EVALUATION OF WIND HAZARD OVER JEJU ISLAND

Similar documents
INTERFERENCE EFFECTS OF TWO BUILDINGS ON PEAK WIND PRESSURES

ValidatingWindProfileEquationsduringTropicalStormDebbyin2012

STRUCTURAL DESIGN FIGURE INTERNATIONAL BUILDING CODE 288aR

EFFECTS OF SIDEWALL OPENINGS ON THE WIND LOADS ON PIPE-FRAMED GREENHOUSES

External Pressure Coefficients on Saw-tooth and Mono-sloped Roofs

Effects of directionality on wind load and response predictions

LABORATORY EXPERIMENTS FOR WAVE RUN-UP ON THE TETRAPOD ARMOURED RUBBLE MOUND STRUCTURE WITH A STEEP FRONT SLOPE

SCREENING OF TOPOGRAPHIC FACTOR ON WIND SPEED ESTIMATION WITH NEURAL NETWORK ANALYSIS

Investigation on Atmospheric Boundary Layers: Field Monitoring and Wind Tunnel Simulation

A Study on the Distribution of the Peak Wind Pressure Coefficient for the Wind Resistant Design of Rooftop Hoardings in High-rise Buildings

Generation of an Annual Typical Daily Wind Speed for Heights Equal and Less than 10 meters for Urban Armidale NSW, Australia

Wind Regimes 1. 1 Wind Regimes

NUMERICAL SIMULATION OF STATIC INTERFERENCE EFFECTS FOR SINGLE BUILDINGS GROUP

PRESSURE FLUCTUATIONS ACTING ON A TAPERED TALL BUILDING

MEASUREMENTS ON THE SURFACE WIND PRESSURE CHARACTERISTICS OF TWO SQUARE BUILDINGS UNDER DIFFERENT WIND ATTACK ANGLES AND BUILDING GAPS

Post-mortem study on structural failure of a wind farm impacted by super typhoon Usagi

ABNORMALLY HIGH STORM WAVES OBSERVED ON THE EAST COAST OF KOREA

Critical Gust Pressures on Tall Building Frames-Review of Codal Provisions

SIMULATION OF THE FLOW FIELD CHARACTERISTICS OF TRANSIENT FLOW

6.28 PREDICTION OF FOG EPISODES AT THE AIRPORT OF MADRID- BARAJAS USING DIFFERENT MODELING APPROACHES

An Investigation of a Safety Level in Terms of. Excessive Acceleration in Rough Seas

A New Strategy for Harbor Planning and Design

WAVE LOAD ACTING ON HORIZONTAL PLATE DUE TO BORE

Yasuyuki Hirose 1. Abstract

PROPAGATION OF LONG-PERIOD WAVES INTO AN ESTUARY THROUGH A NARROW INLET

Evaluating the Design Safety of Highway Structural Supports

Flow modelling hills complex terrain and other issues

THREE DIMENSIONAL STRUCTURES OF FLOW BEHIND A

MODELING OF CLIMATE CHANGE IMPACTS ON COASTAL STRUCTURES - CONTRIBUTION TO THEIR RE-DESIGN

Keywords: Wind Averaging Conversion, WMO guidelines, Gust Factor, Statistical Approach.

A New Generator for Tsunami Wave Generation

Effect of channel slope on flow characteristics of undular hydraulic jumps

Effect of Wind Induced on Road Accident along East Coast Expressway (ECE)

COMPARISONS OF COMPUTATIONAL FLUID DYNAMICS AND

Wind tunnel test and numerical simulation of wind pressure on a high-rise building

Topographic Wind Speed-up and Directionality Factors for Use in the City and County of Honolulu Building Code

WIND TUNNEL TEST ON THE FLOW AND DISPERSION OF AIRBORNE POLLUTANTS IN THE COMPLEX TERRAIN OF COASTAL REGION OF SHIEHE POWER PLANT OF TAIWAN

Wind Tunnel Study on the Structural Stability of a Container Crane According to the Boom Shape

Are Advanced Wind Flow Models More Accurate? A Test of Four Models

ESTIMATION OF THE DESIGN WIND SPEED BASED ON

DAMAGE TO OIL STORAGE TANKS DUE TO TSUNAMI OF THE MW OFF THE PACIFIC COAST OF TOHOKU, JAPAN

LABORATORY EXPERIMENTS ON WAVE OVERTOPPING OVER SMOOTH AND STEPPED GENTLE SLOPE SEAWALLS

Aspects of Using CFD for Wind Comfort Modeling Around Tall Buildings

Chapter 20. Planning Accelerated Life Tests. William Q. Meeker and Luis A. Escobar Iowa State University and Louisiana State University

International Journal of Advanced Engineering Technology E-ISSN

Regional Analysis of Extremal Wave Height Variability Oregon Coast, USA. Heidi P. Moritz and Hans R. Moritz

Numerical Analysis of Wind loads on Tapered Shape Tall Buildings

AERODYNAMIC FEATURES AS AUXILIARY ARCHITECTURE

Impact of New ANSI/TIA-222-H Standard on Broadcast NAB * ERI Breakfast * Apr 11, 2018 James Ruedlinger, P.E

Super-parameterization of boundary layer roll vortices in tropical cyclone models

ESCI 343 Atmospheric Dynamics II Lesson 10 - Topographic Waves

Forest Winds in Complex Terrain

Micro-zoned Design Maps of Topographic Wind Effects and Exposure in the State of Hawaii Building Code

ISOLATION OF NON-HYDROSTATIC REGIONS WITHIN A BASIN

UNIVERSITY OF HONG KONG LIBRARY. Hong Kong Collection

&)' VWXG\ DQG ZLQG IORZ PRGHOLQJ RYHU GLIIHUHQW WHUUDLQ W\SHV

Vertical Wind Velocity Distribution in Typical Hilly Terrain

Nearshore Wind-Wave Forecasting at the Oregon Coast. Gabriel García, H. Tuba Özkan-Haller, Peter Ruggiero November 16, 2011

Examples of Carter Corrected DBDB-V Applied to Acoustic Propagation Modeling

Journal of Emerging Trends in Computing and Information Sciences

How an extreme wind atlas is made

Tension Cracks. Topics Covered. Tension crack boundaries Tension crack depth Query slice data Thrust line Sensitivity analysis.

EXPERIMENTAL STUDY ON THE HYDRODYNAMIC BEHAVIORS OF TWO CONCENTRIC CYLINDERS

Determination of the Design Load for Structural Safety Assessment against Gas Explosion in Offshore Topside

THE EFFECT OF THE OCEAN EDDY ON TROPICAL CYCLONE INTENSITY

Wave Setup at River and Inlet Entrances Due to an Extreme Event

START UP MODELING OF KAIST MICRO MODULAR REACTOR COMPRESSOR USING BETA LINE METHOD WITH GAMMA+ CODE

WIND FORCES ACTING ON INFLATABLE AMUSEMENT PRODUCTS AND CRITICAL WIND SPEEDS CAUSING ACCIDENTS

2016 NC Coastal Local Governments Annual Meeting

Figure 1 Lake Ontario Offshore Study Area near East Toronto

Large-eddy simulation study of effects of clearing in forest on wind turbines

WIND CONDITIONS MODELING FOR SMALL WIND TURBINES

Windcube FCR measurements

Technical Note AN EMPIRICAL. METHOD FOR DESIGN OF BREAKWATERS AS SHORE PROTECTION STRUCTURES

DEVELOPMENT OF SAFE VERTICAL AXIS WIND TURBINE

Extreme typhoon wind speeds considering the random variation in a full-scale observation

Quantification of the Effects of Turbulence in Wind on the Flutter Stability of Suspension Bridges

Aalborg Universitet. Estimation of wave conditions at Liseleje location Bogarino, Bruno; Brorsen, Michael. Publication date: 2007

Building Planning PART. Chapter 3. Chapter 3. Building Planning. Climatic and Geographic Design Criteria C

Wind Blow-out Hollow Generated in Fukiage Dune Field, Kagoshima Prefecture, Japan

EVALUATION OF TSUNAMI FLUID FORCE ACTING ON THE BRIDGE DECK

Atmospheric Forces and Force Balances METR Introduction

19.1 Problem: Maximum Discharge

SPECTRAL CHARACTERISTICS OF FLUCTUATING WIND LOADS ON A SEPARATE TWIN-BOX DECK WITH CENTRAL SLOT

Effects of Geometry on Speed Flow Relationships for Two Lane Single Carriageway Roads Othman CHE PUAN 1,* and Nur Syahriza MUHAMAD NOR 2

Aspects of Using CFD for Wind Comfort Modeling Around Tall Buildings Rasmussen, Michael Robdrup; Andersen, Lars Vabbersgaard

Experimental Investigation on Changes of Water Surface Profile with Gaussian Shaped Bottom and Side Roughness

MECHANISM AND COUNTERMEASURES OF WAVE OVERTOPPING FOR LONG-PERIOD SWELL IN COMPLEX BATHYMETRY. Hiroaki Kashima 1 and Katsuya Hirayama 1

WINDA-GALES wind damage probability planning tool

Observed Roughness Lengths for Momentum and Temperature on a Melting Glacier Surface

CVEN Computer Applications in Engineering and Construction. Programming Assignment #4 Analysis of Wave Data Using Root-Finding Methods

A Wind-Tunnel Study of a Cubic Rooftop AC Unit on a Low Building

Failure Data Analysis for Aircraft Maintenance Planning

A Study on Weekend Travel Patterns by Individual Characteristics in the Seoul Metropolitan Area

Tidal regime along Vietnam coast under impacts of sea level rise

August 1990 H. Kondo 435. A Numerical Experiment on the Interaction between Sea Breeze and

+ R. gr T. This equation is solved by the quadratic formula, the solution, as shown in the Holton text notes given as part of the class lecture notes:

Proceedings of the 7 th International Conference on HydroScience and Engineering Philadelphia, USA September 10-13, 2006 (ICHE 2006) ISBN:

Investigation of Vertical Wind Shear Characteristics Using 50m Meteorological Tower Data

Comparisons of Discretionary Lane Changing Behavior

Transcription:

The Seventh Asia-Pacific Conference on Wind Engineering, November 8-12, 2009, Taipei, Taiwan EVALUATION OF WIND HAZARD OVER JEJU ISLAND Young-Kyu Lee 1, Sungsu Lee 2 and Hak-Sun Kim 3 1 Ph.D Candidate, Structural Systems & CAE, Chungbuk National University 410 Seongbong-ro, Heungduk-gu, Cheongju, Republic of Korea, youngkyulee@cbnu.ac.kr 2 Professor, Schoool of Civil Engineering, Chungbuk National University 410 Seongbong-ro, Heungduk-gu, Cheongju, Republic of Korea, joshua@cbnu.ac.kr 3 Ph.D Candidate, Structural Systems & CAE, Chungbuk National University 410 Seongbong-ro, Heungduk-gu, Cheongju, Republic of Korea, haksun@cbnu.ac.kr ABSTRACT In the study the evaluation of wind hazard overall Jeju island, South Korea, is performed with a technique of the typhoon Monte Carlo simulation. Especially, the surface roughness model and the topographical effect model are used to consider the regional wind characteristics. The surface roughness model is developed by using the land cover map and the topographical effect model, the DEM (digital elevation model) and Korean Building Code- Structural. KEYWORDS: WIND HAZARD, SURFACE ROUGHNESS MODEL, TOPOGRAPHICAL EFFECT MODEL 1. Introduction Jeju island, South Korea, is located at the south point and experiences typhoons almost every year. A statistical extreme value analysis is not proper to estimate return period winds for the typhoon-prone regions such as Jeju. In these areas the typhoon Monte Carlo simulation is an alternative to the wind hazard assessment (Simiu and Scanlan, 1996). Surface roughness takes a roll to retard a wind speed near surface and determines the vertical wind profile in the boundary layer. In a channel flow a flow accelerates when the cross-section reduces. Similarly in the atmospheric boundary layer winds have a speed-up effect when a flow comes along with topology such as hills, ridges, or escarpments. In the study we develop a surface roughness model and a topographical effect model to represent these effects prescribed previously and evaluates the wind hazard with regional wind characteristics. Bietry et al. (1978) investigates roughness lengths for suburbs and centers of cities. Oliver (1971) examines the wind profiles for a forest canopy. These results are used to make the surface roughness model. Korean Building Code-Structural specifies the topographic effects by hills, ridges, and escarpments. The code and a DEM are applied to the topographical effect model. The use of mathematical simulation methods to estimate hurricane wind speeds was first implemented by Russell (1971, 1974) for the Texas coast. Others have used this approach to estimate extreme winds or to evaluate effects induced by tropical cyclones (Batts et al., 1980; Vickery and Twisdale, 1995a, 1995b). In chapter 2 the homogeneous wind-map model is explained, which is based on a typhoon Monte Carlo simulation. The surface roughness and the topographic effect models are introduced in chapter 3 and 4 respectively. Chapter 5 shows the wind hazard map for Jeju.

2. Homogeneous Wind-map Model A homogeneous wind-map model (HWM) is developed by the typhoon Monte Carlo simulation. The HWM is defined as a wind-map of the 100-year return period 10-minute averaged wind speed at 10m above ground on the homogeneous surface condition with no topographic features, on which a roughness length, z 0, equals to 0.07m. The climatological characteristics of the typhoons are estimated from the RSMC (Regional Specialized Meteorological Center) best tracks from 1951 to 2007. The typhoon Monte Carlo simulation is performed at Jeju, Seongsan, Seoguipo, and Gosan having meteorological stations. The sampled typhoons having approached within 250km into the sites are used to estimate the distributions of an annual occurrence rates, the central pressure depths (depict between peripheral and central pressures), the translation speeds, the nearest distances, and the headings. The radius of maximum winds is assumed to be correlated with the central pressure depth by Fujii s equation (1998). Table 1 shows the distributions of the climatological characteristics to the typhoons. Table 1: Climatological characteristics of the typhoons hitting Jeju Central pressure depths ( p Δ ) Nearest distances ( d min ) Translation speeds ( s ) Headings (θ ) Radii of max. winds ( R max ) Occurrence rate Weibull distribution b Δp Y = F( Δp a, b) = 1 exp, min( ΔPi ) Δp max( ΔPi ) a Uniform distribution Y = F( dmin a, b) = ( dmin a) /( b a), b > a Gamma distribution 1 s (, ) b 1 t Y = F s a b = t exp dt, min( Si) s max( Si) a b Γ( a) 0 b Extreme value distribution θ μ Y = F( θ μ, σ ) = 1 exp exp, min( Θi) θ max( Θi) σ Fujii s experimental formula (Fujii, 1998) R = 66.19logΔp 335.18 (km) max + Poisson process The SPH (Standard Project Hurricane, 1972) wind field model and the Fujii s filling rate describing for central pressures to increase on the land are adopted into the typhoon Monte Carlo simulation. The typhoons are assumed to move with a constant speed and heading. 5,000 of typhoons are generated by the typhoon Monte Carlo simulation. The 100- year return period 10-min wind speeds on the homogeneous surface having 0.07m of the roughness length, z 0 are estimated to 27.0m/s, 27.7m/s, 27.9m/s and 27.5m/s at Jeju, Gosan, Seongsan, and Seoguipo respectively. The HWM overall Jeju island is developed by a inverse distance interpolation with the speeds of 4 sites (see Figure 1).

Figure 1: Homogeneous wind-map model for Jeju island. 3. Surface Roughness Model Surface roughness elements retard wind speeds and determine the vertical wind profile. Since surface roughness surroundings are not homogeneous all directions upwind, the surface roughness model should have directionality. The 8-directional SRM (Surface Roughness Model) is developed to consider the effects of the upwind surface roughness by manipulating the land cover map (LCM). The LCM categories are weighted to generate the SRM. The used LCM has 8 of categories such as water, built-up region, bare ground, swampy land, grassland, forest, rice field, and dry field. Each category has the weighting values shown in Table 2. Table 2: Weighting values for LCM categories LCM categories Weighting values Water 0 Built-up region 15 Bare ground 0.5 Swampy land 2 Grassland 1 Forest 15 Rice field 1 Dry field 1 In the study to estimate wind hazards 10m above ground we calculate an arithmetic mean over 1/8 circle fetch with 1000m upwind, which Korean Building Code-Structural recommends corresponding to 100 times of height. The arithmetic mean and the conditions on Table 3 generate the 8-directional SRMs which have 3 of surface roughness categories such

as 0.3m, 0.07m, and 0.005m of roughness lengths (Z0). Bietry et al. (1978) presents 20~40cm of roughness length for sparsely built-up suburbs. The zones on which the built-up region and the forest occupy over half are judged as 0.3m roughness length and correspond to over 8.5 of arithmetic mean. Oliver (1971) suggests 4~10cm of roughness length for high grass. We judge the zones on which the arithmetic mean exists between 1 and 8.5 as 0.07m of roughness length. The other zones are assigned to 0.005m of roughness length. Figure 2 shows the SRM for north upwind overall Jeju island. North coast has short roughness length while south has tall roughness length. The central region almost consists of forest so that 0.3m of roughness length is assigned. Table 3: Surface roughness categories corresponding to arithmetic mean Category conditions Surface roughness categories Arithmetic mean >= 8.5 Z0 = 0.3m 1 <= Arithmetic mean < 8.5 Z0 = 0.07m Arithmetic mean < 1.0 Z0 = 0.005m Figure 2: Surface roughness model for north upwind 4. Topographical Effect Model As shown in Figure 3, the wind speed accelerates when the winds flow along with topographic features such as hills or ridges. The TEM (Topographical Effect Model) is developed to represent the speed-up effects induced by topology. The TEM is developed for 8-direction to consider none-homogeneous topology to the fetch upwind. The 30m-resolution DEM and Korean Building Code-Structural are used in the process of the development. Bringing the elevation profile corresponding to the upwind direction from the DEM, we find

the parameters which substitute to Table 4 to calculate the topographic factor defined in Korean Building Code-Structural. In Table 4 the slope, φ is defined as φ = H /( 2Lh ) (1) where H is a height of hill or escarpment relative to the upwind terrain, Lh, a distance upwind of crest to where the difference in ground elevation is half the height of hill or escarpment. In Table 4 the values of topographic factor are given for some slopes, φ. For other than those shown, linear interpolation is permitted. Figure 4 shows the TEM for north upwind overall Jeju island. Jeju has many small hills called Oreum where the speed-up induced by topology exists. Halla mountain is located at the center, of which top has 1,950m of height, experiencing the speed-up. Table 4: Topographic factor for slopes φ Topographic factor =0.05 1.05 =0.10 1.09 =0.20 1.18 0.30 1.27 Figure 3: Speed-up description on hill, ridge, and escarpment.

Figure 4: Topographical effect model for north upwind. 5. Evaluation of Wind Hazard over Jeju island Figure 5 illustrates the process for wind hazard map generation. The SRM, TEM, and HWM are assumed to be independent. It makes 8 combination wind maps by raster-based upwind-wise operation. The wind hazard map (WHM) is a set of maximums among all combinations at each raster. The process of wind conversion into the other surface roughness categories uses the similarity model for the log-law profile (Simiu and Scanlan, 1996). Figure 6 shows the wind hazard map based on 100-year return period 10-min wind speed without considering wind directions. As shown in Figure 6 coast SRM TEM HWM Raster-based upwind-wise combination operation Wind Hazard Map =Set of maximums among all combinations at each raster Figure 5: Process of wind hazard map generation.

Figure 6 Wind hazard map for Jeju island. 6. Conclusions We performed the evaluation of wind hazard considering the local wind characteristics for Jeju island. The HWM developed by the typhoon Monte Carlo simulation, the SRM describing the surface roughness effect, and the TEM representing the speed-up effects are used in the process. According to the result it estimates the coastal areas to be more vulnerable and shows that urban and forest region is safe relatively. Acknowledgment This work was supported by the grant from Natural Hazard Mitigation Research Group funded by National Emergency Management Agency, South Korea. References Simiu, E and Scanlan, R. H. (1996), Wind Effects on Structures, 3 rd Edition, John Wiley & Sons, New York, NY, USA. Revised Standard Project Hurricane Criteria for the Atlantic and Gulf Coasts of the United States, Memorandum HUR7-120, U.S. Dept. of Commerce, NOAA, June 1972. Fujii, T. (1998), Statistical Analysis of the Characteristics of Severe Typhoons Hitting the Japanese Main Islands, Monthly Weather Review, Vol. 126, pp. 1091-1097. Bietry, J., Sacre, C., and Simiu, E. (1978), Mean Wind Profiles and Changes of Terrain Roughness, Journal of Structural Division, ASCE, Vol. 104, pp. 1585-1593. Oliver, H.R. (1971), Wind Profiles in and above a Forest Canopy, The Quaterly Journal of the Royal Meteorological Society, Vol. 97, pp. 548-553. Architectural Institute of Korea (2005), Korean Building Code-Structual, AIK, Seoul, South Korea

Russell, L.R. (1971), Probability Distributions for Texas Gulf Hurricane Effects, Journal of Waterways, Harbors, and Coastal Engineering Division, Proceedings of the American Society of Civil Engineers, No. 1, pp. 139-154. Russell, L.R., and Schueller, G.F. (1974), Probabilistic Models for Texas Gulf Coast Hurricane Occurrences, Journal Petroleum Technology, pp. 279-288. Batts, M.E., Cordes, M.R., Russell, C.R. and Simiu, E. (1980), Hurricane Wind Speeds in the United States, Naional Bureau of Standards Report Number BSS-124, U.S. Dept. of Commerce, Washington, DC. USA. Vickery, P.J. and Twisdale, L.A. (1995a), Wind-Field and Filling Models for Hurricane Wind-speed Predictions, Journal of Structural Engineering, Vol. 121, No. 11, pp. 1700-1709. Vickery, P.J. and Twisdale, L.A. (1995b), Prediction of Hurricane Wind Speeds in the United States, Journal of Structural Engineering, Vol. 121, No. 11, pp. 1691-1699.