Extreme Wind Speeds in the Kingdom of - Semantic Scholar · Extreme Wind Speeds in the Kingdom of...
Transcript of Extreme Wind Speeds in the Kingdom of - Semantic Scholar · Extreme Wind Speeds in the Kingdom of...
Extreme Wind Speeds in the Kingdom of
Saudi Arabia
by
A. M. Arafah1, G. H. Siddiqi2 and A. Dakheelallah3
ABSTRACT
Extreme value analysis of wind data in the Kingdom of
Saudi Arabia is described. Probabilistic models of wind
behavior at twenty stations are generated which yield the
basic design wind speeds for a given recurrence interval
in fastest mile units. The models are verified by the Chi-
square and Kolmogorov-Smirnov goodness-of-fit tests at 5
percent significance level. Basic design wind speeds are
calculated at each station and an isotach map of design
speeds for a 50 year mean reccurrence interval is
presented. The information obtained allows evaluation of
design wind loads by the ANSI A58.1 procedure.
___________________
1Asistant Professor, Department of Civil Engineering, College of Engineering, Riyadh, Saudi Arabia.
2Associate Professor, Department of Civil Engineering, College of Engineering, Riyadh, Saudi Arabia.
3Postgraduate Student, Department of Civil Engineering, College of Engineering, Riyadh, Saudi Arabia.
INTRODUCTION
Wind loads, among the other design loads, are crucial
for the design of structures such as tall buildings,
towers, radar and communication antennas. This paper
considers the reliability and homogeneity aspects of the
wind data and studies the distribution of extreme annual
wind speeds over the Kingdom of Saudi Arabia to obtain a
rational basis for the evaluation of wind induced loads
according to American National Standards Institute's Code
for design loads, ANSI A58.1-19821.
RELIABILITY AND HOMOGENEITY OF DATA
In order for the wind speed data to provide useful
information it must be reliable and form a homogeneous
set.
Measured data are considered reliable if the
recording instruments are adequately calibrated and are
not exposed to local effects due to proximity of
obstructions. However, if at any time in future the
calibration is found to be inadequate, it is possible to
evaluate the corrections and adjust the data.
Measured data form a homogeneous set when they are
obtained under identical conditions of averaging time,
height above ground and roughness of the surrounding
terrain.
Averaging Time
The data averaged over short intervals, like highest
gust, 5 second average etc., in certain cases, can be
affected by stronger than usual local turbulence, which
results in distorted picture of the mean winds. Averaging
over longer periods like 5 or 10 minutes is, therefore,
desirable.
Anemometer Height above Ground
Height of 10 m above gorund is considered to be the
standard instrument height. Wind data measured at any
other height are adjusted to the standard height by power
law2 . The values of exponent in the power law for
different "exposures" are available in literature2.
Specifically for meteorological stations, which are
invariably located in open country, the exponent is one-
seventh.
Roughness of Surrounding Terrain
The measured data are affected by the roughness of
the surrounding terrain. In case the roughness around an
anemometer changes significantly during the period of
record under consideration, it is possible to adjust the
measured record to a common terrain roughness by using
similarity model9.
DESIGN WIND FORCES
Basic Design Wind Speed
Basic design wind (BDW) speed is defined as the
maximum expected annual wind speed at the standard height
of 10 meters above ground in open country over a chosen
recurrence interval. This speed is established by extreme
value analysis of the instrumental data of maximum annual
wind collected from meteorological stations over a
geographical region.
American National Standards Institute's code for
design loads, ANSI A58.1-19821, employs fastest mile wind
(FMW) speed as the BDW speed. FMW speed is the maximum
annual wind speed at which a one mile long column of wind
passes by an anemometer.
Isotach Map
An individual extreme value model for a station
predicts the BDW speeds at various recurrence intervals at
the station. The speeds at a network of stations form the
three dimensional input data to a contouring software
which plots isotachs (lines of equal wind speed) over the
geographic region. BDW speed at a chosen location can be
interpolated from this map.
Wind Induced Forces
Most codes translate the BDW speed to an equivalent
static wind load intensity which varies over the height of
a given structure. This procedure accounts for type of
"terrain exposure" facing the structure, shape and form of
the structure, and its "importance" and other related
factors.
DATA PROCESSING
The data comprising of the largest annual wind speeds
available with the Meteorological and Environmental
Protection Agency (MEPA) include records varying over
periods of three to thirty three years measured at twenty
eight stations well distributed over the Kingdom. Twenty
of these stations have records over a continuous duration
of fifteen or more years which is desirable for the
probabilistic analysis involved here. These stations
along with the anemometer heights and duration of their
record are listed in Table 1 and considered in this study.
It is presumed that the anemometers at all the
weather stations in the Kingdom are situated in open
country environments throughout their period of commission
and that they are well maintained and adequately
calibrated. However, if at any time in future, it is
determined that the calibration was not adequate, height
of instrument or the
Table 1. Profile of Wind Monitoring Stations in the Kingdom
-------------------------------------------------------- Station Station Anemometer Years of No. Name Height (m) Continuous Records -------------------------------------------------------- 1 Badanah 6 19 2 Bisha 6 20 3 Dhahram 10 26 4 Gassim 7 23 5 Gizan 8 22 6 Hail 8 26 7 Jeddah 10 19 8 Jouf 7 19 9 Kamis Mushit 9 23 10 Madina 10 26 11 Najran 8 15 12 Hafer-Albatian 8 19 13 Riyadh 10 26 14 Rafah 12 18 15 Sulayel 10 20 16 Tabouk 9 26 17 Taif 8 26 18 Turaif 8 17 19 Wajeh 10 26 20 Yanbu 10 23 21 AL-Ehsa 10 4 22 Abha 10 8 23 Baha 10 6 24 Gurayat 10 5 25 Jeddah (KAIA) 10 7 26 Mekkah 10 9 27 Riyadh(KKIA) 10 5 28 Sharurah 10 5 ------------------------------------------------------
terrain roughness did change, the corrections can be
evaluated and the data adjusted accordingly.
The measured annual wind speeds at all the stations
are averaged over ten-minute duration. The ten-minute
speed in knots is converted to ten-minute speed in miles
per hour. The averaging time for conversion of this speed
to FMW speed is obtained by an iterative procedure, and is
used to derive the desired fastest mile2. This speed, in
case of non-standard instrumental heights, is then reduced
to the standard height by power law.
EXTREME VALUE ANALYSIS
Extreme Value Distributions
The theory of extreme values has been successfully
used in civil engineering applications. Floods, winds,
and floor loadings are all variables whose largest value
in a sequence may be critical to a civil engineering
system3. In case of well behaved climates (i.e. ones in
which infrequent strong winds are not expected to occur)
it is reasonable to assume that each of the data in a
series of the largest annual wind speeds contributes to
the probabilistic behavior of the extreme winds.
The design wind speed can be defined in probabilistic
terms, where the largest wind speed in a year is
considered as a random variable with its cumulative
density function characterizing its probabilistic
behavior.
A commonly used distribution in extreme value
analysis is the double exponential distribution in which
an annual wind speed record, Xi, is considered to be a
random variable in the i-th year. For n successive years,
variables Xi are assumed to be mutually independent and to
have identical distributions. Supposing that random
variables Xi are unlimited in the positive direction and
that the upper tail of their distribution falls in an
exponential manner then variable V, the largest of n
independent variables Xi, has Type I (Gumbel) extreme
distribution, FV (υ) , as follows,
FV (υ) = exp [ - exp ( - خطأ! ) ] , (1)
where α and u are the scale and location parameters and estimated from the observed data at each station. The
distribution function FV(υ) is the probability of not
exceeding the wind speed υ.
The Type II (Frechet) extreme-value distribution also
arises as the limiting distribution of the largest value
of many independent identically distributed random
variables. In this case each of the underlying variables
has a distribution which, on the left, is limited to zero.
The Type II distribution function, FV (υ) , is,
FV (υ) = exp [ - ( خطأ! )خطأ! ] , (2)
where the parameters ω and γ are estimated from the
observed data at each station. The parameter, γ , is known
as the tail length parameter3.
Based on the method of order statistics developed by
Lieblein13, the values of cumulative density function,
FV(υ), corresponding to a series of extreme annual wind
speeds, can be estimated as follows,
FV(υ) = (3) !خطأ
where n is the number of years of record and m(υ) is rank
of the event, υ, in the ascending order of the magnitudes.
The inverse function of FV(υ) is known as the
percentage point function (PPF) which gives the value of
wind speed υ at a sellected value of FV(υ). For Type I
(Gumbel) extreme distribution the PPF is,
υ(F) = u + α y(F) (4)
which is a linear relation between υ(F) and the
intermediate variate y(F) which is given by,
y(F) = - ln(- ln F) (5)
Relation between the Two Distributions
The Type II distribution with small values of tail
length parameter results in higher estimates of the
extreme wind speeds than the Type I distribution. It can
be shown that for values of parameter γ equal to 15 or more the two distributions, Type I and II , are almost
identical4. It can also be shown that if V has Type II
distribution then Z = ln V has the Type I distribution
with parameters u = ln ω and α = ( 1/γ ). This relationship affords use of Type I probability paper for Type II
distribution also3.
Errors in Prediction of Wind Speeds
Errors are inherent in the process of wind speed
prediction. Besides the errors associated with the
quality of the data, there are sampling and modeling
errors.
The sampling errors are a consequence of the limited
size of samples from which the distribution parameters are
estimated. These errors, in theory, vanish as the size of
the sample increases indefinitely9. A sample size of 15 or
more, at a station, employed in this study is adequate in
this regard.
The modeling errors are due to inadequate choice of
the probabilistic model. Chi-square and K-S Test are
performed to choose the best fitting model.
Probabilistic Wind Models in Use
One major question that arises in the wind speed
extreme value analysis is the type of probability
distribution best suited for modeling the behaviour of the
extreme winds. Thom5 studied the annual extreme wind data
for 141 open country stations in the United States. The
Type II distribution was chosen to fit the annual extreme
wind series giving isotach maps for 2, 50 and 100-year
mean recurrence intervals.
Thom6 also developed new distributions of extreme
winds in the United States for 138 stations. New maps were
drawn for 2-year, 10-year, 25-year, 50-year and 100-year
mean recurrence intervals. In his study, Thom used the
Type II (Frechet) distribution. He indicated that
examination of extensive non-extreme wind data indicated
that such data follow a log-normal distribution quite
closely, which reinforces the choice of the Type II
distribution.
Simiu7 presented a study in which a 37 year-series of
five- minute largest yearly speeds measured at stations
with well-behaved climates were subjected to the
probability plot correlation coefficient test to determine
the tail length parameter of the best fitting distribution
of the largest values. Of these series, 72% were best
modeled by Type I distribution or equivalently by the Type
II distribution with γ=13; 11% by the Type II distribution with 7<γ<13; and 17% by the Type II distributions with
2<γ<7. Simiu8 obtained the same percentages from the
analysis of 37 data sets generated by Monte Carlo
simulation from a population with a Type I distribution
which indicates that in well-behaved climates extreme wind
speeds are well modeled by Type I rather than Type II
distributions.
Simiu4 showed that the Type I distribution of the
largest values is an adequate representation of extreme
wind behaviour in most regions not subjected to hurricane-
force winds. Simiu9 indicated that for hurricane-prone
regions the Type II distribution with a small value of the
tail length parameter may give better estimation of
extreme wind speeds.
The ANSI #A58.1-821 wind load provision is based on a
wind speed contour map developed by Simiu10. The wind
speeds in the map were established from the data collected
at 129 meteorological stations in the contiguous United
States. The Type I (Gumbel) distribution is used in the
analysis. Simiu used data only for locations for which a
minimum of 10 years of continuous records were available11.
The provisions of National Building Code of Canada12
are also based upon the assumption that extreme wind speed
is best modeled by the Type I distribution.
STEPS OF EXTREME VALUE ANALYSIS
The determination of appropriate distribution type
involves the following steps,
1) the annual extreme wind speeds records at each
station are first corrected for the standard
anemometer height, terrain exposure, and the
averaging time,
2) the data, for each station, are then arranged in an
ascending order. The corresponding values of the
CDF are calculated from Eq.3 ,
3) the intermediate parameter, y, is calculated using
Eq. 5,
4) linear regression analysis is performed between
values of υ and the corresponding values of y, to estimate values of parametrs u and α in Eq. 4. such an analysis for Madian is shown in Fig. 1 as a
sample,
5) the Chi-Square ,χ 2, test with 95 percent confidence level is performed for model verification,
6) steps 4 and 5 are repeated using ln (V) in place of
V,
7) based on the distribution of the data on the
modified extreme Type I probability paper and on
the minimum value of χ 2 , the more appropriate
model for the wind speed data is selected, and
8) in case of the Type II distribution, the parameters
ω = eu and γ = (1/α) are also calculated.
RESULTS OF EXTREME VALUE ANALYSIS
The extreme value analysis is performed on the wind
speed data of the 20 stations which have fifteen or more
years of continuous record. The extreme distribution models
obtained are presented in Table 2. As seen in the table, at
fifteen stations wind speed data are best modeled by the
Type I distribution and the remaining five stations they
follow the Type II distribution.
As a specific example of analysis, Fig. 1. presents the
fastest mile annual extreme wind speed data for Madina
Station ploted on the Extreme Type I propability paper.
The appropraite model is found to be,
V = 45.34 + 9.75 y
Table 2 Extreme Value Models of Fastest Mile Speed in Mile per Hour at 20 Stations in the Kingdom of Saudi Arabia
----------------------------------------------
Station Type u (ω) α (γ)
(1) (2) (2)
----------------------------------------------
Badana I 59.54 11.37
Bisha I 51.16 8.73
Dhahran I 45.95 4.90
Gassim I 63.19 11.59
Gizan I 53.48 11.59
Hail II 53.52 7.99
Jeddah I 48.59 6.44
Jouf I 56.88 7.09
Khamis-Mushiat I 42.05 7.58
Madina I 45.34 9.87
Najran II 47.94 8.03
Hafer-Albatin I 57.46 6.66
Riyadh II 51.98 7.57
Rafah I 55.26 7.27
Sulayel II 51.22 6.55
Tabuk II 54.54 8.05
Taif I 51.36 8.68
Turaif I 56.53 8.19
Wajh I 47.17 8.21
Yanbu I 46.58 6.68
---------------------------------------------- (1) Extreme value distribution type. (2) In case of the Type II distribution, the values
listed belong to the parameters within the parentheses in the column heading.
which means,
FV(υ) = exp [ - exp ( - ( خطأ! ) ) ]
On the other hand, in Riyadh, the fastest mile annual
extreme wind speeds were found to be best modeled by
extreme Type II given by,
Fv(υ) = exp [ - ( خطأ! )خطأ! ]
MODEL VERIFICATION
The models obtained are checked by the Chi-square and
Kolmogorov-Smirnov (K-S) goodness-of-fit tests at 5 percent
significance level. The calculated values of the statistic
D1 for the Chi-Square and D2 for Kolmogrov-Smirnov
goodness-of-fit tests are listed in Table 3 along with the
corresponding critical values, D1c and D2c , at 5 percent
significance level. The results indicate that the
calculated values of D1 are below the critical values at
sixteen stations. At the remaining four stations, Dhahran,
Jouf, Hafer Al-batin and Yanbu, they however, exceed the
critical limits. Such a result, when several events are
clustered in one wind speed interval, is expected in Chi-
square analysis. On the other hand, the calculated values
of statistic D2 are less than the critical values at all
the stations which indicates that the models are acceptable
at 95 percent confidence level.
Table 3 Calculated and Critical Values of Statistics D1
and D2 at 5 percent Significance Level.
------------------------------------------------------------- Chi-Square Test Kolmogorov-Smirnov Test ---------------------------------------------- Station D D D D 1 1c 2 2c-------------------------------------------------------------
Badana 2.087 11.07 0.0835 0.300
Bisha 1.493 11.07 0.0791 0.290
Dhahran 19.110 11.07 0.1541 0.256
Gassim 4.163 11.07 0.0748 0.272
Gizan 5.247 11.07 0.1414 0.278
Hail 5.903 11.07 0.1177 0.256
Jeddah 3.169 11.07 0.1569 0.300
Jouf 16.558 11.07 0.1368 0.300
Khamis-Mushiat 9.310 11.07 0.0929 0.272
Madina 3.661 11.07 0.1529 0.256
Najran 7.949 11.07 0.1625 0.340
Hafer-Albatin 22.741 11.07 0.1346 0.300
Riyadh 10.215 11.07 0.2198 0.256
Rafah 9.255 11.07 0.1463 0.310
Sulayel 7.234 11.07 0.1074 0.290
Tabuk 10.376 11.07 0.1054 0.256
Taif 5.345 11.07 0.1122 0.256
Turaif 4.313 11.07 0.1136 0.320
Wajh 4.547 11.07 0.1377 0.256
Yanbu 17.608 11.07 0.1228 0.272
-------------------------------------------------------------
EXTRAPOLATION OF WIND SPEED MODELS
At any station, the extreme wind speed at a particular
annual probability of exceedance, Pa, can be calculated
using the corresponding wind speed model. The mean
recurrence interval or return period, N, is defined as
N = (6) !خطأ
If a structure has a life span of n years, then for a
specific wind with a return period of N years, the
percentage risk, which expresses the probability that this
design wind is exceeded at least once during the lifetime
of the structure, is given by
Pr = 1 - [ 1 - Pa ]
n = 1 - [ 1- خطأ! ](7) !خطأ
If the return period is taken to be the same as the
lifetime of the structure, there is always a risk of
63% that this speed is exceeded at least once during the
lifetime of the structure.
The mean recurrence interval or the return period for
specified accepted risk percentage and design service
lifetime of the structrue is given as,
N = (8) !خطأ
ANSI A58.1-821 specifies that a basic design wind speed
corresponding to a 50-year mean recurrence interval should
be used in designing all permanent structures. However,
the structures with an unusually high degree of hazard to
life and property in the case of failure, are to be
designed for a 100-year mean recurrence interval while the
structures having no human occupants or where there is
negligible risk to human life, are to be designed for a
25-year mean recurrence interval.
Based on a given set of observed annual wind speeds, the
principal output from this procedure is the estimated wind
speeds, VN, for various mean recurrence intervals. Wind
speeds at 25, 50, 100, and 475 years return period are
listed in Table 4. The return period of 475 is calculated
using 50 year design lifetime of the structure and 10
percent accepted risk.
PLOTTING OF ISOTACHS
Isotachs for given recurrence intervals are plotted over
the geographic map of the Arabian peninsula from the
estimated extreme winds of twenty stations. A contouring
software is employed to plot the isotachs. The software
first generates information on a regularly spaced grid
from the irregular grid information supplied to it and
then develops a best fitting surface over the grid. The
fifty year return period wind speed contour map is plotted
in Fig.2.
CONCLUSIONS
In this study, appropriate extreme wind distribution
models for the largest yearly fastest-mile wind speed at
20 weather stations in the Kingdom are developed. The
analysis of the data revealed that the probabilistic
behavior of the series of the largest annual winds at
fifteen of the twenty stations can be described by the
Type I extreme distribution while at the remaining
stations by the Type II distribution. An isotach map for
50-year recurrence intervals is developed
Table 4. Fastest-Mile Design Wind Speed (MPH) at
Weather Stations for Different Mean Recurrence
Intervals.
----------------------------------------------------- Mean Recurrence Interval, years Station ------------------------------------ 25 50 100 475
-----------------------------------------------------
Badana 95.9 103.9 111.8 129.6
Bisha 79.1 85.2 91.3 104.9
Dhahran 61.6 65.1 68.5 76.1
Gassim 99.3 107.2 115.1 132.7
Gizan 90.6 98.6 106.8 124.9
Hail 79.8 87.2 95.2 115.8
Jeddah 69.2 73.7 78.2 88.3
Jouf 79.6 84.5 89.5 100.5
Khamis-Mushiat 66.3 71.6 76.9 88.4
Madiah 76.9 83.83 90.7 106.1
Najran 71.4 77.9 85.0 112.0
Hafer-Albatin 78.8 83.4 88.1 98.5
Riyadh 79.3 87.0 95.4 117.3
Rafah 78.5 83.6 88.7 100.0
Sulayel 83.4 92.9 103.3 131.1
Tabuk 81.1 88.5 96.6 117.2
Taif 79.1 85.2 91.3 104.9
Turaif 82.7 88.8 94.2 107.0
Wajh 73.9 79.7 85.4 98.3
Yanbu 67.9 72.6 77.3 87.7
------------------------------------------------------
Fig. 1 Isotach, in mile per hour, annual fastest-
mile, 33 feet above ground for exposure C,
with 50-year mean recurrence interval.
for use with the ANSI-procedure in developing wind loads.
The maximum basic design wind speed of 107.2 mph, for 50-
year mean recurrence interval, is obtained at Gassim
Station, while the minimum of 65.1 mph is obtained at
Dhahran. The ANSI-prescribed minimum of 70 mph is
exceeded at all stations excepting Dhahran.
REFERENCES
1- American National Standard Building Code Requirements
for Minimum Design Loads in Buildings and Other
Structures, A58.1, American National Standards
Institute, New York, NY, 1982.
2- Wind Loading and Wind-Induced Structural Response,
Report by the Committee on Wind Effects of the
Committee on Dynamic Effects of the Structral Division,
American Society of Civil Engineers, New York, N.Y,
1987.
3- Benjamin, J. R., and Cornell, C.A., Probability,
Statistics, and Decision for Civil Engineers, McGraw-
Hill Book Co. Inc., New York, N.Y, 1970.
4- Simiu, E. and Filliben, J.J., "Probability
Distributions of Extreme Wind Speeds", Journal of the
Structural Division, ASCE, Vol. 102, No. ST9,
September 1976, pp. 1861-1877.
5- Thom, H.C.S., "Distribution of Extreme Winds in the
United States", Journal of the Structural Division,
ASCE, Vol. 86, No. ST4, April, 1960, pp. 11-24.
6- Thom, H.C.S., "New Distributions of Extreme Winds in
the United States", Journal of the Structural
Division, ASCE, Vol. 94, No. ST7, July 1968, pp. 1787-
1801.
7- Simiu, E., and Filliben, J.J., "Statistical Analysis
of Extreme Winds," Technical Note No. 868, National
Bureau of Standards, Washington, D.C., 1975.
8- Simiu, E., Bietry, J. and Filliben, J.J., " Sampling
Errors in the Estimation of Extreme Winds," Journal of
the Structural Division, ASCE, Vol. 104, No. ST3,
March, 1978, pp. 491-501.
9- Simiu, E., and Scanlan, R., Wind Effects on
Structures, Second Edition, Wiley-Interscience
Publication, New York, 1986.
10- Simiu E., Changery, M.J., and Filliben, J.J., "Extreme
Wind Speeds at 129 Stations in the Contiguous United
States," NBS Building Science Series 118, U.S. Dept.
of Commerce, National Bureau of Standards, Mar. 1979.
11- Mehta, K.C., "Wind Load Provision ANSI #A58.1-1982,"
ASCE Annual Convention and Structural Congress, New
Orleans, La., October 1982, pp.769-784.
12- Canadian Structural Design Manual, Supplement No.4 to
the National Building Code of Canada, National
Research Council of Canada, 1970.
13- Lieblein, J., "A New Method of Analyzing Extreme-value
Data", National Bureau of Standards Report No. 2190,
Washington, D.C., 1953.