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International Journal of Electrical and Computer Engineering (IJECE)
Vol. 10, No. 5, October 2020, pp. 5296~5305
ISSN: 2088-8708, DOI: 10.11591/ijece.v10i5.pp5296-5305  5296
Journal homepage: http://ijece.iaescore.com/index.php/IJECE
On the performance of energy harvesting AF partial relay
selection with TAS and outdated channel state
information over identical channels
Kehinde O. Odeyemi1
, Pius A. Owolawi2
1
Department of Electrical and Electronic Engineering, Faculty of Technology, University of Ibadan, Nigeria
2
Department of Computer Systems Engineering, Tshwane University of Technology, South Africa
Article Info ABSTRACT
Article history:
Received Apr 27, 2019
Revised Apr 7, 2020
Accepted Apr 20, 2020
Energy scarcity has been known to be one of the most noticeable challenges
in wireless communication system. In this paper, the performance of an
energy harvesting based partial relay selection (PRS) cooperative system
with transmit antenna selection (TAS) and outdated channel state information
(CSI) is investigated. The system dual-hops links are assumed to follow
Rayleigh distribution and the relay selection is based on outdated CSI of
the first link. To realize the benefit of multiple antenna, the amplified-and-
forward (AF) relay nodes then employs the TAS technique for signal
transmission and signal reception is achieved at the destination through
maximum ratio combining (MRC) scheme. Thus, the closed-form expression
for the system equivalent end-to-end cumulative distribution function (CDF)
is derived. Based on this, the analytical closed-form expressions for
the outage probability, average bit error rate, and throughput for the delay-
limited transmission mode are then obtained. The results illustrated that
the energy harvesting time, relay distance, channel correlation coefficient,
the number of relay transmit antennas and destination received antenna have
significant effect on the system performance. Monte-carol simulation is
employed to validate the accuracy of the derived expressions.
Keywords:
Channel state information
Energy harvesting
Maximum ratio combining
Partial relay selection
Transmit antenna selection
Copyright Β© 2020 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Kehinde O. Odeyemi,
Department of Electrical and Electronic Engineering,
Factulty of Technology, University of Ibadan,
Ibadan, Nigeria.
Email: odeyemikenny@gmail.com
1. INTRODUCTION
Traditionally, relay nodes within the wireless cooperative network are usually equipped with power-
limited batteries that are infeasible, costly and even impossible to replace in some applications [1, 2].
As a result of this, energy harvesting (EH) has been considered as a promising solution to alleviate this stated
energy constraint in wireless system. Therefore, research studies have suggested that batteries can be
wirelessly recharge using external power sources from free ambient such as solar, wind, thermal and
vibration [3]. These conventional sources are not always available and mostly suffers from time-varying
problem and materials inefficiency [4, 5]. Based on this, RF source has been regarded as the best alternative
means of harvesting energy in wireless communication since it carries both the energy and information at
the same time without monitoring and maintenance [6]. In this case, two schemes have been suggested in
literature through which energy can be harvested and this include time switching (TS) and power splitting
(PS) protocols. In TS protocol, the transmission time is divided into two parts where the receiver nodes spend
one to harvest energy from the source and the remaining for information transmission. In PS protocol on
the other hand, the receiver nodes used part of the EH and the other for information processing [7].
Int J Elec & Comp Eng ISSN: 2088-8708 
On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi)
5297
The deployment of relays in wireless networks can extend the signal coverage and overcoming
the channel impairment as a result of fading [8]. Therefore, two strategies have been suggested for relay to
transmit its received signal to the destination for which include decode-and-forward (DF) and amplify-and-
forward (AF) of relaying system [4, 9]. In DF relaying system, the received signal is fully decoded and
the decoded copy is retransmitted to the destination. In AF relaying system on the other hand, the received
signal is simply amplified and forwarded to the destination without decoding leading to its simplicity and
effective implementation cost [10]. In the wireless cooperative system with multiple relays, numerous relay
selection techniques have proposed [6] and this include the partial relay selection where selection of relays
depends on the CSI of the source-relay links or relay-destination links. This thus avoids the issues such as
high power consumption, overhead and network delays, and can also prolong the network lifetime [11, 12].
Unlike the best and opportunistic relay selection approaches, which require global knowledge of the CSI of each
of the two hops [12, 13] leading to time synchronization, continuous channel feedback and high power
consumption.
Reducing the energy consumption of cooperative relaying system through the energy harvesting has
drawn more attention in the research community has attracted attention in the research community.
The performance of dual-hop relaying network with three different wireless EH mechanisms at the DF relay
nodes over the generalized channels was studied [14]. In [15], the performance of a wireless information
power transfer in AF relay network with multiple antenna over dissimilar channel and the benefit of
MRC/TAS was exploit for the relay node was investigated. The Ergodic outage and capacity performance of
wireless power transfer based AF relaying system was presented in [16]. Also, the performance of DF-based
EH with the source node and the destination employing TAS and MRC respectively was evaluated in [17].
The throughput performance of an AF relay based EH under delay-tolerance and limited transmission modes
was investigated in [7] over Rayleigh fading channels. However, all these aforementioned works are limited
to a single relay-based EH cooperative systems.
In case of multiple relay selection, the performance of EH cooperative system with optimal relay
selection under the CSI and energy side information was investigated in [18]. In addition, incremental relay
network with EH-based relay selection was proposed in [19] where the selected relay harvesting the largest
source energy was chosen to forward the information to the destination. In [20], the performance of AF
relaying energy harvesting system with π‘˜π‘‘β„Ž best PRS and energy beamforming over Nakagami-m was
evaluated. In this work, it was assumed that both the source and the destination are multiple antenna nodes
and the relay are single antenna nodes. In all these aforementioned studies, perfect CSI was assumed for
the system. Motivated by this, the performance of the PRS-based EH system under the TAS/MRC is
investigated in this paper where the relay nodes employ the TAS technique at the relay nodes and maximum
ratio combining (MRC) scheme at the destination. The exact closed-form expression for the system outage
probability and average bit error rate are obtained. Utilizing the outage probability, the throughput for
the system is obtained based on delay-limited transmission mode. The impact of energy harvesting time,
relay distance, channel correlation coefficient, the number of relay transmit antennas and destination received
antenna on the concerned system are demonstrated.
2. SYSTEM AND CHANNEL MODEL
In this paper, a dual-hops PRS based energy harvesting system with PRS and outdated CSI is
presented in Figure 1 (a). The source (S) is equipped with a single transmit antenna and the destination (D)
has multiple receive antenna 𝑁 𝐷. The relay (R) of 𝑁 nodes utilize a single receive antenna and multiple
transmit antenna 𝑁𝑅
𝑑
. It is assumed that the S-to-R and R-to-D links undergo Rayleigh fading distribution
without direct link between the source and the destination. The relay nodes employ TAS scheme to select
the best antenna to forward the signal to the destination through which the instantaneous SNR at
the destination is maximized. At the destination, MRC is used to combine the transmitted signal from
the relay node(s). As a result of channel fast fading, it is considered that relay selection is based on outdated
CSI. Thus, the instantaneous SNR of the first link and the one used for PRS are two correlated random
variables with channel correlation coefficient 𝜌.The transmission over the links is assumed to be in
half-duplex mode so as to avoid inter-signal interference. Therefore, the overall systems communication is
established in two different phases.
During the first phase, the communication between the S and R nodes is divided into power
transmission and information transmission as presented in Figure 1(b). Based on this, the π‘˜ βˆ’ π‘‘β„Ž selected
relay(s) harvest the energy and then receive the information from the source using the time switching-base
relay (TSR) protocol. Thereafter, the source information is amplified through AF relaying and then convey to
the destination using TAS technique. In TSR protocol, a total block time slot of 𝑇 is divided into three parts:
for energy harvesting as 𝛼𝑇, information transmission between S-to-R as (1 βˆ’ 𝛼)𝑇/2 and information
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 5, October 2020 : 5296 - 5305
5298
transmission between R-to-D as (1 βˆ’ 𝛼)𝑇/2. The parameter 𝛼 denotes the energy having time factor at
0 ≀ 𝛼 ≀ 1. Thus, the receive signal by the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) can be expressed as:
𝑦1(π‘˜)(𝑑) = √
𝑃𝑠
𝑑1
πœ—1
β„Ž1(π‘˜) π‘₯(𝑑) + 𝑛 𝑅(π‘˜)(𝑑) (1)
where 𝑃𝑠 is the source transmitted power, β„Ž1(π‘˜) is π‘˜ βˆ’ π‘‘β„Ž the channel gain, 𝑑1 is the distance between
the source and the relay, πœ—1 denotes the path loss exponent, π‘₯(𝑑) represents the sources information and 𝑛 𝑅(π‘˜)
is the AWGN at the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) with zero mean and variance 𝜎1
2
. The energy harvested by an
energy receiver at the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) over the time 𝛼𝑇 can be expressed as [1, 11]:
πΈβ„Ž,π‘˜ =
πœ‚π›Όπ‘‡|β„Ž1(π‘˜)|
2
𝑑1
πœ—1
(2)
where 0 ≀ πœ‚ ≀ 1 denotes the energy harvesting efficiency which depends on the rectification process and
the circuitry.
During the second phase, the remaining time slot of (1 βˆ’ 𝛼)𝑇/2 duration is then used by the π‘˜ βˆ’ π‘‘β„Ž
selected relay(s) to amplifies and retransmit the information to the destination using TAS principle.
The destination thus employs MRC technique to combine the transmitted signal from the π‘˜ βˆ’ π‘‘β„Ž selected
relay(s) and the received signal can be expressed as:
𝑦2(𝑑) = √
𝑃 𝑅(π‘˜)
𝑑2
πœ—2
β„Ž2(π‘˜) π‘₯Μ‚(𝑑) + 𝑛 𝐷(𝑑) (3)
where β„Ž2(π‘˜) the channel gain, 𝑑2 is the distance between the relay and destination, πœ—2 denotes the path loss
exponent, π‘₯Μ‚(𝑑) represents the decoded information of π‘₯(𝑑), 𝑛 𝐷 is the AWGN at the destination with zero
mean and variance 𝜎2
2
, and 𝑃𝑅(π‘˜) is the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) transmit power obtained from energy
harvesting for relaying amplification and this can be expressed as [14]:
𝑃𝑅(π‘˜) =
πΈβ„Ž(π‘˜)
(1βˆ’π›Ό)𝑇/2
β‰œ
2πœ‚π›Όπ‘ƒπ‘ |β„Ž1(π‘˜)|
2
(1βˆ’π›Ό)𝑑1
πœ—1
(4)
Since the relays are fixed-gain AF nodes, the equivalent end-to-end instantaneous SNR at the destination for
the system can be approximately expressed by following the same approach in [11] as:
π›Ύπ‘’π‘ž =
πœ™π›ΎΜƒ1(π‘˜) 𝛾2(π‘˜)
πœ“π›Ύ2(π‘˜)+1
(5)
where 𝛾̃1(π‘˜) = |β„Ž1(π‘˜)|
2
, 𝛾2(π‘˜) = |β„Ž2(π‘˜)|
2
, πœ“ =
2πœ‚π›Ό
(1βˆ’π›Ό)𝑑1
πœ—1
, and πœ™ =
2πœ‚π›Όπ›Ύ 𝑇
(1βˆ’π›Ό)𝑑1
πœ—1 𝑑1
πœ—2
for 𝛾 𝑇 denotes the average
transmit SNR.
In this study, the dual-hops links for the system are characterized by the Rayleigh fading and
the probability density function (PDF) for the distribution for the S-to-R link under the partial relay selection
system can be expressed as [11, 12]:
𝑓𝛾1(π‘˜)
(π‘₯) = π‘˜( 𝑁
π‘˜
) βˆ‘ ( π‘˜βˆ’1
𝑛
)π‘˜βˆ’1
𝑛=0
(βˆ’1) 𝑛
((π‘βˆ’π‘˜+𝑛)(1βˆ’πœŒ)+1)Ξ©1
(6)
Γ— 𝑒π‘₯𝑝 (βˆ’
(π‘βˆ’π‘˜+𝑝+1)π‘₯
((π‘βˆ’π‘˜+𝑛)(1βˆ’πœŒ)+1)Ξ©1
)
where 𝜌 is the channel correlation coefficient, Ξ©1 = 𝚬 [|β„Ž1(π‘˜)|
2
]
Also, the corresponding CDF can be obtained by integrating (6) as:
𝐹𝛾1(π‘˜)
(π‘₯) = 1 βˆ’ π‘˜( 𝑁
π‘˜
) βˆ‘ ( π‘˜βˆ’1
𝑛
)π‘˜βˆ’1
𝑛=0
(βˆ’1) 𝑛
((π‘βˆ’π‘˜+𝑛)+1)
(7)
Γ— 𝑒π‘₯𝑝 (βˆ’
(π‘βˆ’π‘˜+𝑛+1)π‘₯
((π‘βˆ’π‘˜+𝑛)(1βˆ’πœŒ)+1)Ξ©1
)
Int J Elec & Comp Eng ISSN: 2088-8708 
On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi)
5299
By the principle of TAS/MRC, the PDF for the R-to-D channel can be defined as [21]:
𝑓𝛾2
(π‘₯) =
𝑁 𝑅
𝑑
Ξ“(𝑁 𝐷)
βˆ‘ ( 𝑁 𝑅
𝑑
βˆ’1
𝑝
) (βˆ’1) 𝑝𝑁 𝑅
𝑑
βˆ’1
𝑝=0 𝑒π‘₯𝑝 (βˆ’
(𝑝+1)π‘₯
Ξ©2
) ∏ [βˆ‘ (
𝑗 π‘žβˆ’1
𝑗 π‘ž
)
𝑗 π‘žβˆ’1
𝑗 π‘ž=0
(
1
π‘ž!
)
𝑗 π‘žβˆ’π‘— π‘ž+1
] Ξ©2
βˆ’πœ‰
π‘₯ πœ‰βˆ’1𝑁 π·βˆ’1
π‘ž=1 (8)
where
{
πœ‰ = π›½π‘ž + 𝑁 𝐷,
π›½π‘ž = βˆ‘ 𝑗 π‘ž
𝑁 π·βˆ’1
π‘ž=1 ,
𝑗0 = 𝑝, 𝑗 𝑁 𝐷
= 0, and
Ξ©2 = 𝚬 [|β„Ž2(π‘˜)|
2
]
(9)
Figure 1: (a) Partial relay selection system model with energy harvesting
(b) TSR protocol for power and information transfer at the relay
3. STATISTICAL CHARACTERISTICS
The CDF of the equivalent end-to-end instantaneous SNR at the destination for the concerned
system can be expressed as [15]:
πΉπ‘’π‘ž(𝛾) = π‘ƒπ‘Ÿ [𝛾1 <
πœ“π›Ύπ›Ύ2+𝛾
πœ™π›Ύ1
| 𝛾2 > 0] (10)
β‰œ ∫ 𝐹𝛾1
(
πœ“π›Ύπ›Ύ2+𝛾
πœ™π›Ύ2
) 𝑓𝛾2
(𝛾2)𝑑𝛾2
∞
0
By substituting (7) and (8) into (10), the equivalent end-to-end instantaneous SNR for the system can be
expressed as:
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 5, October 2020 : 5296 - 5305
5300
πΉπ‘’π‘ž(𝛾) = 1 βˆ’
π‘˜π‘ 𝑅
𝑑
Ξ“(𝑁 𝐷)
βˆ‘ βˆ‘ ( 𝑁
π‘˜
)( π‘˜βˆ’1
𝑛
) ( 𝑁 𝑅
𝑑
βˆ’1
𝑝
) Ξ©2
βˆ’πœ‰π‘ 𝑅
𝑑
βˆ’1
𝑝=0
π‘˜βˆ’1
𝑛=0
(βˆ’1) 𝑛+𝑝
((π‘βˆ’π‘˜+𝑛)+1)
𝑒π‘₯𝑝 (βˆ’
Ξ”πœ“π›Ύ
πœ™Ξ©1
) (11)
Γ— ∏ [βˆ‘ (
𝑗 π‘žβˆ’1
𝑗 π‘ž
)
𝑗 π‘žβˆ’1
𝑗 π‘ž=0
(
1
π‘ž!
)
𝑗 π‘žβˆ’π‘— π‘ž+1
]
𝑁 π·βˆ’1
π‘ž=1 ∫ 𝛾2
πœ‰βˆ’1
𝑒π‘₯𝑝 (βˆ’
(𝑝+1)𝛾2
Ξ©2
) 𝑒π‘₯𝑝 (βˆ’
μ𝛾
πœ™Ξ©1 𝛾2
) 𝑑𝛾2
∞
0
where
ΞΌ =
(π‘βˆ’π‘˜+𝑛+1)𝛾
((π‘βˆ’π‘˜+𝑛)(1βˆ’πœŒ)+1)
By converting the 𝑒π‘₯𝑝 (βˆ’
μ𝛾
πœ™Ξ©1 𝛾2
) to Meijer-G function form using the identity defined [22, (11)] and
invert the function using the identity detailed in [23 (8.2.2(14)], then the integral part of (10) can be
expressed as:
𝑣1 = ∫ 𝛾2
πœ‰βˆ’1
𝑒π‘₯𝑝 (βˆ’
(𝑝+1)𝛾 𝑅𝐷
Ξ© 𝑅𝐷
) 𝐺1,0
0,1
(
πœ™Ξ©2 𝛾2
ΞΌΞ³
|
1
βˆ’
) 𝑑𝛾2
∞
0
(12)
By utilizing the integral identity defined in [24, (7.813(1))], the (12) can be solved as:
𝑣1 = (
Ξ©2
(𝑝+1)
)
πœ‰
𝐺2,0
0,2
(
πœ™Ξ©1 𝛾2
ΞΌΞ³(𝑝+1)
|
1 βˆ’ πœ‰, 1
βˆ’
) (13)
By putting (13) into (11), then the equivalent end-to-end instantaneous SNR for the system can be obtained as:
πΉπ‘’π‘ž(𝛾) = 1 βˆ’
π‘˜π‘ 𝑅
𝑑
Ξ“(𝑁 𝐷)
βˆ‘ βˆ‘ ( 𝑁
π‘˜
)( π‘˜βˆ’1
𝑛
) ( 𝑁 𝑅
𝑑
βˆ’1
𝑝
) Ξ©2
βˆ’πœ‰π‘ 𝑅
𝑑
βˆ’1
𝑝=0
π‘˜βˆ’1
𝑛=0
(βˆ’1) 𝑛+𝑝
((π‘βˆ’π‘˜+𝑛)+1)
𝑒π‘₯𝑝 (βˆ’
ΞΌπœ“π›Ύ
πœ™Ξ©1
) Γ—
∏ [βˆ‘ (
𝑗 π‘žβˆ’1
𝑗 π‘ž
)
𝑗 π‘žβˆ’1
𝑗 π‘ž=0
(
1
π‘ž!
)
𝑗 π‘žβˆ’π‘— π‘ž+1
]
𝑁 π·βˆ’1
π‘ž=1 (
Ξ©2
(𝑝+1)
)
πœ‰
𝐺2,0
0,2
(
πœ™Ξ©1Ξ© 𝑅2
ΞΌΞ³(𝑝+1)
|
1 βˆ’ πœ‰, 1
βˆ’
) (14)
4. PERFORMANCE ANALYSIS
The performance analysis of the concerned system in terms of outage probability, ABER and
throughput are presented in this section.
4.1. Outage probability analysis
The outage probability is an important measure for evaluating the performance of a wireless systems over
fading channels. At a given transmission rate 𝑅 bits/s/Hz, the outage probability can be defined as [25, 26]:
π‘ƒπ‘œπ‘’π‘‘ = πΉπ‘’π‘ž(π›Ύπ‘‘β„Ž) (15)
where π›Ύπ‘‘β„Ž = 2 𝑅
βˆ’ 1 is the predetermined threshold SNR required to support the fixed transmission rate 𝑅 at
the source in delay-limited transmission mode.
By substituting (14) into (15), the system outage probability can be expressed as:
π‘ƒπ‘œπ‘’π‘‘ = 1 βˆ’
π‘˜π‘ 𝑅
𝑑
Ξ“(𝑁 𝐷)
βˆ‘ βˆ‘ ( 𝑁
π‘˜
)( π‘˜βˆ’1
𝑛
) ( 𝑁 𝑅
𝑑
βˆ’1
𝑝
) Ξ©2
βˆ’πœ‰π‘ 𝑅
𝑑
βˆ’1
𝑝=0
π‘˜βˆ’1
𝑛=0
(βˆ’1) 𝑛+𝑝
((π‘βˆ’π‘˜+𝑛)+1)
𝑒𝑒π‘₯𝑝 (βˆ’
ΞΌπœ“π›Ύ π‘‘β„Ž
πœ™Ξ©1
) Γ—
∏ [βˆ‘ (
𝑗 π‘žβˆ’1
𝑗 π‘ž
)
𝑗 π‘žβˆ’1
𝑗 π‘ž=0
(
1
π‘ž!
)
𝑗 π‘žβˆ’π‘— π‘ž+1
]
𝑁 π·βˆ’1
π‘ž=1 (
Ξ©2
(𝑝+1)
)
πœ‰
𝐺2,0
0,2
(
πœ™Ξ©1Ξ©2
μ𝛾 π‘‘β„Ž(𝑝+1)
|
1 βˆ’ πœ‰, 1
βˆ’
) (16)
4.2. Average bit error rate
In this section, the ABER for the system is derived under the BPSK modulation and the ABER for
the concerned system can be expressed as [15]:
𝑃𝑏 =
𝛿
2√2πœ‹
∫ πΉπ‘’π‘ž (
π‘₯
πœ”
)
∞
0
exp(βˆ’π‘₯/2)π‘₯βˆ’
1
2 𝑑π‘₯ (17)
where 𝛿 = 1 and πœ” = 2 for the BPSK modulation.
By substituting (11) into (17), the ABER for the system can be expressed as:
Int J Elec & Comp Eng ISSN: 2088-8708 
On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi)
5301
𝑃𝑏 =
𝛿
2√2πœ‹
[∫ exp(βˆ’π‘₯/2)π‘₯βˆ’1/2
𝑑π‘₯
∞
0
βˆ’ Ξ1 ∫ π‘₯βˆ’1/2
𝑒π‘₯𝑝 (βˆ’ (
ΞΌπœ“
πœ™πœ”Ξ©1
+
1
2
) 𝑑) 𝐺2,0
0,2
(
πœ™Ξ©1Ξ©2 πœ”
ΞΌ(𝑝 + 1)π‘₯
|
1 βˆ’ πœ‰, 1
βˆ’
) 𝑑π‘₯
∞
0
]
(18)
where
Ξ1 =
π‘˜π‘ 𝑅
𝑑
Ξ“(𝑁 𝐷)
βˆ‘ βˆ‘ ( 𝑁
π‘˜
)( π‘˜βˆ’1
𝑛
) ( 𝑁 𝑅
𝑑
βˆ’1
𝑝
) Ξ©2
βˆ’πœ‰π‘ 𝑅
𝑑
βˆ’1
𝑝=0
π‘˜βˆ’1
𝑛=0
(βˆ’1) 𝑛+𝑝
((π‘βˆ’π‘˜+𝑛)+1)
(19)
Γ— ∏ [βˆ‘ (
𝑗 π‘žβˆ’1
𝑗 π‘ž
)
𝑗 π‘žβˆ’1
𝑗 π‘ž=0
(
1
π‘ž!
)
𝑗 π‘žβˆ’π‘— π‘ž+1
]
𝑁 π·βˆ’1
π‘ž=1 (
Ξ©2
(𝑝+1)
)
πœ‰
The first integral part of (18) can be solve by using the integral identity detailed in [24, (3.326(2))]
and the second integral can be solved by inverting the Meijer-G function using the identity defined in
[23, (8.2.2 (14))] as:
𝑣3 = ∫ π‘₯βˆ’1/2
𝑒π‘₯𝑝 (βˆ’ (
ΞΌπœ“
πœ™πœ”Ξ©1
+
1
2
) 𝑑) 𝐺2,0
0,2
(
ΞΌ(𝑝+1)π‘₯
πœ™Ξ©1Ξ©2 πœ”
|
βˆ’
πœ‰, 0) 𝑑π‘₯
∞
0
(20)
Then, by using the integral identity defined in [24, (7.813(1))], the 𝑣3 can be solved as:
𝑣3 = (
2πœ™πœ”Ξ©1
2ΞΌπœ“+πœ™πœ”Ξ©1
)
1/2
𝐺0,2
2,0
(
2ΞΌ(𝑝+1)
Ξ©2(2ΞΌπœ“+πœ™πœ”Ξ©1)
|
1/2
πœ‰, 0
) (21)
Substituting 𝑣3 into (18), the ABER for the TAS/MRC can be expressed as:
𝑃𝑏 =
𝛿
2√2πœ‹
[
Ξ“(1/2)
√1/2
βˆ’
π‘˜π‘ 𝑅
𝑑
Ξ“(𝑁 𝐷)
βˆ‘ βˆ‘ ( 𝑁
π‘˜
)( π‘˜βˆ’1
𝑛
) ( 𝑁 𝑅
𝑑
βˆ’1
𝑝
) Ξ©2
βˆ’πœ‰π‘ 𝑅
𝑑
βˆ’1
𝑝=0
π‘˜βˆ’1
𝑛=0
(βˆ’1) 𝑛+𝑝
((π‘βˆ’π‘˜+𝑛)+1)
Γ—
∏ [βˆ‘ (
𝑗 π‘žβˆ’1
𝑗 π‘ž
)
𝑗 π‘žβˆ’1
𝑗 π‘ž=0
(
1
π‘ž!
)
𝑗 π‘žβˆ’π‘— π‘ž+1
]
𝑁 π·βˆ’1
π‘ž=1 (
Ξ©2
(𝑝+1)
)
πœ‰
(
2πœ™πœ”Ξ©1
2ΞΌπœ“+πœ™πœ”Ξ©1
)
1/2
𝐺0,2
2,0
(
2ΞΌ(𝑝+1)
Ξ©2(2ΞΌπœ“+πœ™πœ”Ξ©1)
|
1/2
πœ‰, 0
)] (22)
4.3. Throughput analysis
In this paper, the delay-limited transmission mode is employed for the concerned system and
the throughput is obtained by determining the outage probability of the system at a fixed source transmission
rate 𝑅 𝑏𝑖𝑑𝑠/𝑠/𝐻𝑧. Therefore, at a fixed transmission rate with effective communication time of (1 βˆ’ 𝛼)𝑇/2
from the source to destination, the throughput 𝜏 can be expressed as [7]:
𝜏 = (1 βˆ’ π‘ƒπ‘œπ‘’π‘‘)𝑅
(1βˆ’π›Ό)𝑇/2
𝑇
β‰œ
𝑅
2
(1 βˆ’ π‘ƒπ‘œπ‘’π‘‘)(1 βˆ’ 𝛼) (23)
By putting (16) into (23), the throughput for the concerned system can be expressed as:
𝜏 =
(1βˆ’π›Ό)π‘…π‘˜π‘ 𝑅
𝑑
2Ξ“(𝑁 𝐷)
βˆ‘ βˆ‘ ( 𝑁
π‘˜
)( π‘˜βˆ’1
𝑛
) ( 𝑁 𝑅
𝑑
βˆ’1
𝑝
) Ξ©2
βˆ’πœ‰π‘ 𝑅
𝑑
βˆ’1
𝑝=0
π‘˜βˆ’1
𝑛=0
(βˆ’1) 𝑛+𝑝
((π‘βˆ’π‘˜+𝑛)+1)
𝑒π‘₯𝑝 (βˆ’
ΞΌπœ“π›Ύ π‘‘β„Ž
πœ™Ξ©1
) Γ—
∏ [βˆ‘ (
𝑗 π‘žβˆ’1
𝑗 π‘ž
)
𝑗 π‘žβˆ’1
𝑗 π‘ž=0
(
1
π‘ž!
)
𝑗 π‘žβˆ’π‘— π‘ž+1
]
𝑁 π·βˆ’1
π‘ž=1 (
Ξ©2
(𝑝+1)
)
πœ‰
𝐺2,0
0,2
(
πœ™Ξ©1Ξ©2
Δ𝛾 π‘‘β„Ž(𝑝+1)
|
1 βˆ’ πœ‰, 1
βˆ’
) (24)
5. NUMERICAL RESULTS AND DISCUSSIONS
In this section, the numerical results for the system outage probability, ABER, and throughput are
presented based on the derived analytical closed form expression presented in (16), (22), and (24)
respectively. Unless specified, the system parameters adopted are set to be: 𝑅 = 2 𝑏𝑖𝑑𝑠/𝑠/𝐻𝑧, Ξ©1 = 1,
Ξ©2 = 1, πœ‚ = 1, πœ—1 = 2, πœ—2 = 3, and 𝛾 𝑇 = 20𝑑𝐡. Two selection scenarios are considered as follows: worst
relay selection when π‘˜ = 1 and best relay selection when π‘˜ = 𝑁
In Figure 2, the effect of S-to-R distance on the concerned system under different relay selection
scenarios is demonstrated The result shows that as 𝑑1 increases, both the energy harvested and received
signal at the relay nodes become weaker causing the system outage probability to be degraded. However,
beyond an optimum distance of 𝑑1 where the distance between the relay and destination becomes smaller,
the system outage probability starts decreasing even with less transmit power for the relay to transmit
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 5, October 2020 : 5296 - 5305
5302
information. Irrespective of this, the best relay selection offers the system better performance than the worst
relay selection.
The outage performance of the concerned system under different values of channel correlation
coefficient at different relay distant is illustrated in Figure 3. The results show that as the transmit SNR
increase the better the system outage probability. In addition, it can be depicted that the increase in
correlation coefficient the better the system outage performance. However, the as the relays location far from
the source, the worse the outage performance becomes due to less transmit power received at the relay node
for information transmission. The results also indicated the simulation result perfectly match with
the analytical result which proves the correctness of our derived expressions.
The effect of channel correlation coefficient on the ABER of the system is illustrated in Figure 4
under different number of antenna at the destination. It can be clearly seen that increase in the number of
destination antenna leads to reduction in the system error performance. It is also depicted from the results that
the higher the channel correlation the better the system performance. The results also indicate that
the analytical results are well agreed with the simulation results which shows the accuracy of our derivation.
The error performance as a function of energy harvesting time is presented in Figure 5 under number
of relay selection. It can be shown that as the energy harvesting time increases the better the system error
performance. This is owing to the large amount of time available for relay nodes to replenished energy for
information transmission. Also, the increase in the number of relay selection for transmission significantly
improves the system error performance.
Figure 2. Outage probability vs the S-to-R distance
under different number of 𝑁 𝐷 at 𝛼 = 0.5,
𝜌 = 0.6, and 𝑑2 = 6 βˆ’ 𝑑1
Figure 3. Effect of correlation coefficient on
the system outage probability under
different S-to-R distance
Figure 4. Impact of number of antenna at the
destination 𝑁 𝐷 on the system ABER under different
correlation coefficients at 𝛼 = 0.6, π‘˜ = 𝑁 = 4
Figure 5. ABER performance of the system
under different relay selection at
𝑁 = 4, 𝜌 = 0.6, 𝑁 𝐷 = 2, 𝑁𝑅
𝑑
= 2
Int J Elec & Comp Eng ISSN: 2088-8708 
On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi)
5303
In Figure 6, the throughput performance of the system as a function of energy harvesting time is
depicted under different average transmit SNR. The results show that the increase in the source transmit
power, the higher the system throughput because larger energy is harvested at relay nodes. It can be deduced
from the results that, at high transmit power, the optimum time is very short for energy harvesting and large
time is used to decode information. Compare with the lower transmit power. The analytical results are
perfectly matched with the simulation results showing the accuracy of the derived expression.
The throughput as a function of relay distance from the source under different number of antenna at
the destination is demonstrated in Figure 7. The results indicate that the system performance is significantly
improved with the increase in the number of antenna at the destination. It can be seen from the results that at
small values 𝑑1, the system throughput becomes degraded due to larger distance between the relay and
the destination, and the outage probability is high at the regime. Thus, at the optimum relay location,
the system performance starts increasing snice the smaller value of 𝑑2 result into higher system throughput
with better system outage. As expected, the results depict that the system has better performance under
the best relay selection compare with worst relay selection.
The throughput performance of the system at different channel correlation coefficient and 𝑁 𝐷 is
depicted in Figure 8. It can be seen from the results that higher throughput performance can be achieved with
the best relay selection at high SNR. At low and high SNR, the throughput becomes saturated which shows
that the outage probability has higher and lower values respectively. In addition, the results also prove that
increase in the correlation coefficient significantly improve the system performance. The simulation results
perfect matched with the analytical results which indicate the correctness of our derivation.
Figure 6. Throughput versus the energy harvesting time under different average transmit SNR at 𝜌 = 0.6,
𝑁 𝐷 = 2, 𝑁𝑅
𝑑
= 4, π‘˜ = 𝑁 = 4
Figure 7. Effect of S-to-R distance on the system
throughput under different number of 𝑁 𝐷 for
different relay selection scenarios when
𝛼 = 0.2, 𝜌 = 0.6, and 𝑑2 = 6 βˆ’ 𝑑1
Figure 8. Performance system throughput under
different correlation coefficient and 𝑁 𝐷 when
𝛼 = 0.2 at π‘˜ = 𝑁 = 4
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 5, October 2020 : 5296 - 5305
5304
6. CONCLUSION
The performance of energy harvesting based PRS cooperative system with TAS and outdated
channel state is presented. Based on the TS protocol, the analytical closed form expression for the system
outage probability and ABER are obtained. Through the outage probability, the system throughput for
delay-limited transmission mode is determined. These exact expressions are verified by the Monte Carlo
simulation. The results illustrated that the increase in channel coefficient significantly improve the system
performance. In addition, the system offers better performance with the increase in number of the destination
receive antenna. Also, the result shows that system outage probability, ABER and throughput performance
improved with increasing the number of relays or the values of the correlation coefficient.
REFERENCES
[1] K. Zhu, F. Wang, S. Li, F. Jiang, and L. Cao, "Relay Selection for Cooperative Relaying in Wireless Energy
Harvesting Networks," Proceedings of IOP Conference Series: Earth and Environmental Science, vol. 108,
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[2] Y. Gu and S. AΓ―ssa, "RF-based energy harvesting in decode-and-forward relaying systems: Ergodic and outage
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[4] A. Andrawes, R. Nordin, and M. J. E. Ismail, "Wireless Energy Harvesting with Cooperative Relaying under the
Best Relay Selection Scheme," Energies, vol. 12, no. 5, pp. 1-22, 2019.
[5] C. Zhong, H. A. Suraweera, G. Zheng, I. Krikidis, and Z. Zhang, "Wireless information and power transfer with
full duplex relaying," IEEE Transactions on Communications, vol. 62, no. 10, pp. 3447-3461, 2014.
[6] K.-H. Liu and Te-Lin Kung, "Performance improvement for RF energy-harvesting relays via relay selection,"
IEEE Transactions on Vehicular Technology, vol. 66, no. 9, pp. 8482-8494, 2017.
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information processing," IEEE Transactions on Wireless Communications, vol. 12, no. 7, pp. 3622-3636, 2013.
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Relay Selection over Nakagami-m Fading Channels," Proceedings of International Conference on Industrial
Networks and Intelligent Systems, pp. 100-110, 2017.
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On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi)
5305
[21] N. Yang, P. L. Yeoh, M. Elkashlan, R. Schober, and I. B. Collings, "Transmit antenna selection for
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algebraic computation, pp. 212-224, 1990.
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and Breach science publishers, 1986.
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networks with different antenna selection schemes," IEEE Access, vol. 6, pp. 5654-5665, 2018.
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BIOGRAPHIES OF AUTHORS
Kehinde Oluwasesan Odeyemi received his B.Tech. degree in Electronic Engineering from
Ladoke Akintola University of Technology Ogbomosho, Oyo State, Nigeria, in 2008. He later
obtained an M.Eng. Degree in the same field from the Federal University of Technology,
Akure in 2012. He received his Ph.D. degree in Electronic Engineering at the University of
KwaZulu-Natal, Durban, South Africa in 2018. In 2012, he joined the department of Electrical
and Electronic Engineering, University of Ibadan, Nigeria. He is a member of The Council for
the Regulation of Engineering in Nigeria (COREN). He has written several research articles
and his research interests are in the antenna design, optical wireless communications, diversity
combining techniques and MIMO systems.
Pius Adewale Owolawi received his B.Tech. degree in Physics/Electronics from the Federal
University of Technology, Akure, in 2001. He then obtained a M.Sc. and Ph.D. degrees in
Electronic Engineering from the University of KwaZulu-Natal in 2006 and 2010, respectively.
He holds several industry certifications such as CCNA, CCNP, CWNP, CFOA, CFOS/D and
MCITP. Member of several professional bodies like SAIEE, IEEE, and SA AMSAT. In 2007,
he joined the faculty of the Engineering, Department of Electrical Engineering at Mangosuthu
University of Technology, South Africa. Thereafter, in 2017, he joined the department of
Computer Systems Engineering, Tshwane University of Technology, Pretoria, South Africa
where is currently the head of department. His research interests are in the computational of
Electromagnetic, modeling of radio wave propagation at high frequency, fiber optic
communication, radio planning and optimization techniques and renewable energy. He has
written several research articles and serves as a reviewer for many scientific journals.

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On the performance of energy harvesting AF partial relay selection with TAS and outdated channel state information over identical channels

  • 1. International Journal of Electrical and Computer Engineering (IJECE) Vol. 10, No. 5, October 2020, pp. 5296~5305 ISSN: 2088-8708, DOI: 10.11591/ijece.v10i5.pp5296-5305  5296 Journal homepage: http://ijece.iaescore.com/index.php/IJECE On the performance of energy harvesting AF partial relay selection with TAS and outdated channel state information over identical channels Kehinde O. Odeyemi1 , Pius A. Owolawi2 1 Department of Electrical and Electronic Engineering, Faculty of Technology, University of Ibadan, Nigeria 2 Department of Computer Systems Engineering, Tshwane University of Technology, South Africa Article Info ABSTRACT Article history: Received Apr 27, 2019 Revised Apr 7, 2020 Accepted Apr 20, 2020 Energy scarcity has been known to be one of the most noticeable challenges in wireless communication system. In this paper, the performance of an energy harvesting based partial relay selection (PRS) cooperative system with transmit antenna selection (TAS) and outdated channel state information (CSI) is investigated. The system dual-hops links are assumed to follow Rayleigh distribution and the relay selection is based on outdated CSI of the first link. To realize the benefit of multiple antenna, the amplified-and- forward (AF) relay nodes then employs the TAS technique for signal transmission and signal reception is achieved at the destination through maximum ratio combining (MRC) scheme. Thus, the closed-form expression for the system equivalent end-to-end cumulative distribution function (CDF) is derived. Based on this, the analytical closed-form expressions for the outage probability, average bit error rate, and throughput for the delay- limited transmission mode are then obtained. The results illustrated that the energy harvesting time, relay distance, channel correlation coefficient, the number of relay transmit antennas and destination received antenna have significant effect on the system performance. Monte-carol simulation is employed to validate the accuracy of the derived expressions. Keywords: Channel state information Energy harvesting Maximum ratio combining Partial relay selection Transmit antenna selection Copyright Β© 2020 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Kehinde O. Odeyemi, Department of Electrical and Electronic Engineering, Factulty of Technology, University of Ibadan, Ibadan, Nigeria. Email: odeyemikenny@gmail.com 1. INTRODUCTION Traditionally, relay nodes within the wireless cooperative network are usually equipped with power- limited batteries that are infeasible, costly and even impossible to replace in some applications [1, 2]. As a result of this, energy harvesting (EH) has been considered as a promising solution to alleviate this stated energy constraint in wireless system. Therefore, research studies have suggested that batteries can be wirelessly recharge using external power sources from free ambient such as solar, wind, thermal and vibration [3]. These conventional sources are not always available and mostly suffers from time-varying problem and materials inefficiency [4, 5]. Based on this, RF source has been regarded as the best alternative means of harvesting energy in wireless communication since it carries both the energy and information at the same time without monitoring and maintenance [6]. In this case, two schemes have been suggested in literature through which energy can be harvested and this include time switching (TS) and power splitting (PS) protocols. In TS protocol, the transmission time is divided into two parts where the receiver nodes spend one to harvest energy from the source and the remaining for information transmission. In PS protocol on the other hand, the receiver nodes used part of the EH and the other for information processing [7].
  • 2. Int J Elec & Comp Eng ISSN: 2088-8708  On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi) 5297 The deployment of relays in wireless networks can extend the signal coverage and overcoming the channel impairment as a result of fading [8]. Therefore, two strategies have been suggested for relay to transmit its received signal to the destination for which include decode-and-forward (DF) and amplify-and- forward (AF) of relaying system [4, 9]. In DF relaying system, the received signal is fully decoded and the decoded copy is retransmitted to the destination. In AF relaying system on the other hand, the received signal is simply amplified and forwarded to the destination without decoding leading to its simplicity and effective implementation cost [10]. In the wireless cooperative system with multiple relays, numerous relay selection techniques have proposed [6] and this include the partial relay selection where selection of relays depends on the CSI of the source-relay links or relay-destination links. This thus avoids the issues such as high power consumption, overhead and network delays, and can also prolong the network lifetime [11, 12]. Unlike the best and opportunistic relay selection approaches, which require global knowledge of the CSI of each of the two hops [12, 13] leading to time synchronization, continuous channel feedback and high power consumption. Reducing the energy consumption of cooperative relaying system through the energy harvesting has drawn more attention in the research community has attracted attention in the research community. The performance of dual-hop relaying network with three different wireless EH mechanisms at the DF relay nodes over the generalized channels was studied [14]. In [15], the performance of a wireless information power transfer in AF relay network with multiple antenna over dissimilar channel and the benefit of MRC/TAS was exploit for the relay node was investigated. The Ergodic outage and capacity performance of wireless power transfer based AF relaying system was presented in [16]. Also, the performance of DF-based EH with the source node and the destination employing TAS and MRC respectively was evaluated in [17]. The throughput performance of an AF relay based EH under delay-tolerance and limited transmission modes was investigated in [7] over Rayleigh fading channels. However, all these aforementioned works are limited to a single relay-based EH cooperative systems. In case of multiple relay selection, the performance of EH cooperative system with optimal relay selection under the CSI and energy side information was investigated in [18]. In addition, incremental relay network with EH-based relay selection was proposed in [19] where the selected relay harvesting the largest source energy was chosen to forward the information to the destination. In [20], the performance of AF relaying energy harvesting system with π‘˜π‘‘β„Ž best PRS and energy beamforming over Nakagami-m was evaluated. In this work, it was assumed that both the source and the destination are multiple antenna nodes and the relay are single antenna nodes. In all these aforementioned studies, perfect CSI was assumed for the system. Motivated by this, the performance of the PRS-based EH system under the TAS/MRC is investigated in this paper where the relay nodes employ the TAS technique at the relay nodes and maximum ratio combining (MRC) scheme at the destination. The exact closed-form expression for the system outage probability and average bit error rate are obtained. Utilizing the outage probability, the throughput for the system is obtained based on delay-limited transmission mode. The impact of energy harvesting time, relay distance, channel correlation coefficient, the number of relay transmit antennas and destination received antenna on the concerned system are demonstrated. 2. SYSTEM AND CHANNEL MODEL In this paper, a dual-hops PRS based energy harvesting system with PRS and outdated CSI is presented in Figure 1 (a). The source (S) is equipped with a single transmit antenna and the destination (D) has multiple receive antenna 𝑁 𝐷. The relay (R) of 𝑁 nodes utilize a single receive antenna and multiple transmit antenna 𝑁𝑅 𝑑 . It is assumed that the S-to-R and R-to-D links undergo Rayleigh fading distribution without direct link between the source and the destination. The relay nodes employ TAS scheme to select the best antenna to forward the signal to the destination through which the instantaneous SNR at the destination is maximized. At the destination, MRC is used to combine the transmitted signal from the relay node(s). As a result of channel fast fading, it is considered that relay selection is based on outdated CSI. Thus, the instantaneous SNR of the first link and the one used for PRS are two correlated random variables with channel correlation coefficient 𝜌.The transmission over the links is assumed to be in half-duplex mode so as to avoid inter-signal interference. Therefore, the overall systems communication is established in two different phases. During the first phase, the communication between the S and R nodes is divided into power transmission and information transmission as presented in Figure 1(b). Based on this, the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) harvest the energy and then receive the information from the source using the time switching-base relay (TSR) protocol. Thereafter, the source information is amplified through AF relaying and then convey to the destination using TAS technique. In TSR protocol, a total block time slot of 𝑇 is divided into three parts: for energy harvesting as 𝛼𝑇, information transmission between S-to-R as (1 βˆ’ 𝛼)𝑇/2 and information
  • 3.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 5, October 2020 : 5296 - 5305 5298 transmission between R-to-D as (1 βˆ’ 𝛼)𝑇/2. The parameter 𝛼 denotes the energy having time factor at 0 ≀ 𝛼 ≀ 1. Thus, the receive signal by the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) can be expressed as: 𝑦1(π‘˜)(𝑑) = √ 𝑃𝑠 𝑑1 πœ—1 β„Ž1(π‘˜) π‘₯(𝑑) + 𝑛 𝑅(π‘˜)(𝑑) (1) where 𝑃𝑠 is the source transmitted power, β„Ž1(π‘˜) is π‘˜ βˆ’ π‘‘β„Ž the channel gain, 𝑑1 is the distance between the source and the relay, πœ—1 denotes the path loss exponent, π‘₯(𝑑) represents the sources information and 𝑛 𝑅(π‘˜) is the AWGN at the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) with zero mean and variance 𝜎1 2 . The energy harvested by an energy receiver at the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) over the time 𝛼𝑇 can be expressed as [1, 11]: πΈβ„Ž,π‘˜ = πœ‚π›Όπ‘‡|β„Ž1(π‘˜)| 2 𝑑1 πœ—1 (2) where 0 ≀ πœ‚ ≀ 1 denotes the energy harvesting efficiency which depends on the rectification process and the circuitry. During the second phase, the remaining time slot of (1 βˆ’ 𝛼)𝑇/2 duration is then used by the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) to amplifies and retransmit the information to the destination using TAS principle. The destination thus employs MRC technique to combine the transmitted signal from the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) and the received signal can be expressed as: 𝑦2(𝑑) = √ 𝑃 𝑅(π‘˜) 𝑑2 πœ—2 β„Ž2(π‘˜) π‘₯Μ‚(𝑑) + 𝑛 𝐷(𝑑) (3) where β„Ž2(π‘˜) the channel gain, 𝑑2 is the distance between the relay and destination, πœ—2 denotes the path loss exponent, π‘₯Μ‚(𝑑) represents the decoded information of π‘₯(𝑑), 𝑛 𝐷 is the AWGN at the destination with zero mean and variance 𝜎2 2 , and 𝑃𝑅(π‘˜) is the π‘˜ βˆ’ π‘‘β„Ž selected relay(s) transmit power obtained from energy harvesting for relaying amplification and this can be expressed as [14]: 𝑃𝑅(π‘˜) = πΈβ„Ž(π‘˜) (1βˆ’π›Ό)𝑇/2 β‰œ 2πœ‚π›Όπ‘ƒπ‘ |β„Ž1(π‘˜)| 2 (1βˆ’π›Ό)𝑑1 πœ—1 (4) Since the relays are fixed-gain AF nodes, the equivalent end-to-end instantaneous SNR at the destination for the system can be approximately expressed by following the same approach in [11] as: π›Ύπ‘’π‘ž = πœ™π›ΎΜƒ1(π‘˜) 𝛾2(π‘˜) πœ“π›Ύ2(π‘˜)+1 (5) where 𝛾̃1(π‘˜) = |β„Ž1(π‘˜)| 2 , 𝛾2(π‘˜) = |β„Ž2(π‘˜)| 2 , πœ“ = 2πœ‚π›Ό (1βˆ’π›Ό)𝑑1 πœ—1 , and πœ™ = 2πœ‚π›Όπ›Ύ 𝑇 (1βˆ’π›Ό)𝑑1 πœ—1 𝑑1 πœ—2 for 𝛾 𝑇 denotes the average transmit SNR. In this study, the dual-hops links for the system are characterized by the Rayleigh fading and the probability density function (PDF) for the distribution for the S-to-R link under the partial relay selection system can be expressed as [11, 12]: 𝑓𝛾1(π‘˜) (π‘₯) = π‘˜( 𝑁 π‘˜ ) βˆ‘ ( π‘˜βˆ’1 𝑛 )π‘˜βˆ’1 𝑛=0 (βˆ’1) 𝑛 ((π‘βˆ’π‘˜+𝑛)(1βˆ’πœŒ)+1)Ξ©1 (6) Γ— 𝑒π‘₯𝑝 (βˆ’ (π‘βˆ’π‘˜+𝑝+1)π‘₯ ((π‘βˆ’π‘˜+𝑛)(1βˆ’πœŒ)+1)Ξ©1 ) where 𝜌 is the channel correlation coefficient, Ξ©1 = 𝚬 [|β„Ž1(π‘˜)| 2 ] Also, the corresponding CDF can be obtained by integrating (6) as: 𝐹𝛾1(π‘˜) (π‘₯) = 1 βˆ’ π‘˜( 𝑁 π‘˜ ) βˆ‘ ( π‘˜βˆ’1 𝑛 )π‘˜βˆ’1 𝑛=0 (βˆ’1) 𝑛 ((π‘βˆ’π‘˜+𝑛)+1) (7) Γ— 𝑒π‘₯𝑝 (βˆ’ (π‘βˆ’π‘˜+𝑛+1)π‘₯ ((π‘βˆ’π‘˜+𝑛)(1βˆ’πœŒ)+1)Ξ©1 )
  • 4. Int J Elec & Comp Eng ISSN: 2088-8708  On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi) 5299 By the principle of TAS/MRC, the PDF for the R-to-D channel can be defined as [21]: 𝑓𝛾2 (π‘₯) = 𝑁 𝑅 𝑑 Ξ“(𝑁 𝐷) βˆ‘ ( 𝑁 𝑅 𝑑 βˆ’1 𝑝 ) (βˆ’1) 𝑝𝑁 𝑅 𝑑 βˆ’1 𝑝=0 𝑒π‘₯𝑝 (βˆ’ (𝑝+1)π‘₯ Ξ©2 ) ∏ [βˆ‘ ( 𝑗 π‘žβˆ’1 𝑗 π‘ž ) 𝑗 π‘žβˆ’1 𝑗 π‘ž=0 ( 1 π‘ž! ) 𝑗 π‘žβˆ’π‘— π‘ž+1 ] Ξ©2 βˆ’πœ‰ π‘₯ πœ‰βˆ’1𝑁 π·βˆ’1 π‘ž=1 (8) where { πœ‰ = π›½π‘ž + 𝑁 𝐷, π›½π‘ž = βˆ‘ 𝑗 π‘ž 𝑁 π·βˆ’1 π‘ž=1 , 𝑗0 = 𝑝, 𝑗 𝑁 𝐷 = 0, and Ξ©2 = 𝚬 [|β„Ž2(π‘˜)| 2 ] (9) Figure 1: (a) Partial relay selection system model with energy harvesting (b) TSR protocol for power and information transfer at the relay 3. STATISTICAL CHARACTERISTICS The CDF of the equivalent end-to-end instantaneous SNR at the destination for the concerned system can be expressed as [15]: πΉπ‘’π‘ž(𝛾) = π‘ƒπ‘Ÿ [𝛾1 < πœ“π›Ύπ›Ύ2+𝛾 πœ™π›Ύ1 | 𝛾2 > 0] (10) β‰œ ∫ 𝐹𝛾1 ( πœ“π›Ύπ›Ύ2+𝛾 πœ™π›Ύ2 ) 𝑓𝛾2 (𝛾2)𝑑𝛾2 ∞ 0 By substituting (7) and (8) into (10), the equivalent end-to-end instantaneous SNR for the system can be expressed as:
  • 5.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 5, October 2020 : 5296 - 5305 5300 πΉπ‘’π‘ž(𝛾) = 1 βˆ’ π‘˜π‘ 𝑅 𝑑 Ξ“(𝑁 𝐷) βˆ‘ βˆ‘ ( 𝑁 π‘˜ )( π‘˜βˆ’1 𝑛 ) ( 𝑁 𝑅 𝑑 βˆ’1 𝑝 ) Ξ©2 βˆ’πœ‰π‘ 𝑅 𝑑 βˆ’1 𝑝=0 π‘˜βˆ’1 𝑛=0 (βˆ’1) 𝑛+𝑝 ((π‘βˆ’π‘˜+𝑛)+1) 𝑒π‘₯𝑝 (βˆ’ Ξ”πœ“π›Ύ πœ™Ξ©1 ) (11) Γ— ∏ [βˆ‘ ( 𝑗 π‘žβˆ’1 𝑗 π‘ž ) 𝑗 π‘žβˆ’1 𝑗 π‘ž=0 ( 1 π‘ž! ) 𝑗 π‘žβˆ’π‘— π‘ž+1 ] 𝑁 π·βˆ’1 π‘ž=1 ∫ 𝛾2 πœ‰βˆ’1 𝑒π‘₯𝑝 (βˆ’ (𝑝+1)𝛾2 Ξ©2 ) 𝑒π‘₯𝑝 (βˆ’ μ𝛾 πœ™Ξ©1 𝛾2 ) 𝑑𝛾2 ∞ 0 where ΞΌ = (π‘βˆ’π‘˜+𝑛+1)𝛾 ((π‘βˆ’π‘˜+𝑛)(1βˆ’πœŒ)+1) By converting the 𝑒π‘₯𝑝 (βˆ’ μ𝛾 πœ™Ξ©1 𝛾2 ) to Meijer-G function form using the identity defined [22, (11)] and invert the function using the identity detailed in [23 (8.2.2(14)], then the integral part of (10) can be expressed as: 𝑣1 = ∫ 𝛾2 πœ‰βˆ’1 𝑒π‘₯𝑝 (βˆ’ (𝑝+1)𝛾 𝑅𝐷 Ξ© 𝑅𝐷 ) 𝐺1,0 0,1 ( πœ™Ξ©2 𝛾2 ΞΌΞ³ | 1 βˆ’ ) 𝑑𝛾2 ∞ 0 (12) By utilizing the integral identity defined in [24, (7.813(1))], the (12) can be solved as: 𝑣1 = ( Ξ©2 (𝑝+1) ) πœ‰ 𝐺2,0 0,2 ( πœ™Ξ©1 𝛾2 ΞΌΞ³(𝑝+1) | 1 βˆ’ πœ‰, 1 βˆ’ ) (13) By putting (13) into (11), then the equivalent end-to-end instantaneous SNR for the system can be obtained as: πΉπ‘’π‘ž(𝛾) = 1 βˆ’ π‘˜π‘ 𝑅 𝑑 Ξ“(𝑁 𝐷) βˆ‘ βˆ‘ ( 𝑁 π‘˜ )( π‘˜βˆ’1 𝑛 ) ( 𝑁 𝑅 𝑑 βˆ’1 𝑝 ) Ξ©2 βˆ’πœ‰π‘ 𝑅 𝑑 βˆ’1 𝑝=0 π‘˜βˆ’1 𝑛=0 (βˆ’1) 𝑛+𝑝 ((π‘βˆ’π‘˜+𝑛)+1) 𝑒π‘₯𝑝 (βˆ’ ΞΌπœ“π›Ύ πœ™Ξ©1 ) Γ— ∏ [βˆ‘ ( 𝑗 π‘žβˆ’1 𝑗 π‘ž ) 𝑗 π‘žβˆ’1 𝑗 π‘ž=0 ( 1 π‘ž! ) 𝑗 π‘žβˆ’π‘— π‘ž+1 ] 𝑁 π·βˆ’1 π‘ž=1 ( Ξ©2 (𝑝+1) ) πœ‰ 𝐺2,0 0,2 ( πœ™Ξ©1Ξ© 𝑅2 ΞΌΞ³(𝑝+1) | 1 βˆ’ πœ‰, 1 βˆ’ ) (14) 4. PERFORMANCE ANALYSIS The performance analysis of the concerned system in terms of outage probability, ABER and throughput are presented in this section. 4.1. Outage probability analysis The outage probability is an important measure for evaluating the performance of a wireless systems over fading channels. At a given transmission rate 𝑅 bits/s/Hz, the outage probability can be defined as [25, 26]: π‘ƒπ‘œπ‘’π‘‘ = πΉπ‘’π‘ž(π›Ύπ‘‘β„Ž) (15) where π›Ύπ‘‘β„Ž = 2 𝑅 βˆ’ 1 is the predetermined threshold SNR required to support the fixed transmission rate 𝑅 at the source in delay-limited transmission mode. By substituting (14) into (15), the system outage probability can be expressed as: π‘ƒπ‘œπ‘’π‘‘ = 1 βˆ’ π‘˜π‘ 𝑅 𝑑 Ξ“(𝑁 𝐷) βˆ‘ βˆ‘ ( 𝑁 π‘˜ )( π‘˜βˆ’1 𝑛 ) ( 𝑁 𝑅 𝑑 βˆ’1 𝑝 ) Ξ©2 βˆ’πœ‰π‘ 𝑅 𝑑 βˆ’1 𝑝=0 π‘˜βˆ’1 𝑛=0 (βˆ’1) 𝑛+𝑝 ((π‘βˆ’π‘˜+𝑛)+1) 𝑒𝑒π‘₯𝑝 (βˆ’ ΞΌπœ“π›Ύ π‘‘β„Ž πœ™Ξ©1 ) Γ— ∏ [βˆ‘ ( 𝑗 π‘žβˆ’1 𝑗 π‘ž ) 𝑗 π‘žβˆ’1 𝑗 π‘ž=0 ( 1 π‘ž! ) 𝑗 π‘žβˆ’π‘— π‘ž+1 ] 𝑁 π·βˆ’1 π‘ž=1 ( Ξ©2 (𝑝+1) ) πœ‰ 𝐺2,0 0,2 ( πœ™Ξ©1Ξ©2 μ𝛾 π‘‘β„Ž(𝑝+1) | 1 βˆ’ πœ‰, 1 βˆ’ ) (16) 4.2. Average bit error rate In this section, the ABER for the system is derived under the BPSK modulation and the ABER for the concerned system can be expressed as [15]: 𝑃𝑏 = 𝛿 2√2πœ‹ ∫ πΉπ‘’π‘ž ( π‘₯ πœ” ) ∞ 0 exp(βˆ’π‘₯/2)π‘₯βˆ’ 1 2 𝑑π‘₯ (17) where 𝛿 = 1 and πœ” = 2 for the BPSK modulation. By substituting (11) into (17), the ABER for the system can be expressed as:
  • 6. Int J Elec & Comp Eng ISSN: 2088-8708  On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi) 5301 𝑃𝑏 = 𝛿 2√2πœ‹ [∫ exp(βˆ’π‘₯/2)π‘₯βˆ’1/2 𝑑π‘₯ ∞ 0 βˆ’ Ξ1 ∫ π‘₯βˆ’1/2 𝑒π‘₯𝑝 (βˆ’ ( ΞΌπœ“ πœ™πœ”Ξ©1 + 1 2 ) 𝑑) 𝐺2,0 0,2 ( πœ™Ξ©1Ξ©2 πœ” ΞΌ(𝑝 + 1)π‘₯ | 1 βˆ’ πœ‰, 1 βˆ’ ) 𝑑π‘₯ ∞ 0 ] (18) where Ξ1 = π‘˜π‘ 𝑅 𝑑 Ξ“(𝑁 𝐷) βˆ‘ βˆ‘ ( 𝑁 π‘˜ )( π‘˜βˆ’1 𝑛 ) ( 𝑁 𝑅 𝑑 βˆ’1 𝑝 ) Ξ©2 βˆ’πœ‰π‘ 𝑅 𝑑 βˆ’1 𝑝=0 π‘˜βˆ’1 𝑛=0 (βˆ’1) 𝑛+𝑝 ((π‘βˆ’π‘˜+𝑛)+1) (19) Γ— ∏ [βˆ‘ ( 𝑗 π‘žβˆ’1 𝑗 π‘ž ) 𝑗 π‘žβˆ’1 𝑗 π‘ž=0 ( 1 π‘ž! ) 𝑗 π‘žβˆ’π‘— π‘ž+1 ] 𝑁 π·βˆ’1 π‘ž=1 ( Ξ©2 (𝑝+1) ) πœ‰ The first integral part of (18) can be solve by using the integral identity detailed in [24, (3.326(2))] and the second integral can be solved by inverting the Meijer-G function using the identity defined in [23, (8.2.2 (14))] as: 𝑣3 = ∫ π‘₯βˆ’1/2 𝑒π‘₯𝑝 (βˆ’ ( ΞΌπœ“ πœ™πœ”Ξ©1 + 1 2 ) 𝑑) 𝐺2,0 0,2 ( ΞΌ(𝑝+1)π‘₯ πœ™Ξ©1Ξ©2 πœ” | βˆ’ πœ‰, 0) 𝑑π‘₯ ∞ 0 (20) Then, by using the integral identity defined in [24, (7.813(1))], the 𝑣3 can be solved as: 𝑣3 = ( 2πœ™πœ”Ξ©1 2ΞΌπœ“+πœ™πœ”Ξ©1 ) 1/2 𝐺0,2 2,0 ( 2ΞΌ(𝑝+1) Ξ©2(2ΞΌπœ“+πœ™πœ”Ξ©1) | 1/2 πœ‰, 0 ) (21) Substituting 𝑣3 into (18), the ABER for the TAS/MRC can be expressed as: 𝑃𝑏 = 𝛿 2√2πœ‹ [ Ξ“(1/2) √1/2 βˆ’ π‘˜π‘ 𝑅 𝑑 Ξ“(𝑁 𝐷) βˆ‘ βˆ‘ ( 𝑁 π‘˜ )( π‘˜βˆ’1 𝑛 ) ( 𝑁 𝑅 𝑑 βˆ’1 𝑝 ) Ξ©2 βˆ’πœ‰π‘ 𝑅 𝑑 βˆ’1 𝑝=0 π‘˜βˆ’1 𝑛=0 (βˆ’1) 𝑛+𝑝 ((π‘βˆ’π‘˜+𝑛)+1) Γ— ∏ [βˆ‘ ( 𝑗 π‘žβˆ’1 𝑗 π‘ž ) 𝑗 π‘žβˆ’1 𝑗 π‘ž=0 ( 1 π‘ž! ) 𝑗 π‘žβˆ’π‘— π‘ž+1 ] 𝑁 π·βˆ’1 π‘ž=1 ( Ξ©2 (𝑝+1) ) πœ‰ ( 2πœ™πœ”Ξ©1 2ΞΌπœ“+πœ™πœ”Ξ©1 ) 1/2 𝐺0,2 2,0 ( 2ΞΌ(𝑝+1) Ξ©2(2ΞΌπœ“+πœ™πœ”Ξ©1) | 1/2 πœ‰, 0 )] (22) 4.3. Throughput analysis In this paper, the delay-limited transmission mode is employed for the concerned system and the throughput is obtained by determining the outage probability of the system at a fixed source transmission rate 𝑅 𝑏𝑖𝑑𝑠/𝑠/𝐻𝑧. Therefore, at a fixed transmission rate with effective communication time of (1 βˆ’ 𝛼)𝑇/2 from the source to destination, the throughput 𝜏 can be expressed as [7]: 𝜏 = (1 βˆ’ π‘ƒπ‘œπ‘’π‘‘)𝑅 (1βˆ’π›Ό)𝑇/2 𝑇 β‰œ 𝑅 2 (1 βˆ’ π‘ƒπ‘œπ‘’π‘‘)(1 βˆ’ 𝛼) (23) By putting (16) into (23), the throughput for the concerned system can be expressed as: 𝜏 = (1βˆ’π›Ό)π‘…π‘˜π‘ 𝑅 𝑑 2Ξ“(𝑁 𝐷) βˆ‘ βˆ‘ ( 𝑁 π‘˜ )( π‘˜βˆ’1 𝑛 ) ( 𝑁 𝑅 𝑑 βˆ’1 𝑝 ) Ξ©2 βˆ’πœ‰π‘ 𝑅 𝑑 βˆ’1 𝑝=0 π‘˜βˆ’1 𝑛=0 (βˆ’1) 𝑛+𝑝 ((π‘βˆ’π‘˜+𝑛)+1) 𝑒π‘₯𝑝 (βˆ’ ΞΌπœ“π›Ύ π‘‘β„Ž πœ™Ξ©1 ) Γ— ∏ [βˆ‘ ( 𝑗 π‘žβˆ’1 𝑗 π‘ž ) 𝑗 π‘žβˆ’1 𝑗 π‘ž=0 ( 1 π‘ž! ) 𝑗 π‘žβˆ’π‘— π‘ž+1 ] 𝑁 π·βˆ’1 π‘ž=1 ( Ξ©2 (𝑝+1) ) πœ‰ 𝐺2,0 0,2 ( πœ™Ξ©1Ξ©2 Δ𝛾 π‘‘β„Ž(𝑝+1) | 1 βˆ’ πœ‰, 1 βˆ’ ) (24) 5. NUMERICAL RESULTS AND DISCUSSIONS In this section, the numerical results for the system outage probability, ABER, and throughput are presented based on the derived analytical closed form expression presented in (16), (22), and (24) respectively. Unless specified, the system parameters adopted are set to be: 𝑅 = 2 𝑏𝑖𝑑𝑠/𝑠/𝐻𝑧, Ξ©1 = 1, Ξ©2 = 1, πœ‚ = 1, πœ—1 = 2, πœ—2 = 3, and 𝛾 𝑇 = 20𝑑𝐡. Two selection scenarios are considered as follows: worst relay selection when π‘˜ = 1 and best relay selection when π‘˜ = 𝑁 In Figure 2, the effect of S-to-R distance on the concerned system under different relay selection scenarios is demonstrated The result shows that as 𝑑1 increases, both the energy harvested and received signal at the relay nodes become weaker causing the system outage probability to be degraded. However, beyond an optimum distance of 𝑑1 where the distance between the relay and destination becomes smaller, the system outage probability starts decreasing even with less transmit power for the relay to transmit
  • 7.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 5, October 2020 : 5296 - 5305 5302 information. Irrespective of this, the best relay selection offers the system better performance than the worst relay selection. The outage performance of the concerned system under different values of channel correlation coefficient at different relay distant is illustrated in Figure 3. The results show that as the transmit SNR increase the better the system outage probability. In addition, it can be depicted that the increase in correlation coefficient the better the system outage performance. However, the as the relays location far from the source, the worse the outage performance becomes due to less transmit power received at the relay node for information transmission. The results also indicated the simulation result perfectly match with the analytical result which proves the correctness of our derived expressions. The effect of channel correlation coefficient on the ABER of the system is illustrated in Figure 4 under different number of antenna at the destination. It can be clearly seen that increase in the number of destination antenna leads to reduction in the system error performance. It is also depicted from the results that the higher the channel correlation the better the system performance. The results also indicate that the analytical results are well agreed with the simulation results which shows the accuracy of our derivation. The error performance as a function of energy harvesting time is presented in Figure 5 under number of relay selection. It can be shown that as the energy harvesting time increases the better the system error performance. This is owing to the large amount of time available for relay nodes to replenished energy for information transmission. Also, the increase in the number of relay selection for transmission significantly improves the system error performance. Figure 2. Outage probability vs the S-to-R distance under different number of 𝑁 𝐷 at 𝛼 = 0.5, 𝜌 = 0.6, and 𝑑2 = 6 βˆ’ 𝑑1 Figure 3. Effect of correlation coefficient on the system outage probability under different S-to-R distance Figure 4. Impact of number of antenna at the destination 𝑁 𝐷 on the system ABER under different correlation coefficients at 𝛼 = 0.6, π‘˜ = 𝑁 = 4 Figure 5. ABER performance of the system under different relay selection at 𝑁 = 4, 𝜌 = 0.6, 𝑁 𝐷 = 2, 𝑁𝑅 𝑑 = 2
  • 8. Int J Elec & Comp Eng ISSN: 2088-8708  On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi) 5303 In Figure 6, the throughput performance of the system as a function of energy harvesting time is depicted under different average transmit SNR. The results show that the increase in the source transmit power, the higher the system throughput because larger energy is harvested at relay nodes. It can be deduced from the results that, at high transmit power, the optimum time is very short for energy harvesting and large time is used to decode information. Compare with the lower transmit power. The analytical results are perfectly matched with the simulation results showing the accuracy of the derived expression. The throughput as a function of relay distance from the source under different number of antenna at the destination is demonstrated in Figure 7. The results indicate that the system performance is significantly improved with the increase in the number of antenna at the destination. It can be seen from the results that at small values 𝑑1, the system throughput becomes degraded due to larger distance between the relay and the destination, and the outage probability is high at the regime. Thus, at the optimum relay location, the system performance starts increasing snice the smaller value of 𝑑2 result into higher system throughput with better system outage. As expected, the results depict that the system has better performance under the best relay selection compare with worst relay selection. The throughput performance of the system at different channel correlation coefficient and 𝑁 𝐷 is depicted in Figure 8. It can be seen from the results that higher throughput performance can be achieved with the best relay selection at high SNR. At low and high SNR, the throughput becomes saturated which shows that the outage probability has higher and lower values respectively. In addition, the results also prove that increase in the correlation coefficient significantly improve the system performance. The simulation results perfect matched with the analytical results which indicate the correctness of our derivation. Figure 6. Throughput versus the energy harvesting time under different average transmit SNR at 𝜌 = 0.6, 𝑁 𝐷 = 2, 𝑁𝑅 𝑑 = 4, π‘˜ = 𝑁 = 4 Figure 7. Effect of S-to-R distance on the system throughput under different number of 𝑁 𝐷 for different relay selection scenarios when 𝛼 = 0.2, 𝜌 = 0.6, and 𝑑2 = 6 βˆ’ 𝑑1 Figure 8. Performance system throughput under different correlation coefficient and 𝑁 𝐷 when 𝛼 = 0.2 at π‘˜ = 𝑁 = 4
  • 9.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 5, October 2020 : 5296 - 5305 5304 6. CONCLUSION The performance of energy harvesting based PRS cooperative system with TAS and outdated channel state is presented. Based on the TS protocol, the analytical closed form expression for the system outage probability and ABER are obtained. Through the outage probability, the system throughput for delay-limited transmission mode is determined. These exact expressions are verified by the Monte Carlo simulation. The results illustrated that the increase in channel coefficient significantly improve the system performance. In addition, the system offers better performance with the increase in number of the destination receive antenna. Also, the result shows that system outage probability, ABER and throughput performance improved with increasing the number of relays or the values of the correlation coefficient. REFERENCES [1] K. Zhu, F. Wang, S. Li, F. Jiang, and L. 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  • 10. Int J Elec & Comp Eng ISSN: 2088-8708  On the performance of energy harvesting AF partial relay selection… (Kehinde O. Odeyemi) 5305 [21] N. Yang, P. L. Yeoh, M. Elkashlan, R. Schober, and I. B. Collings, "Transmit antenna selection for security enhancement in MIMO wiretap channels," IEEE Transactions on Communications, vol. 61, no. 1, pp. 144-154, 2013. [22] V. Adamchik and O. Marichev, "The algorithm for calculating integrals of hypergeometric type functions and its realization in REDUCE system," Proceedings of Proceedings of the international symposium on Symbolic and algebraic computation, pp. 212-224, 1990. [23] Y. A. Brychkov, O. Marichev, and A. Prudnikov, "Integrals and Series, vol 3: more special functions," ed: Gordon and Breach science publishers, 1986. [24] I. Gradshteyn, I. Ryzhik, and R. H. Romer, "Tables of integrals, series, and products," ed: AAPT, 1988. [25] Y. Huang, J. Wang, P. Zhang, and Q. Wu, "Performance analysis of energy harvesting multi-antenna relay networks with different antenna selection schemes," IEEE Access, vol. 6, pp. 5654-5665, 2018. [26] K. O. Odeyemi and P. A. Owolawi, "Selection combining hybrid FSO/RF systems over generalized induced-fading channels," Optics Communications, vol. 433, pp. 159-167, 2019. BIOGRAPHIES OF AUTHORS Kehinde Oluwasesan Odeyemi received his B.Tech. degree in Electronic Engineering from Ladoke Akintola University of Technology Ogbomosho, Oyo State, Nigeria, in 2008. He later obtained an M.Eng. Degree in the same field from the Federal University of Technology, Akure in 2012. He received his Ph.D. degree in Electronic Engineering at the University of KwaZulu-Natal, Durban, South Africa in 2018. In 2012, he joined the department of Electrical and Electronic Engineering, University of Ibadan, Nigeria. He is a member of The Council for the Regulation of Engineering in Nigeria (COREN). He has written several research articles and his research interests are in the antenna design, optical wireless communications, diversity combining techniques and MIMO systems. Pius Adewale Owolawi received his B.Tech. degree in Physics/Electronics from the Federal University of Technology, Akure, in 2001. He then obtained a M.Sc. and Ph.D. degrees in Electronic Engineering from the University of KwaZulu-Natal in 2006 and 2010, respectively. He holds several industry certifications such as CCNA, CCNP, CWNP, CFOA, CFOS/D and MCITP. Member of several professional bodies like SAIEE, IEEE, and SA AMSAT. In 2007, he joined the faculty of the Engineering, Department of Electrical Engineering at Mangosuthu University of Technology, South Africa. Thereafter, in 2017, he joined the department of Computer Systems Engineering, Tshwane University of Technology, Pretoria, South Africa where is currently the head of department. His research interests are in the computational of Electromagnetic, modeling of radio wave propagation at high frequency, fiber optic communication, radio planning and optimization techniques and renewable energy. He has written several research articles and serves as a reviewer for many scientific journals.