±100 kn load is applied in the longitudinal direction by a hydraulic vibration exciter. Displacement gauges were attached to 36 points and strain gauges to 180 points including reinforcement of upper and lower bends and upper and lower chords of the intermediate part. 3.4 Dynamic Vibration Test In the dynamic vibration test, we shook the test model with escalator frame upper and lower supports free in longitudinal direction at around 0 to 20 Hz. Based on the acceleration generated at the escalator frame, we calculated the natural frequency etc. of the frame. 3.5 Test Result and Analysis Validity Evaluation 3.5.1 Frame Deformation at Static Loading Fig. 9 shows displacement of escalator frame nodes in Y and Z directions at 100 kn compression. As shown in the figure, the escalator frame displaces to the left overall when compression load is applied. The upper bends deform more upward and lower bends downward. In other words, the frame deforms in a manner where angles of bends become more acute. Rigid Rigid Beam base model and Beam base model pit reinforcement fastened (H-shape steel cross at the center of bolts section 350 175 11) Fig. 10 Escalator Frame Analysis Model 3.6 Comparison of Experiment Values and Analysis Values Fig. 11 shows comparison result of analysis results using the analysis model in the previous section and measured displacement. Fig. 11 shows values of the upper right chords (see numbers in Fig. 9) at 100 kn compression. That figure is an example of data in the Y direction, and it confirmed that measurement results and analysis results agree well. We gained similar results in Z direction too. Next, Fig. 12 shows the results of comparison between analysis results using that analysis model and measured stress. Fig. 12 shows values near the upper bend shown in Fig. 10. Fig. 12 indicates that measurement results agree well with analysis results for stress too. We show stress data near the upper bend as an example, and similar tendency is seen for the most part at other points too. Here we showed only displacement the compression side; however, similar tendency is seen on tension side too. 3.7 Dynamic Vibration Test Results and Validity Evaluation of Natural Values of the Escalator Frame In dynamic vibration tests, we found natural frequency and damping ratio of the frame based on acceleration at different parts of escalators measured by acceleration sensors. Table 1 shows the measurement results, indicating that frequencies of the frame and that analysis results agree well with each other. We also confirmed that no failure such as resonance and no 23

remarkable change of mounting dimensions of component devices occurred during operation of that aseismatic escalator. Stress (MPa) Displacement (mm) Lower bend Analyzed value Joint Upper bend Measured value Fig. 11 Comparison of Displacement Measured and Analyzed Values at 100 kn Compression Measured value (at compression) Measured value (at tension) Distance from upper chord upper surface (mm) Analyzed value (at tension) Analyzed value (at compression) Fig. 12 Comparison of Stress Near Upper Bend Table 1 Frame Analysis Model Taking Analysis Elements into Account Degree Mode chart Primary bending in width direction Secondary bending in width direction Primary bending in deflection direction Table 2 Acceptable Horizontal Force and Displacement for Aseismatic Escalator Load direction Escalator longitudinal direction Escalator width direction Acceptable horizontal force Less than 682.5 kn Less than 36 kn Acceptable displacement Within ± 10 mm Within ± 20mm We examined the junction structure on the building side so horizontal force and displacement at the aseismatic escalator remain within target values in earthquakes. In escalator width direction, we chose the structure where horizontal force is not transferred and the aseismatic escalator goes back to the prescribed position after earthquake by applying sliding bearings. Since the sliding bearing part has four-degree V-shape slope structure, the escalator goes back to the home position with its own weight even after sliding and displacement in an earthquake. In escalator longitudinal direction, deformation performance is required between the building and the aseismatic escalator. We therefore added a low yield stress steel junction panel. When larger load than predicted is applied, that junction panel plastically deforms; so, larger horizontal force than predicted is not transformed to the aseismatic escalator. Based on that plan, we designed and produced actual junctions. Fig. 14 shows the specific plan of the junction for element tests. We produced mounting as a building and a test model for the aseismatic escalator truss to check function and performance of the bearing part by loading horizontal force in width direction on that model truss. In longitudinal direction, we extracted the low yield stress steel junction panel for between an aseismatic escalator truss and a building. By applying vertical load, we checked whether that could prevent the aseismatic escalator from bearing larger horizontal force than expected and whether it could follow relative displacement at earthquakes. 4 Natural frequency Measured Damping ratio Natural Analyzed frequency 6.5 Hz 0.058 5.8 Hz 8.5 Hz 0.053 7.3 Hz Junction of Aseismatic Escalator and Building 14.8 Hz 0.105 13.7 Hz When rigidly connecting an aseismatic escalator and a building, larger stress than estimated occurs at the highly rigid escalator truss. Thus, an aseismatic escalator must not be made to bear larger horizontal force than prescribed at the junction with a building. Furthermore, that junction should have structure that can follow relative displacement at earthquakes. In the light of those, we studied a structure for that junction and carried out elemental tests. 4.1 Required Performance of Junction Table 2 shows the horizontal force and displacement that can be loaded on the aseismatic escalator. Acceptable displacement in the table is specified based on the analysis results of the support beam design frame. 4.2 Loading Test of Junction 4.2.1 Width Direction Loading Test We put load cells in holes of the mounting beside the test model, and loaded those on the aseismatic escalator frame to measure reaction force in the width direction of that frame. We also applied a 70 kn vertical load that is equal to the weight of the aseismatic escalator itself, assuming that it is for an over-track station building, then we also loaded 30 kn and 0 kn vertical axial force for comparison. Table 3 shows loading results. Table 3 Width Direction Loading Results Axial force N (kn) First time Second time First time Second time First time Second time Slip load (kn) Average (kn) Even when vertically applying a 70 kn load that is equal to the weight of the aseismatic escalator itself (excluding jig load), assuming it is an over-track station building, reaction force in width direction was only 12.70 kn. That means sufficient margin is present 24

compared to the acceptable value of 36 kn in the escalator width direction shown in Table 2. We could also confirm that the escalator returned to the position before loading after removing that load in width direction thanks to four-degree V-shaped slope structure. 4.2.2 Junction Loading Test 4.2.2.1 Material Test In advance of the junction loading test, we carried out a material tensile test to check mechanical nature of the material used for that junction. Table 4 lists test results of low yield stress steel (LYP235), and Fig. 13 shows stress-strain curve of LYP235 that was calculated from that tensile test results. For calculation of yield strain, the index of this test, we used the data of Test Sample 3 that has a high yield point instead of the average of three test samples. Furthermore, we took values of the upper yield point because lower yield point was not clear. Yield strain of Test Sample 3 was defined as 1.033 from Fig. 13. flange; so, we quit testing. Fig. 15 shows test loading. In this test, yield load was the load whereby one of the strain measurement points (three-axis strain gauge) on the panel surface reached 1.033μ (the load when yield was determined on the von Mises yield condition formula). Vertical jack (equivalent to escalator s own weight) Sliding bearing (four-degree V-shaped slope) Load cell Building beam Escalator frame (a) Loading test in width direction Table 4 Tensile Test Results (LYP235) Vertical jack Work No. Purpose Order No. Received order No. R87F7B022 Test temperature 22 C Material LYP235 Spec No. Test item Spec Test sample No. Width Thickness (mm) Gauge length (mm) Mechanical nature Tensile test 0.2% bearing force (yield point) (N/mm 2) Tensile strength (N/mm 2) Stretch (%) Squeeze (%) Cut-off point Ultralow-carbon steel LYP235 Building beam Aseismatic escalator (b) Loading test in longitudinal direction LYP235 Tensile Test, Stress-Strain Fig. 14 Junction Plan for Element Test Stress (N/mm 2 ) Strain (µ) Fig. 13 Tensile Test, Stress-Strain (LYP235) 4.2.2.2 Test Plan and Overview\ We carried out a loading test by vertically placing a junction panel alone and applying load only on one side (compression side) in one direction using a vertical jack. Fig. 14 shows the actual junction plan for element test. We measured strain of the panel at the position shown in Fig. 14 (b). 4.2.2.3 Destruction (Loading) As for deformation and destruction of test samples, strain in Z direction (45 degree) at panel measurement point S13 reached yield strain. The load at that time was 222 kn, and the displacement was 3.23 mm (1δ). Then, when displacement exceeded around 25.81 mm (8δ), out-plane deformation occurred and shear deformation of the panel developed. When displacement reached 90.11 mm (28δ), cracking occurred at the welding of the lower Fig. 15 Loading on Junction Panel 4.2.2.4 Load-Displacement Relation Fig. 16 shows load-displacement relation at loading point. The yield point in Fig. 16 is defined in section 4.2.2.3. Fig. 17 shows shear strain at S1 - S13 and B1 measurement points. Looking at displacement increase tendency in load-displacement relation at loading point in Fig. 16, we can find nonlinearity from approx. 450 kn load. At the same time, in increase tendency for load-shear strain relation in Fig. 17, shear strain becomes predominant at around 450 kn to 500 kn at each measurement point. Those mean that increase tendencies for displacement and strain correspond to each other well. We can therefore presume that destruction by shear yield development of junction panel is predominant in destruction of test samples. 25

Special edition paper Load (kn) Load-Displacement Relation Figure at Loading Point Displacement at loading point Yield point Displacement (mm) Fig. 16 Load-Displacement Relation at Loading Point Load (kn) Load-shear strain relation Shear strain (µ) Load (kn) Load-shear strain relation displacement where story drift is 1/100 at 7 m story height), and Fig. 18 (c) the main strain distribution at the final deformation. In Fig. 18 (a), we can see that panel shear stress is predominant, and in Fig. 18 (b) and (c), we find that such tendency becomes more remarkable as load increases. Furthermore, since Fig. 18 (b) and (c) show that main strain plasticity in shear direction develops, we can confirm that ultralow-carbon steel panel absorbs energy (horizontal force). 4.3 Summary of Junction Loading Test The loading test in the width direction using model aseismatic escalator frame and simple loading test using test samples with low yield stress steel (LYP235) panel have given us the following information. (1) We confirmed that an aseismatic escalator can have sufficient recovery performance by adding a sliding bearing part to the junction between the escalator and building and making the ESC have a four-degree V-shaped slope structure. (2) We confirmed that using low yield stress steel panel attached to the junction between the aseismatic escalator and building could control load when larger horizontal force than that prescribed occurs. (3) The load-displacement and load-strain relation suggests that fracture morphology by junction panel shear yield development is predominant in fracture morphology of test samples. 5 Shear strain (µ) Fig. 17 Load-Shear Strain Relation 4.2.2.5 Main Strain Distribution of Junction Panel (Front) (Rear) Conclusion We have proposed a specification for aseismatic escalators that can withstand 682.5 kn maximum horizontal force. By using the escalator frame as an aseismatic member, we can omit braces and effectively improve aseismatic performance. That can also be applied to new structures. In the future, we are going to obtain general structural appraisal to fully apply and follow up on the results of this research in seismic reinforcement and barrier-free accessibility projects. * This study has been carried out as joint research and development with Hitachi, Ltd. (a) At yield load (b) At 70 mm displacement No plotting of main strain on the panel rear surface at (b) and (c) because gauges broke while loading. Reference 1) Act for Promotion of the Earthquake Proof Retrofit of Buildings, as revised on November 7, 2005, Law No. 120 of 2005 (c) At final deformation Fig. 18 Main Strain Distribution of Junction Panel 2) Guidelines for Over-track Building Aseismatic Diagnosis and Renovation, Railway Technology Research Institute, May 1998 3) Explanation of Escalator and Elevator Technical Standards Fig. 18 shows main strain distribution on the front of the junction panel. Fig. 18 (a) is the main strain distribution at the yield load defined in 4.2.2.3. Fig. 18 (b) is the status when the interval of the aseismatic escalator and the building beam reached 70 mm (equal to 26 (2002), Building Guidance Division, Housing Bureau, Ministry of Land, Infrastructure, Transport and Tourism; Edited by Japan Building Equipment and Elevator Center Foundation and Japan Elevator Association