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INTERNATIONAL JOURNAL FOR TRENDS IN ENGINEERING & TECHNOLOGY
VOLUME 4 ISSUE 2 – APRIL 2015 - ISSN: 2349 - 9303
71
Weibull Distribution Based Channel Prototype For
Decrease of Rain Attenuation in Satellite
Communication Links Beyond 10GHz
Shanmugaraj. G1
1
Assistant Professor, Velammal Institute of Technology,
Electronics and Communication Engineering,
gsraj76@gmail.com
Guruprasad. B2
2
Velammal Institute of Technology, Bachelor of
Electronics and Communication Engineering
bguruprasadece@gmail.com
Sujith. S3
3
Velammal Institute of Technology, Bachelor of
Electronics and Communication Engineering,
ssujithece@gmail.com
Yuvaraj. S4
4
Velammal Institute of Technology, Bachelor of
Electronics and Communication Engineering
uvrajvit@gmail.com
Abstract— Current satellite communication networks will workat frequencies above 10GHz for transmission and reception of signals.
At these frequency bands, the most prevailing fading mechanism, is rain attenuation. In this paper, a unique channel prototype, a
synthesizer for generating rain attenuation time series for satellite links operating at 10GHz and above is offered. The proposed
channel prototype modifies M-B model since it generates rain attenuation time series that follow the Weibull distribution. The novel
dynamic model is based on the first-order Stochastic Differential Equations (SDEs) and deliberates rain attenuation induced on a slant
path as a Weibull-based stochastic process. Moreover, the theoretical terminologies for the computation of the exceedance probability
of hitting time random variable are presented. The synthesizer is substantiated in terms of the exceedance probability and the
speculative CCDF of hitting time comparing to these derived from the simulations in the hitting time section. The hitting time
statistics may be engaged for the prime strategy of Fade Mitigation Techniques (FMTs).
Index Terms—Satellite communications, Weibull distribution, stochastic differential equations, hitting time statistics, Brownian
motion.
————————————————————
1 INTRODUCTION
HE growing demand for high data rate services and the
insufficiency of the spectrum lead to the employment of
high frequency bands such as Ka and Q/V bands for the
operation of satellite systems. At operating frequencies above 10
GHz rainfall is the prevailing fading mechanism since it causes
the highest attenuation among the other atmospheric effects [1].
Due to the high values of rain attenuation for small time
percentage, though still critical for high availability systems, the
adoption of a fixed power margin as a countermeasure of rain
attenuation is not the optimal solution. Therefore, FadeMitigation
Techniques (FMTs) must be introduced into the system [1].
Such techniques include the Adaptive Coding and Modulation
(ACM) technique and the power control. For the estimation of the
FMTs, time series synthesizers are needed. Time series
synthesizers are also useful for system evaluation in case that
investigational rain attenuation time series are not available. In
[2], the M-B model, a time series synthesizer, hasbeen proposed
based on SDEs assuming that rain attenuation follows the
lognormal distribution and that the rate of change of rain
attenuation is proportional to the instantaneous value of rain
attenuation.
The methodical solution of the SDE proposed in [2] has been
given in [4]. The application of SDEs to communication systems
is presented in [5]. However, in [6] and [7], it is shown that rain
attenuation can be also described with the Weibull distribution.
Recently, the experimental results has been shown that the
Weibull based model of [7] gives much better expectation than
other prediction models [8]. Furthermore, apart from the
generation of time series, one of the metrics that are required for
the depiction of rain attenuation dynamics is the hitting time
measurements [9]. Hitting time statistical properties have been
used for the advance of an analytical method for the calculation of
the rain attenuation active parameter [4], as well as, their
application for the optimization of FMTs [10].
The contribution of this prototype, is the development of a new
rain attenuation time series synthesizer and the calculation ofits
hitting time distribution. The basic conventions are that first-order
statistics of rain follow Weibull distribution and that the rate of
change of rain attenuation is proportional to the instantaneous
value of rain attenuation. These new theoretical results, given in
this proposal, are methodical and can be used for the
development and the ideal design of next generation FMTs and
new protocols for broadband satellite communication networks
operating above 10GHz. In Section II, the SDE for the generation
of Weibull distributed rain attenuation time series is presented as
well as its analytical solution.
T
INTERNATIONAL JOURNAL FOR TRENDS IN ENGINEERING & TECHNOLOGY
VOLUME 4 ISSUE 2 – APRIL 2015 - ISSN: 2349 - 9303
72
The theoretical expressions for the computation of the exceedance
probability of hitting time statistical distribution is presented,
along with a brief portrayal for its possible use in satellite FMTs.
In the numerical results section it is proven that the generated
time series of rain attenuation follow in long-term the Weibull
distribution and that the theoretical expressions of the hitting time
statistics essentially reproduce these of the synthesizer presented.
2 CLOUD ATTENUATION
The liquid water content of clouds is the physical cause of cloud
attenuation. Prophecy models for this particular attenuation factor
have been developed within the framework of ITU-R and
elsewhere. The figure depicts attenuation values due to clouds
and fog exceeded for a certain range of probabilities. Here,
attenuation refers to the turbulences made due to the clouds which
results in a loss of data communication or a severe distortion in
signals. A novel method to have a better efficiency against cloud
attenuation has been proposed. The proposed prototype has been
considered as a pictorial representation in order to obtain the
main aspects of the prototype, which solves the issue of
accomplishing higher data rate during disturbances. The ITU-R
model was selected as the underlying prediction method for
generating the model, which resemble the three frequency bands
examined in this study.
Fig. 1. Illustration of cloud attenuation
3 BROWNIAN MOTION
Brownian motion is a contemporary reference to a mathematical
model of the random motion of particles deferred in a fluid. This
category of motion was named after Robert Brown that observed
it in water. Considering the Brownian motion as a standard
parameter, the rain attenuation in satellite
communication is further reduced. The procedures were
described accurately by Norbert Wiener, and are thus also called
Wiener Processes. Some mathematical incorporations of a
standard Brownian motion are into existence. They point out that,
the process starts at zero with a probability of 1, and thatthe
probability, that anarbitrarilyengendered Brownian path be
continuous is 1.The path augmentations are independent
Gaussian, zero mean, with variance equivalent to the temporal
extension of the increment. A figure portraying Brownian motion
can be given by:
Fig. 2. Nature of Brownian motion.
4FMT
In satellite communication systems, accessibilityis defined as the
time percentage in a year throughout which the bit error rate
(BER) is inferior than a certain threshold, beyond which an
outage of the system occurs, although the fade margin is
appropriatelydefined as the difference in dB between the
precipitation prompted attenuation resulting in an outage and the
attenuationunder clear sky environments. To elaborate on the
concept of availability, and illustrate the transformation from the
rain attenuation distribution to the equivalentBER distribution, a
clear sky bit energy to noise power density ratio Eb/N0 of 12dB
and a QPSK modulation scheme may be anticipated. Since the
proposals, deduce that if, for example, a BER threshold higher
than 10 –7 makes the system unavailable, the outage percentage
for this definite satellite link will be 0.060 percent at the Ku band,
0.096 percent at the Ka band, and 0.205 percent at the V band, the
assumption comes into use. In terms of min/year this event takes
place, the conforming outage times are 315.4min/year,
504.6min/year, and 1077.5min/year, respectively.
Fig. 3. FMT control loop flow chart
5WEIBULL BASED STOCHASTIC DYNAMIC
MODEL
An extended comparative test took place considering
experimental data from ITUs database of Study Group 3
(DBSG3) [11] in order to observe the suitability of Weibull
distribution for modeling the rain attenuation exceedance
INTERNATIONAL JOURNAL FOR TRENDS IN ENGINEERING & TECHNOLOGY
VOLUME 4 ISSUE 2 – APRIL 2015 - ISSN: 2349 - 9303
73
probability. Considering 86 experiments from DBSG3 database it
was found that the RMS value of the relative error was 13.47%
for Weibull distribution and 13.8% for lognormal
distribution.Furthermore weibull distribution has a lesser error
probability than the other counterpart distributions which adds up
to its advantage. This leads to the conclusion that Weibull
distribution in many cases may describe better rain attenuation
exceedance probability than lognormal distribution. This is a
strong motivation in order to derive a rain attenuation synthesizer
based on Weibull distribution.The Probability Density Function
(PDF) of Weibull distribution is:
w
x
v
X
v
ex
w
v
xp


 1
)( , x >0 (1)
where ν and w are the two parameters of Weibull distribution
which must be greater than 0.
The SDE for the rain attenuation modeling, is:
dA(t)=K1(A(t)).dt+ √𝐾2(𝐴(𝑡))dB(t) (2)
where B(t) is the Brownian Motion [13] and dB(t) the Brownian
increments. K1(A(t)) is the drift coefficient and K2(A(t)) the
diffusion coefficient of the SDE. The rate of change of rain
attenuation is considered proportional to the instantaneous value
of rain attenuation, similarly with [2] and has been verified by
experimental data. Therefore, given the definition of the diffusion
coefficient the latter is chosen equal to:
K2(A(t)) =
2𝑑 𝑎 𝑤
𝑣
A2
(t) (3)
where da is the dynamic parameter of rain attenuation. The value
of the dynamic parameter may be computed either from local rain
attenuation measurements or set equal to the proposed value 2 ・
10−4, according to the recommendation ITU-R. P.1853-1 [3].
Now, considering that the static distribution of rain attenuation
stochastic process A(t) follows the Weibull distribution.The
strong solution of the SDE is:
v
t swdvsB
v
wd
v
v
a
a
v
wd
dseAvd
twdtBeA
tA
a
a
a
1
0
)(
2
0
2
0
1
)(
)(













where B(t) is the Brownian Motion and A0 is the initial value of
rain attenuation, which can be a low value such as 0.5dB.
Therefore, by consuming this expression, rain attenuation time
series can be generated. A MATLAB file can be easily developed
for the rain attenuation time series synthesis, expending the
expression.
6 HITTING TIME
Hitting time is the time needed for a stochastic process to reach a
minimum or maximum attenuation threshold value, Amin or
Amax, respectively, given that the value of a stochastic process is
A0, with Amin ≤ A0 ≤ Amax, at the initial time occurrence t=t0.
Since hitting time refers to a stochastic process, the prior term is,
a random variable.
Fig. 4. CCDF of hitting time of rain attenuation
7 EXCEEDANCE PROBABILITY
Sometimes the actualities about what are the chances over a given
time period that a flood will reach or exceed a
definiteenormousness may need to be known. This is called the
probability of occurrence or the exceedance probability. The
exceedance probability may be articulated simply as the inverse
of the return period Let's say the value "p" is the exceedance
probability, in whichever given year. For instance, for atwo-year
return period the exceedance probability in any given year is one
over two is equivalent to 0.5, or 50 percent.We need to know the
technique to calculate the exceedance probability for a particular
retro of years, and not just one certain year. To do this, we use the
authentic expression of exceedance probabilitywhich may be
inferred as 1- (1 - p) n
. In this formula we consider all possible
flows over the period of interest "n" and we can denote the whole
set of flows with "1." Then (1-p) is the chance of the flow not in
the works, or the non-exceedance probability, but for any given
year. Finally, "1," all possible flows, minus (1-p) n
, all flows
during the time period than are inferior than our interest, leaves
us with this specific expression, and the probability of those flows
of interest happening within the stated time period. A one-
hundred yearflood is an event of flood, that has a 1% probability
of occurrence in whichever given year. The 100-year flood is
similarlydenoted as the 1% flood, since its annual exceedance
probability is 1%.So, if we need to calculate the odds for a 100-
year flood, over a 30-year time period, we can then use these
values in the formula for the exceedance probability.
8 CONCLUSION
In this paper a new channel prototype has been presented for
fixed satellite communication links operating above 10GHz.
Firstly, it is shown that the Weibull distribution can be used for
modeling of rain attenuation exceedance probability with similar
10
1
10
2
10
3
10
-3
10
-2
10
-1
10
0
Hitting Time(sec)
ExceedanceProbability
CCDF of Hitting Time
Simulated CCDF(A0
=8dB,Amin
=6dB,Amax
=12dB)
Theoritical CCDF(A0
=8dB,Amin
=6dB,Amax
=12dB)
Simulated CCDF(A0
=7dB,Amin
=4dB,Amax
=11dB)
Theoritical CCDF(A0
=7dB,Amin
=4dB,Amax
=11dB)
INTERNATIONAL JOURNAL FOR TRENDS IN ENGINEERING & TECHNOLOGY
VOLUME 4 ISSUE 2 – APRIL 2015 - ISSN: 2349 - 9303
74
results to the lognormal distribution. Brownian motion is
considered as a standard parameter. It also improves the results
for fade slope statistics at high levels of rain attenuation. This is
imperative for the proposal and optimization of FMTs for
systemsoperating in tropical expanses, which are subject to high
rainfall proportions. Empirical expressions for estimating the
dynamics parameter as a function of the path length were
obtained, that allow the synthesizer implementation without the
need of experimental data.
9REFERENCES
[1] .A. D. Panagopoulos, P.-D. M. Arapoglou, and P. G. Cottis,
―Satellite communications at ku, ka and V bands: propagation
impairments and mitigation techniques,‖ IEEE Commun. Surveys
Tuts., pp. 2–14, 2004.
[2]. T. Maseng and P. M. Bakken, ―Satellite communications at
ku, ka and V bands: propagation impairments and mitigation
techniques,‖ IEEE Trans. Commun., vol. COM-29, no. 5, pp.
660–669, 1981.
[3]. ITU-R. P. 1853, Tropospheric attenuation time series
synthesis, Geneva, 2009.
[4]. S. A. Kanellopoulos, A. D. Panagopoulos, and J. D.
Kanellopoulos, ―Calculation of the dynamic input parameter for a
stochastic model simulating rain attenuation: a novel
mathematical approach,‖ IEEE Trans. Antennas Propag., vol. 55,
no. 11, pp. 3257–3264, 2007.
[5]. S. Primak, V. Kontronovih, and V. Lyandres, Stochastic
Methods and their Applications to Communications: Stochastic
Differential Equations Approach. John Wiley & Sons, 2005.
[6]. S. N. Livieratos, V. Katsambas, and J. D. Kanellopoulos, ―A
global method for the prediction of the slant path rain attenuation
statistics,‖ J. Electrom. Waves and Applic., vol. 14, no. 5, pp.
713–724, 2000.
[7]. A. D. Panagopoulos, P.-D. M. Arapoglou, J. D.
Kanellopoulos, and P. G. Cottis, ―Long-term rain attenuation
probability and site diversity gain prediction formulas,‖ IEEE
Trans. Antennas Propag., vol. 53, no. 7, pp. 2307–2313, 2005.
[8]. J. M. Garcia-Rubia, J. M. Riera, P. Garcia-del-Pino, and A.
Benarroch, ―Five-year results of a slant-path propagation
experiment at 20 GHz in Madrid,‖ in 2012 Conference at Ka and
Broadband Communications.
[9]. S. Karlin and H. Taylor, A Second Course in Stochastic
Processes. Academic, 1981.
[10] C. I. Kourogiorgas, S. A. Kanellopoulos, A. D.
Panagopoulos, S. N. Livieratos, G. E. Chatzarakis, and J. D.
Kanellopoulos, ―Rain attenuation hitting time statistical
distribution: application to fade mitigation techniques of future
satellite communication systems,‖ in 2012 ESTEL Conference.
[11]ITU-R. Databank DBSG3, http://www.itu.int/publ/R-
SOFTSG3/en,Geneva, 2010.

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Weibull Distribution Based Channel Prototype For Decrease of Rain Attenuation in Satellite Communication Links Beyond 10GHz

  • 1. INTERNATIONAL JOURNAL FOR TRENDS IN ENGINEERING & TECHNOLOGY VOLUME 4 ISSUE 2 – APRIL 2015 - ISSN: 2349 - 9303 71 Weibull Distribution Based Channel Prototype For Decrease of Rain Attenuation in Satellite Communication Links Beyond 10GHz Shanmugaraj. G1 1 Assistant Professor, Velammal Institute of Technology, Electronics and Communication Engineering, gsraj76@gmail.com Guruprasad. B2 2 Velammal Institute of Technology, Bachelor of Electronics and Communication Engineering bguruprasadece@gmail.com Sujith. S3 3 Velammal Institute of Technology, Bachelor of Electronics and Communication Engineering, ssujithece@gmail.com Yuvaraj. S4 4 Velammal Institute of Technology, Bachelor of Electronics and Communication Engineering uvrajvit@gmail.com Abstract— Current satellite communication networks will workat frequencies above 10GHz for transmission and reception of signals. At these frequency bands, the most prevailing fading mechanism, is rain attenuation. In this paper, a unique channel prototype, a synthesizer for generating rain attenuation time series for satellite links operating at 10GHz and above is offered. The proposed channel prototype modifies M-B model since it generates rain attenuation time series that follow the Weibull distribution. The novel dynamic model is based on the first-order Stochastic Differential Equations (SDEs) and deliberates rain attenuation induced on a slant path as a Weibull-based stochastic process. Moreover, the theoretical terminologies for the computation of the exceedance probability of hitting time random variable are presented. The synthesizer is substantiated in terms of the exceedance probability and the speculative CCDF of hitting time comparing to these derived from the simulations in the hitting time section. The hitting time statistics may be engaged for the prime strategy of Fade Mitigation Techniques (FMTs). Index Terms—Satellite communications, Weibull distribution, stochastic differential equations, hitting time statistics, Brownian motion. ———————————————————— 1 INTRODUCTION HE growing demand for high data rate services and the insufficiency of the spectrum lead to the employment of high frequency bands such as Ka and Q/V bands for the operation of satellite systems. At operating frequencies above 10 GHz rainfall is the prevailing fading mechanism since it causes the highest attenuation among the other atmospheric effects [1]. Due to the high values of rain attenuation for small time percentage, though still critical for high availability systems, the adoption of a fixed power margin as a countermeasure of rain attenuation is not the optimal solution. Therefore, FadeMitigation Techniques (FMTs) must be introduced into the system [1]. Such techniques include the Adaptive Coding and Modulation (ACM) technique and the power control. For the estimation of the FMTs, time series synthesizers are needed. Time series synthesizers are also useful for system evaluation in case that investigational rain attenuation time series are not available. In [2], the M-B model, a time series synthesizer, hasbeen proposed based on SDEs assuming that rain attenuation follows the lognormal distribution and that the rate of change of rain attenuation is proportional to the instantaneous value of rain attenuation. The methodical solution of the SDE proposed in [2] has been given in [4]. The application of SDEs to communication systems is presented in [5]. However, in [6] and [7], it is shown that rain attenuation can be also described with the Weibull distribution. Recently, the experimental results has been shown that the Weibull based model of [7] gives much better expectation than other prediction models [8]. Furthermore, apart from the generation of time series, one of the metrics that are required for the depiction of rain attenuation dynamics is the hitting time measurements [9]. Hitting time statistical properties have been used for the advance of an analytical method for the calculation of the rain attenuation active parameter [4], as well as, their application for the optimization of FMTs [10]. The contribution of this prototype, is the development of a new rain attenuation time series synthesizer and the calculation ofits hitting time distribution. The basic conventions are that first-order statistics of rain follow Weibull distribution and that the rate of change of rain attenuation is proportional to the instantaneous value of rain attenuation. These new theoretical results, given in this proposal, are methodical and can be used for the development and the ideal design of next generation FMTs and new protocols for broadband satellite communication networks operating above 10GHz. In Section II, the SDE for the generation of Weibull distributed rain attenuation time series is presented as well as its analytical solution. T
  • 2. INTERNATIONAL JOURNAL FOR TRENDS IN ENGINEERING & TECHNOLOGY VOLUME 4 ISSUE 2 – APRIL 2015 - ISSN: 2349 - 9303 72 The theoretical expressions for the computation of the exceedance probability of hitting time statistical distribution is presented, along with a brief portrayal for its possible use in satellite FMTs. In the numerical results section it is proven that the generated time series of rain attenuation follow in long-term the Weibull distribution and that the theoretical expressions of the hitting time statistics essentially reproduce these of the synthesizer presented. 2 CLOUD ATTENUATION The liquid water content of clouds is the physical cause of cloud attenuation. Prophecy models for this particular attenuation factor have been developed within the framework of ITU-R and elsewhere. The figure depicts attenuation values due to clouds and fog exceeded for a certain range of probabilities. Here, attenuation refers to the turbulences made due to the clouds which results in a loss of data communication or a severe distortion in signals. A novel method to have a better efficiency against cloud attenuation has been proposed. The proposed prototype has been considered as a pictorial representation in order to obtain the main aspects of the prototype, which solves the issue of accomplishing higher data rate during disturbances. The ITU-R model was selected as the underlying prediction method for generating the model, which resemble the three frequency bands examined in this study. Fig. 1. Illustration of cloud attenuation 3 BROWNIAN MOTION Brownian motion is a contemporary reference to a mathematical model of the random motion of particles deferred in a fluid. This category of motion was named after Robert Brown that observed it in water. Considering the Brownian motion as a standard parameter, the rain attenuation in satellite communication is further reduced. The procedures were described accurately by Norbert Wiener, and are thus also called Wiener Processes. Some mathematical incorporations of a standard Brownian motion are into existence. They point out that, the process starts at zero with a probability of 1, and thatthe probability, that anarbitrarilyengendered Brownian path be continuous is 1.The path augmentations are independent Gaussian, zero mean, with variance equivalent to the temporal extension of the increment. A figure portraying Brownian motion can be given by: Fig. 2. Nature of Brownian motion. 4FMT In satellite communication systems, accessibilityis defined as the time percentage in a year throughout which the bit error rate (BER) is inferior than a certain threshold, beyond which an outage of the system occurs, although the fade margin is appropriatelydefined as the difference in dB between the precipitation prompted attenuation resulting in an outage and the attenuationunder clear sky environments. To elaborate on the concept of availability, and illustrate the transformation from the rain attenuation distribution to the equivalentBER distribution, a clear sky bit energy to noise power density ratio Eb/N0 of 12dB and a QPSK modulation scheme may be anticipated. Since the proposals, deduce that if, for example, a BER threshold higher than 10 –7 makes the system unavailable, the outage percentage for this definite satellite link will be 0.060 percent at the Ku band, 0.096 percent at the Ka band, and 0.205 percent at the V band, the assumption comes into use. In terms of min/year this event takes place, the conforming outage times are 315.4min/year, 504.6min/year, and 1077.5min/year, respectively. Fig. 3. FMT control loop flow chart 5WEIBULL BASED STOCHASTIC DYNAMIC MODEL An extended comparative test took place considering experimental data from ITUs database of Study Group 3 (DBSG3) [11] in order to observe the suitability of Weibull distribution for modeling the rain attenuation exceedance
  • 3. INTERNATIONAL JOURNAL FOR TRENDS IN ENGINEERING & TECHNOLOGY VOLUME 4 ISSUE 2 – APRIL 2015 - ISSN: 2349 - 9303 73 probability. Considering 86 experiments from DBSG3 database it was found that the RMS value of the relative error was 13.47% for Weibull distribution and 13.8% for lognormal distribution.Furthermore weibull distribution has a lesser error probability than the other counterpart distributions which adds up to its advantage. This leads to the conclusion that Weibull distribution in many cases may describe better rain attenuation exceedance probability than lognormal distribution. This is a strong motivation in order to derive a rain attenuation synthesizer based on Weibull distribution.The Probability Density Function (PDF) of Weibull distribution is: w x v X v ex w v xp    1 )( , x >0 (1) where ν and w are the two parameters of Weibull distribution which must be greater than 0. The SDE for the rain attenuation modeling, is: dA(t)=K1(A(t)).dt+ √𝐾2(𝐴(𝑡))dB(t) (2) where B(t) is the Brownian Motion [13] and dB(t) the Brownian increments. K1(A(t)) is the drift coefficient and K2(A(t)) the diffusion coefficient of the SDE. The rate of change of rain attenuation is considered proportional to the instantaneous value of rain attenuation, similarly with [2] and has been verified by experimental data. Therefore, given the definition of the diffusion coefficient the latter is chosen equal to: K2(A(t)) = 2𝑑 𝑎 𝑤 𝑣 A2 (t) (3) where da is the dynamic parameter of rain attenuation. The value of the dynamic parameter may be computed either from local rain attenuation measurements or set equal to the proposed value 2 ・ 10−4, according to the recommendation ITU-R. P.1853-1 [3]. Now, considering that the static distribution of rain attenuation stochastic process A(t) follows the Weibull distribution.The strong solution of the SDE is: v t swdvsB v wd v v a a v wd dseAvd twdtBeA tA a a a 1 0 )( 2 0 2 0 1 )( )(              where B(t) is the Brownian Motion and A0 is the initial value of rain attenuation, which can be a low value such as 0.5dB. Therefore, by consuming this expression, rain attenuation time series can be generated. A MATLAB file can be easily developed for the rain attenuation time series synthesis, expending the expression. 6 HITTING TIME Hitting time is the time needed for a stochastic process to reach a minimum or maximum attenuation threshold value, Amin or Amax, respectively, given that the value of a stochastic process is A0, with Amin ≤ A0 ≤ Amax, at the initial time occurrence t=t0. Since hitting time refers to a stochastic process, the prior term is, a random variable. Fig. 4. CCDF of hitting time of rain attenuation 7 EXCEEDANCE PROBABILITY Sometimes the actualities about what are the chances over a given time period that a flood will reach or exceed a definiteenormousness may need to be known. This is called the probability of occurrence or the exceedance probability. The exceedance probability may be articulated simply as the inverse of the return period Let's say the value "p" is the exceedance probability, in whichever given year. For instance, for atwo-year return period the exceedance probability in any given year is one over two is equivalent to 0.5, or 50 percent.We need to know the technique to calculate the exceedance probability for a particular retro of years, and not just one certain year. To do this, we use the authentic expression of exceedance probabilitywhich may be inferred as 1- (1 - p) n . In this formula we consider all possible flows over the period of interest "n" and we can denote the whole set of flows with "1." Then (1-p) is the chance of the flow not in the works, or the non-exceedance probability, but for any given year. Finally, "1," all possible flows, minus (1-p) n , all flows during the time period than are inferior than our interest, leaves us with this specific expression, and the probability of those flows of interest happening within the stated time period. A one- hundred yearflood is an event of flood, that has a 1% probability of occurrence in whichever given year. The 100-year flood is similarlydenoted as the 1% flood, since its annual exceedance probability is 1%.So, if we need to calculate the odds for a 100- year flood, over a 30-year time period, we can then use these values in the formula for the exceedance probability. 8 CONCLUSION In this paper a new channel prototype has been presented for fixed satellite communication links operating above 10GHz. Firstly, it is shown that the Weibull distribution can be used for modeling of rain attenuation exceedance probability with similar 10 1 10 2 10 3 10 -3 10 -2 10 -1 10 0 Hitting Time(sec) ExceedanceProbability CCDF of Hitting Time Simulated CCDF(A0 =8dB,Amin =6dB,Amax =12dB) Theoritical CCDF(A0 =8dB,Amin =6dB,Amax =12dB) Simulated CCDF(A0 =7dB,Amin =4dB,Amax =11dB) Theoritical CCDF(A0 =7dB,Amin =4dB,Amax =11dB)
  • 4. INTERNATIONAL JOURNAL FOR TRENDS IN ENGINEERING & TECHNOLOGY VOLUME 4 ISSUE 2 – APRIL 2015 - ISSN: 2349 - 9303 74 results to the lognormal distribution. Brownian motion is considered as a standard parameter. It also improves the results for fade slope statistics at high levels of rain attenuation. This is imperative for the proposal and optimization of FMTs for systemsoperating in tropical expanses, which are subject to high rainfall proportions. Empirical expressions for estimating the dynamics parameter as a function of the path length were obtained, that allow the synthesizer implementation without the need of experimental data. 9REFERENCES [1] .A. D. Panagopoulos, P.-D. M. Arapoglou, and P. G. Cottis, ―Satellite communications at ku, ka and V bands: propagation impairments and mitigation techniques,‖ IEEE Commun. Surveys Tuts., pp. 2–14, 2004. [2]. T. Maseng and P. M. Bakken, ―Satellite communications at ku, ka and V bands: propagation impairments and mitigation techniques,‖ IEEE Trans. Commun., vol. COM-29, no. 5, pp. 660–669, 1981. [3]. ITU-R. P. 1853, Tropospheric attenuation time series synthesis, Geneva, 2009. [4]. S. A. Kanellopoulos, A. D. Panagopoulos, and J. D. Kanellopoulos, ―Calculation of the dynamic input parameter for a stochastic model simulating rain attenuation: a novel mathematical approach,‖ IEEE Trans. Antennas Propag., vol. 55, no. 11, pp. 3257–3264, 2007. [5]. S. Primak, V. Kontronovih, and V. Lyandres, Stochastic Methods and their Applications to Communications: Stochastic Differential Equations Approach. John Wiley & Sons, 2005. [6]. S. N. Livieratos, V. Katsambas, and J. D. Kanellopoulos, ―A global method for the prediction of the slant path rain attenuation statistics,‖ J. Electrom. Waves and Applic., vol. 14, no. 5, pp. 713–724, 2000. [7]. A. D. Panagopoulos, P.-D. M. Arapoglou, J. D. Kanellopoulos, and P. G. Cottis, ―Long-term rain attenuation probability and site diversity gain prediction formulas,‖ IEEE Trans. Antennas Propag., vol. 53, no. 7, pp. 2307–2313, 2005. [8]. J. M. Garcia-Rubia, J. M. Riera, P. Garcia-del-Pino, and A. Benarroch, ―Five-year results of a slant-path propagation experiment at 20 GHz in Madrid,‖ in 2012 Conference at Ka and Broadband Communications. [9]. S. Karlin and H. Taylor, A Second Course in Stochastic Processes. Academic, 1981. [10] C. I. Kourogiorgas, S. A. Kanellopoulos, A. D. Panagopoulos, S. N. Livieratos, G. E. Chatzarakis, and J. D. Kanellopoulos, ―Rain attenuation hitting time statistical distribution: application to fade mitigation techniques of future satellite communication systems,‖ in 2012 ESTEL Conference. [11]ITU-R. Databank DBSG3, http://www.itu.int/publ/R- SOFTSG3/en,Geneva, 2010.