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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 374
BATCH ARRIVAL RETRIAL QUEUING SYSTEM WITH STATE
DEPENDENT ADMISSION AND BERNOULLI VACATION
J. Ebenesar Anna Bagyam1
, K. Udaya Chandrika2
1
Assistant Professor, Department of Mathematics, SNS College of Technology, Coimbatore, India,
2
Professor, Department of Mathematics, Avinashilingam Deemed University for Women, Tamil Nadu, India,
ebenesar.j@gmail.com, udayachandrika@gmail.com
Abstract
A single server batch arrival retrial queue with server vacation under Bernoulli schedule is considered. Arrivals are controlled
according to the state of the server. The necessary and sufficient condition for the system to be stable is derived. Explicit formulae for
the stationary distributions and performance measures of the system in steady state are obtained. Numerical examples are presented
to illustrate the influence of the parameters on several performance characteristics.
Keywords: Retrial queue, batch arrival, state dependent admission control, Bernoulli vacation.
--------------------------------------------------------------------***--------------------------------------------------------------------------
1. INTRODUCTION
Retrial queues have the feature that arriving customers finding
no free servers must leave the service area and repeat their
demands for service after a random time. A customer is said to
be in orbit between two retrials. Nowadays, retrial queues
have become increasingly important in the analysis of
computer and communication networks. For recent papers on
retrial queues, see [1], [3], [4], [5] and [13].
In recent years queues with server vacation have emerged as
an important area of research due to their various application
in production systems, communication systems, computer
networks and etc. Some comprehensive studies on the recent
results for a variety of vacation models can be found in [6],
[7], [10], [11], [12], [14].
In many queuing situations, the customer’s arrival rate varies
according to the server state idle, busy and on vacation.
Altman et al. [2] considered the state dependent 1/G/M type
queuing analysis for congestion control in data networks.
Madan and Abu-Dayyeh [7] and Madan and Choudhury [8]
have investigated classical queuing system with restricted
admissibility of arriving batches and Bernoulli server
vacation. This paper examines the state dependent retrial
queuing system with bulk arrival and server vacation. The
similar situation of retrial can be realized in on-line ticket
booking centres.
2. SYSTEM DESCRIPTION
Consider a single server infinite capacity queuing facility with
batch arrival. One of the arriving customers begins his service
immediately if the server is available and the remaining
customers leave the service area to join the orbit.
The arrival epochs occur in accordance with a Poisson process
with rate λ and the number of arrivals at each epoch is a
random variable X having distribution nc]nX[P == and
moments nC , .1n ≥ Successive inter retrial times of any
customer in orbit is generally distributed with distribution
function )x(A and Laplace transform ).s(A∗
The service
time is a random variable with distribution function ),x(B
Laplace transform )s(B∗
and finite moments .1n,n ≥µ
After completion of each service, the server may take a
vacation with probability θ or may continue to be in the
system with complementary probability. The vacation times
are generally distributed with distribution function ),x(V
Laplace transform )s(V∗
and finite moments .1n,vn ≥
The arriving batches are allowed to join the system with state
dependent admission control policy. Let 21 ,αα and 3α be the
assigned probabilities for an arriving batch to join the system
during the period of idle, busy and vacation times respectively.
The hazard rate function of retrial time, service time and
vacation time are defined as
;
)x(A1
)x(a
)x(
−
=η ;
)x(B1
)x(b
)x(
−
=µ .
)x(V1
)x(v
)x(
−
=β
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 375
3. THE JOINT DISTRIBUTIONS
The stage of the system at time t can be described by the
Markov process ,0t);t(),t(N),t(J{}0t);t(M{( i ≥ξ=≥
}2,1,0i,0i == where )t(J denotes the server state 2,1,0
according as the server being idle or busy or on vacation and
)t(N denotes the number of customers in the retrial queue at
time .t If 0)t(J = and ,0)t(N > then )t(0ξ represents the
elapsed retrial time, if 1)t(J = and ,0)t(N > )t(1ξ
corresponds to the elapsed service time of the customer at time
5, and if 2)t(J = and ,0)t(N > )t(2ξ corresponds to the
elapsed vacation time .t
For the process },0t);t(M{ ≥ define the probabilities
)t(0Ι = }0)t(N,0)t(J{P ==
dx)x,t(nΙ = 1n},dxx)t(x,n)t(N,0)t(J{P 0 ≥+≤ξ≤==
dx)x,t(Wn = 0n},dxx)t(x,n)t(N,1)t(J{P 1 ≥+≤ξ≤==
dx)x,t(Vn = 0n},dxx)t(x,n)t(N,2)t(J{P 2 ≥+≤ξ≤==
Let )x(W),x(, nn0 ΙΙ and )x(Vn are the limiting densities of
)x,t(W),x,t(),t( nn0 ΙΙ and ).x,t(Vn
Define the probability generating function
;z)x()x,z(
1n
n
n∑
∞
=
Ι=Ι ;z)x(W)x,z(W
0n
n
n∑
∞
=
=
∑
∞
=
=
1n
n
n z)x(V)x,z(V and ∑
∞
=
=
1n
n
n zc)z(c
4. ERGODICITY CONDITION
Let }Nn,{ n ∈τ be the sequence of epochs of the service
completion times or vacation termination times. The sequence
of random vectors )}(N),(J{Q nnn
++
ττ= forms a Markov
chain, which is the embedded Markov chain for our queuing
system with state space S = {0, 1, 2} x {0, 1, 2, ...}
Theorem1
}1n,Q{ n ≥ is ergodic if and only if
1]v[C)](A1[C 1312111 <θα+µαλ+λα− ∗
Proof
}1n,Q{ n ≥ is an irreducible and aperiodic Markov chain. To
prove ergodicity, we shall use Foster’s criterion : An
irreducible and aperiodic Markov chain is ergodic if there
exists a non negative function Nj),j(f ∈ and 0>ε such that
the mean drift ]jQ|)f(Q)Q(f[E nn1nj =−=Ψ + is finite for
all Nj∈ and ε−≤Ψj for all ,Nj∈ except perhaps a finite
number.
Take .j)j(f = Then we have




=−θα+θ−αλ
=−θα+µαλ+λα−
=Ψ
∗
0jif1]v)1([C
,....3,2,1jif1]v[C)](A1[C
1321
1312111
j
Clearly, the inequality
1]v[C)](A1[C 1312111 <θα+µαλ+λα− ∗
is a sufficient
condition for ergodicity. The same inequality is also necessary
for ergodicity. We can guarantee the non-ergodicity of the
Markov chain },1n,Q{ n ≥ if it satisfies Kaplan’s condition,
namely ∞<Ψj for all Nj∈ and there exists Nj0 ∈ such that
0j ≥Ψ for .jj 0≥ In our case, Kaplan’s condition is satisfied
because there exists Nk∈ such that 0rij = for kij −< and
,0i > where )r(R ij= is the one step transition matrix of
}.1n,Q{ n ≥ Then the inequality
1]v[C)](A1[C 1312111 <θα+µαλ+λα− ∗
implies the non
ergodicity of the Markov chain.
Since the arrival stream is a Poisson process, it can be shown
from Burke’s theorem that the steady state probabilities of
}0t),t(N),t(J{ ≥ exist and are positive if and only if
1]v[C)](A1[C 1312111 <θα+µαλ+λα− ∗
.
From the mean drift Ψj=
1]v[C)](A1[C 1312111 −θα+µαλ+λα− ∗
, for 1j ≥ we have
the reasonable conclusion that the term ]v[C 13121 θα+µαλ
represents a batch arrival during service time and on vacation
time. The other term 1)](A1[C 11 −λα− ∗
refers to the
contribution to the orbit size due to batch arrival during the
retrial time excluding the arbitrary customer of the arriving
batch whose service commences so that he no longer belongs
to the orbit. Similar interpretation can be provided for .0j =
the condition 0j <Ψ assures that the orbit size does not grow
indefinitely in course of time.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 376
5. STEADY STATE PROBABILITY
GENERATION FUNCTION
The steady state equations that governs the system under
consideration are
0Ιλ = ∫∫
∞∞
µθ−+β
0
0
0
0 dx)x()x(W)1(dx)x()x(V (1)
)x(
dx
d
nΙ = 1n),x()1()x())x(( n1n ≥Ια−λ+Ιη+λ− (2)
)x(W
dx
d
n = )x(W)1()x(W))x(( n2n α−λ+µ+λ−
0n),x(Wc)1(
n
1k
knkn02 ≥δ−αλ+ ∑
=
− (3)
)x(V
dx
d
n = )x(V)1()x(V))x(( n3n α−λ+β+λ−
0n),x(Vc)1(
n
1k
knkn03 ≥δ−αλ+ ∑
=
− (4)
With boundary conditions
)0(nΙ = 1n,dx)x()x(W)1(dx)x()x(V
0
n
0
n ≥µθ−+β ∫∫
∞∞
(5)
)0(W0 = ∫
∞
ηΙ+Ιλ
0
101 dx)x()x(c (6)
)0(Wn = ∫
∞
++ ηΙ+Ιλ
0
1n01n dx)x()x(c
1n,dx)x(c
0
n
1k
1knk1 ≥Ιαλ+ ∫ ∑
∞
=
+− (7)
)0(Vn = 0n,dx)x()x(W
0
n ≥µθ ∫
∞
(8)
From the equations (2) – (8) we have,
)x,z(Ι = )]x(A1[e)0,z( x1 −Ι λα−
(9)
)x,z(W = )]x(B1[e)0,z(W x))z(c1(2 −−λα−
(10)
)x,z(V = )]x(V1[e)0,z(V x))z(c1(3 −−λα−
(11)
)0,(zΙ = ∫
∞
β
0
dx)x()x,z(V
0
0
dx)x()x,z(W)1( Ιλ−µθ−+ ∫
∞
(12)
)0,z(W = ))](A1)(z(c)(A[)0,z( 11 λα−+λαΙ ∗∗
)z(c0Ιλ+ (13)
)0,z(V = )))z(c1((B)0,z(W 2 −λαθ ∗
(14)
Substituting the expressions of )x,z(V and )x,z(W in terms
of )0,z(W in equation (12), we get
)0,z(Ι = )))z(c1((V)))z(c1((B)0,z(W 32 −λα−λαθ ∗∗
02 )))z(c1((B)0,z(W)1( Ιλ−−λαθ−+ ∗
= )))z(c1((B)0,z(W 2 −λα∗
03 )))]z(c1((V1[ Ιλ−−λαθ+θ− ∗
(15)
Using the expression )0,z(Ι in equation (13) and simplifying
we obtain
)0,z(W = )z(D/)]z(c1[)(A 10 −λαΙλ ∗
(16)
Where
D(z) = )))]z(c1((V1[)))z(c1((B 32 −λαθ+θ−−λα ∗∗
z))](A1)(z(c)(A[ 11 −λα−+λα ∗∗
(17)
Now equations (15) and (14) become
)0,(zΙ = )))z(c1((B)z(cz{ 20 −λα−Ιλ ∗
)z(D/)))]}z(c1((V1[ 3 −λαθ+θ− ∗
(18)
)0,z(V = )))z(c1((B)]z(c1[)(A 210 −λαθ−λαΙλ ∗∗
)z(D/ (19)
Theorem 2
Using equilibrium state, the joint distribution of the server has
the following partial generating functions
)z(Ι = )](A1[)))z(c1((B)z(cz[ 120 λα−−λα−Ι ∗∗
)]z(D/[)))]}z(c1((V1[ 13 α−λαθ+θ− ∗
(20)
)z(W = )]z(D/[)))]}z(c1((B1[)(A 2210 α−λα−λαΙ ∗∗
(21)
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 377
)z(V = )))z(c1((B)(A 210 −λαθλαΙ ∗∗
)]z(D/[)))]}z(c1((V1[ 33 α−λα− ∗
(22)
0Ι = 211 T/Tα (23)
Where
T1 = ]v[C)](A1[C1 1312111 θα+µαλ−λα−− ∗
T2 = )TC)(A)((A1(T 111111 −λαλα−+α ∗∗
]v[C)(A 11111 θ+µλλαα+ ∗
Proof
Substituting for )0,z(W),0,z(Ι and )x,z(V given by equations
(9), (10) and (11) and integrating with respect to x from 0 to
∞ we get the results given in equations (20) – (22).
Now, the unknown constant 0Ι given in equation (23) can be
determined by using the normalizing condition
.1)1(V)1(W)1(0 =++Ι+Ι
6. MEAN ORBIT SIZE AND MEAN SYSTEM SIZE
Theorem 3
The probability generating function of the number of customer
in the orbit is
)z(Pq = )))z(c1((B)(A)1([ 213210 −λαλαα−ααθΙ ∗∗
)))]z(c1((V1[ 3 −λα− ∗
321 )1( αα−α−
)(A)))z(c1((B 12 λα−λα ∗∗
)z(c)](A1[)1( 1321 λα−ααα−− ∗
)))]z(c1((V1)))[z(c1((B 32 −λαθ+θ−−λα ∗∗
)(A 131 λααα+ ∗
)]z(D/[))}(A1(z 3211132 αααλα−α−αα+ ∗
(24)
The probability generating function of number of customer in
the system is
)z(Pq = )))z(c1((B)(A)1([ 213210 −λαλαα−ααθΙ ∗∗
)))]z(c1((V1[ 3 −λα− ∗
)))z(c1((B)(A 21321 −λαλαααα− ∗∗
))(A1()1( 1321 λα−ααα−− ∗
)))z(c1((B)z(c 2 −λα∗
)))]z(c1((V1[ 3 −λαθ+θ− ∗
)(Az)1( 1321 λαααα−+ ∗
))))}z(c1((B( 2121 −λαα−α−α ∗
)]z(D/[ 321 ααα (25)
Proof
The probability generating function for the number of
customer in the orbit is
)z(Pq = )z(V)z(W)z(0 ++Ι+Ι and
The probability generating function for the number of
customer in the system is
)z(Ps = )z(V)z(zW)z(0 ++Ι+Ι
Substituting the expressions of )z(W),z(Ι and ),z(V we get
the equations as in (24) and (25).
Corollary 1
The mean number of customer in the orbit is
qL = )TT/(TNT/N 213122 + (26)
The mean number of customer in the system is
sL = 21111q T/C)(AL µλαλα+ ∗
(27)
Where
3T = ))(A1(CvC 112
2
11132
2
1
2
λα−µαλ+µθααλ ∗
))(A1(vC 113
2
1 λα−θαλ+ ∗
2
2
1
2
2
2
C[ µαλ+
2/))](A1(CvC 122
2
1
22
3 λα−+λαθ+ ∗
1N = 112111 CC[))(A1()1( µλα+λα−α− ∗
))(A1(]vC 11113 λα−α−−θλα+ ∗
])1(v)1([)(AC 1213111 µα−+α−θλαλα+ ∗
2N = 11
2
1
2
2131 vC)(A)1( µλαλαθα−α ∗
2
2
1
2
1331 vC)(A)1({ λλαθα−αα+ ∗
2
2
1
2
1221 C)(A)1( µλλαα−αα+ ∗
2
2
1
22
2211 CC))[(A1)(1( µλα+λα−α−+ ∗
))(A1)(1(2/]}vC 112
2
1
22
3 λα−α−+λαθ+ ∗
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 378
1
2
131
2
12 vCC[ θλα+µλα
]vC 11
2
1
2
23 µλααθ+
Proof
Differentiating )z(Pq and )z(Ps with respect to z and taking
limit 1z → by using L′Hospital rule the expressions for qL
and sL can be obtained.
7. OPERATING CHARACTERISTICS
Some performance measures for the system are given below.
1. The steady state probability that the server is idle in the
empty system is
2110 T/Tα=Ι
2. The steady state probability that the server is idle in the
non-empty system is
211131121 T/]1CvCC)][(A1[ −+λαθ+µλαλα−=Ι ∗
3. The steady state probability that the server is busy is
21111 T/C)(AW µλλαα= ∗
4. The steady state probability that the server is on vacation
is
21111 T/vC)(AV λθλαα= ∗
5. The probability that the orbit is empty while the server is
busy is
)]}(V1[)(BT{/)](B1[TW 32222110 λαθ+θ−λααλα−α= ∗∗∗
6. The probability that the orbit is empty while the server is
on vacation is
)]}(V1[T{/)](V1[TV 3233110 λαθ+θ−αλα−αθ= ∗∗
7. The probability of orbit being empty is
E = 000 VW ++Ι
= )](V1)[p(B{T 323211 λαθ+θ−λααα ∗∗
)](B1[ 23 λα−α+ ∗
)}(V1)[(B 322 λα−λααθ+ ∗∗
8. NUMERICAL ILLUSTRATION
Numerical results are obtained when the service, retrial and
vacation times follow exponential distribution. Table shows
the dependence of the performance measures V,W,,0 ΙΙ and
qL for the fixed values of )c,c,,,,,( 21321 αααβθ = (5, 5,
0.8, 0.5, 0.5, 0.5, 0.5). Figures show the effect of 21 , αα and
3α (joining probability during the period of idle, busy and
vacation) on the performance measures. qL the mean number
of customer in the orbit for the parameters
)c,c,,,,,,,,( 21321 αααβθµηλ = (2, 15, 5, 5, 5, 0.8, 0.5, 0.5,
0.5, 0.5).
Table1. Performance measures for the various values of µµµµλλλλ,
and ηηηη
λ µ η
0Ι Ι W V qL
1 10 20 0.7125 0.0281 0.1297 0.1297 0.0895
30 0.7213 0.0188 0.1299 0.1299 0.0748
40 0.7258 0.0141 0.1301 0.1301 0.0675
50 0.7284 0.0113 0.1301 0.1301 0.0632
30 20 0.7920 0.0271 0.0452 0.1356 0.0644
30 0.8007 0.0181 0.0453 0.1359 0.0520
40 0.8051 0.0136 0.0453 0.1360 0.0459
50 0.8077 0.0109 0.0454 0.1361 0.0423
50 20 0.8088 0.0269 0.0274 0.1369 0.0608
30 0.8175 0.0180 0.0274 0.1371 0.0489
40 0.8218 0.0135 0.0274 0.1372 0.0429
50 0.8244 0.0108 0.0275 0.1373 0.0394
2 10 20 0.4833 0.0608 0.2280 0.2280 0.3565
30 0.5015 0.0407 0.2289 0.2289 0.3005
40 0.5107 0.0306 0.2294 0.2294 0.2738
50 0.5162 0.0245 0.2296 0.2296 0.2581
30 20 0.6129 0.0577 0.0824 0.2471 0.2253
30 0.6307 0.0386 0.0827 0.2481 0.1868
40 0.6396 0.0290 0.0829 0.2486 0.1682
50 0.6450 0.0232 0.0829 0.2488 0.1572
50 20 0.6414 0.0570 0.0503 0.2513 0.2075
30 0.6591 0.0381 0.0505 0.2523 0.1717
40 0.6680 0.0286 0.0506 0.2528 0.1543
50 0.6734 0.0229 0.0506 0.2531 0.1441
3 10 20 0.2949 0.0964 0.3044 0.3044 1.0085
30 0.3227 0.0647 0.3063 0.3063 0.8163
40 0.3367 0.0487 0.3073 0.3073 0.7308
50 0.3451 0.0390 0.3079 0.3079 0.6824
30 20 0.4562 0.0906 0.1133 0.3399 0.5360
30 0.4833 0.0608 0.1140 0.3419 0.4400
40 0.4970 0.0457 0.1143 0.3430 0.3952
50 0.5052 0.0367 0.1145 0.3436 0.3693
50 20 0.4931 0.0893 0.0696 0.3480 0.4808
30 0.5200 0.0599 0.0700 0.3501 0.3956
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 379
40 0.5336 0.0451 0.0702 0.3511 0.3556
50 0.5418 0.0361 0.0704 0.3518 0.3324
CONCLUSIONS
Retrial queue with batch arrival admission control and
Bernoulli vacation has been investigated in this paper. The
necessary and sufficient condition for the system to be stable
is obtained. The inputs of the parameters on the performance
measures are illustrated.
REFERENCES
[1] Aissani A 2011 An MX
/G/1 Energetic retrial queue with
vacation and control IMA Journal of Management
Mathematics22 13-32.
[2] Altman E, Avrachenkov K, Barakat C and Nunez-Queija
R 2002 State-dependent M/G/1 type queuing analysis for
congestion in control in data networks Comp.
Networks39(6) 789-808.
[3] Arivudainambi D and Godhandaraman P 2012 A batch
arrival retrial queue with two phase of service, feedback
and K optional vacations Applied Mathematical
Sciences6(22) 1071-1087.
[4] Artalejo J R and Li Q 2011 Performance analysis of a
block – structured discrete – time retrial queue with state
– dependent arrivals Discrete Event Dynamic Systems
20(3) 325-347.
[5] EbenesarAnnabagyam J and UdayaChandrika K 2012
Performance analysis of single server retrial queuing
system with Bernoulli and phase type vacations
International Journal of Computer Applications54 (7)
30-35.
[6] EbenesarAnnabagyam J and UdayaChandrika K 2010
Single server retrial queuing system with two different
vacation policies Int. J. Contemp. Math. Sciences5(32)
1591-1598.
[7] Khalaf R F, Madan K C and Lukas C A 2011 An
M[X]
/G/1 queue with Bernoulli schedule, general
vacation times, random breakdown, general delay times
and general repair times Applied Mathematical Sciences5
(1) 35-51.
[8] Madan K C and Abu-Dayyeh W 2002 Restricted
admissibility of batches into an MX
/G/1 type bulk queue
with modified Bernoulli schedule server vacations
ESSAIM : Probability and Statistics6, 113-125.
[9] Madan K C and Choudhury G 2004 Steady state analysis
of an M/(G1, G2)/1 queue with restricted admissibility of
arriving batches and modified Bernoulli server vacations
under a single vacation policy Journal of Probability and
Statistical Sciences2 (2) 167-185.
[10] Prakash Rani K, Srinivasan A and UdayaChandrika K
2008 An M/G/1 retrial queue with additional optional
service and server vacation ActaCienciaIndicaXXXIVM
(4) 1807-1813.
[11] Srinivasan A, Prakash Rani K and UdayaChandrika K
2007 Retrial queuing system with two-phase service and
vacation ActaCienciaIndicaXXXIII M (2) 365-370.
[12] Sumitha D and UdayaChandrika K 2012 Performance
analysis of repairable M/G/1 retrial queue with Bernoulli
vacation and orbital search International Journal of
Mathematica Archive3 (2).
[13] Sumitha D, EbenesarAnnabagyam J, UdayaChandrika K
and Prakash Rani K 2012 Bulk arrival two phase retrial
queuing system with orbital search, impatient customers
and different types of server vacations International
Research Journal1.3 977-987.
[14] UdayaChandrika K, Yasodha D and
EbenesarAnnabagyam J 2008 Two phase service retrial
queue with emergency and multiple vacations
ActaCienciaIndicaXXXIV M (1) 161-168.
α1
α2
α3
0
1
2
3
4
5
0 0.5 1 1.5
Lq
Probability values
α1
α2
α3

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Batch arrival retrial queuing system with state

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 374 BATCH ARRIVAL RETRIAL QUEUING SYSTEM WITH STATE DEPENDENT ADMISSION AND BERNOULLI VACATION J. Ebenesar Anna Bagyam1 , K. Udaya Chandrika2 1 Assistant Professor, Department of Mathematics, SNS College of Technology, Coimbatore, India, 2 Professor, Department of Mathematics, Avinashilingam Deemed University for Women, Tamil Nadu, India, ebenesar.j@gmail.com, udayachandrika@gmail.com Abstract A single server batch arrival retrial queue with server vacation under Bernoulli schedule is considered. Arrivals are controlled according to the state of the server. The necessary and sufficient condition for the system to be stable is derived. Explicit formulae for the stationary distributions and performance measures of the system in steady state are obtained. Numerical examples are presented to illustrate the influence of the parameters on several performance characteristics. Keywords: Retrial queue, batch arrival, state dependent admission control, Bernoulli vacation. --------------------------------------------------------------------***-------------------------------------------------------------------------- 1. INTRODUCTION Retrial queues have the feature that arriving customers finding no free servers must leave the service area and repeat their demands for service after a random time. A customer is said to be in orbit between two retrials. Nowadays, retrial queues have become increasingly important in the analysis of computer and communication networks. For recent papers on retrial queues, see [1], [3], [4], [5] and [13]. In recent years queues with server vacation have emerged as an important area of research due to their various application in production systems, communication systems, computer networks and etc. Some comprehensive studies on the recent results for a variety of vacation models can be found in [6], [7], [10], [11], [12], [14]. In many queuing situations, the customer’s arrival rate varies according to the server state idle, busy and on vacation. Altman et al. [2] considered the state dependent 1/G/M type queuing analysis for congestion control in data networks. Madan and Abu-Dayyeh [7] and Madan and Choudhury [8] have investigated classical queuing system with restricted admissibility of arriving batches and Bernoulli server vacation. This paper examines the state dependent retrial queuing system with bulk arrival and server vacation. The similar situation of retrial can be realized in on-line ticket booking centres. 2. SYSTEM DESCRIPTION Consider a single server infinite capacity queuing facility with batch arrival. One of the arriving customers begins his service immediately if the server is available and the remaining customers leave the service area to join the orbit. The arrival epochs occur in accordance with a Poisson process with rate λ and the number of arrivals at each epoch is a random variable X having distribution nc]nX[P == and moments nC , .1n ≥ Successive inter retrial times of any customer in orbit is generally distributed with distribution function )x(A and Laplace transform ).s(A∗ The service time is a random variable with distribution function ),x(B Laplace transform )s(B∗ and finite moments .1n,n ≥µ After completion of each service, the server may take a vacation with probability θ or may continue to be in the system with complementary probability. The vacation times are generally distributed with distribution function ),x(V Laplace transform )s(V∗ and finite moments .1n,vn ≥ The arriving batches are allowed to join the system with state dependent admission control policy. Let 21 ,αα and 3α be the assigned probabilities for an arriving batch to join the system during the period of idle, busy and vacation times respectively. The hazard rate function of retrial time, service time and vacation time are defined as ; )x(A1 )x(a )x( − =η ; )x(B1 )x(b )x( − =µ . )x(V1 )x(v )x( − =β
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 375 3. THE JOINT DISTRIBUTIONS The stage of the system at time t can be described by the Markov process ,0t);t(),t(N),t(J{}0t);t(M{( i ≥ξ=≥ }2,1,0i,0i == where )t(J denotes the server state 2,1,0 according as the server being idle or busy or on vacation and )t(N denotes the number of customers in the retrial queue at time .t If 0)t(J = and ,0)t(N > then )t(0ξ represents the elapsed retrial time, if 1)t(J = and ,0)t(N > )t(1ξ corresponds to the elapsed service time of the customer at time 5, and if 2)t(J = and ,0)t(N > )t(2ξ corresponds to the elapsed vacation time .t For the process },0t);t(M{ ≥ define the probabilities )t(0Ι = }0)t(N,0)t(J{P == dx)x,t(nΙ = 1n},dxx)t(x,n)t(N,0)t(J{P 0 ≥+≤ξ≤== dx)x,t(Wn = 0n},dxx)t(x,n)t(N,1)t(J{P 1 ≥+≤ξ≤== dx)x,t(Vn = 0n},dxx)t(x,n)t(N,2)t(J{P 2 ≥+≤ξ≤== Let )x(W),x(, nn0 ΙΙ and )x(Vn are the limiting densities of )x,t(W),x,t(),t( nn0 ΙΙ and ).x,t(Vn Define the probability generating function ;z)x()x,z( 1n n n∑ ∞ = Ι=Ι ;z)x(W)x,z(W 0n n n∑ ∞ = = ∑ ∞ = = 1n n n z)x(V)x,z(V and ∑ ∞ = = 1n n n zc)z(c 4. ERGODICITY CONDITION Let }Nn,{ n ∈τ be the sequence of epochs of the service completion times or vacation termination times. The sequence of random vectors )}(N),(J{Q nnn ++ ττ= forms a Markov chain, which is the embedded Markov chain for our queuing system with state space S = {0, 1, 2} x {0, 1, 2, ...} Theorem1 }1n,Q{ n ≥ is ergodic if and only if 1]v[C)](A1[C 1312111 <θα+µαλ+λα− ∗ Proof }1n,Q{ n ≥ is an irreducible and aperiodic Markov chain. To prove ergodicity, we shall use Foster’s criterion : An irreducible and aperiodic Markov chain is ergodic if there exists a non negative function Nj),j(f ∈ and 0>ε such that the mean drift ]jQ|)f(Q)Q(f[E nn1nj =−=Ψ + is finite for all Nj∈ and ε−≤Ψj for all ,Nj∈ except perhaps a finite number. Take .j)j(f = Then we have     =−θα+θ−αλ =−θα+µαλ+λα− =Ψ ∗ 0jif1]v)1([C ,....3,2,1jif1]v[C)](A1[C 1321 1312111 j Clearly, the inequality 1]v[C)](A1[C 1312111 <θα+µαλ+λα− ∗ is a sufficient condition for ergodicity. The same inequality is also necessary for ergodicity. We can guarantee the non-ergodicity of the Markov chain },1n,Q{ n ≥ if it satisfies Kaplan’s condition, namely ∞<Ψj for all Nj∈ and there exists Nj0 ∈ such that 0j ≥Ψ for .jj 0≥ In our case, Kaplan’s condition is satisfied because there exists Nk∈ such that 0rij = for kij −< and ,0i > where )r(R ij= is the one step transition matrix of }.1n,Q{ n ≥ Then the inequality 1]v[C)](A1[C 1312111 <θα+µαλ+λα− ∗ implies the non ergodicity of the Markov chain. Since the arrival stream is a Poisson process, it can be shown from Burke’s theorem that the steady state probabilities of }0t),t(N),t(J{ ≥ exist and are positive if and only if 1]v[C)](A1[C 1312111 <θα+µαλ+λα− ∗ . From the mean drift Ψj= 1]v[C)](A1[C 1312111 −θα+µαλ+λα− ∗ , for 1j ≥ we have the reasonable conclusion that the term ]v[C 13121 θα+µαλ represents a batch arrival during service time and on vacation time. The other term 1)](A1[C 11 −λα− ∗ refers to the contribution to the orbit size due to batch arrival during the retrial time excluding the arbitrary customer of the arriving batch whose service commences so that he no longer belongs to the orbit. Similar interpretation can be provided for .0j = the condition 0j <Ψ assures that the orbit size does not grow indefinitely in course of time.
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 376 5. STEADY STATE PROBABILITY GENERATION FUNCTION The steady state equations that governs the system under consideration are 0Ιλ = ∫∫ ∞∞ µθ−+β 0 0 0 0 dx)x()x(W)1(dx)x()x(V (1) )x( dx d nΙ = 1n),x()1()x())x(( n1n ≥Ια−λ+Ιη+λ− (2) )x(W dx d n = )x(W)1()x(W))x(( n2n α−λ+µ+λ− 0n),x(Wc)1( n 1k knkn02 ≥δ−αλ+ ∑ = − (3) )x(V dx d n = )x(V)1()x(V))x(( n3n α−λ+β+λ− 0n),x(Vc)1( n 1k knkn03 ≥δ−αλ+ ∑ = − (4) With boundary conditions )0(nΙ = 1n,dx)x()x(W)1(dx)x()x(V 0 n 0 n ≥µθ−+β ∫∫ ∞∞ (5) )0(W0 = ∫ ∞ ηΙ+Ιλ 0 101 dx)x()x(c (6) )0(Wn = ∫ ∞ ++ ηΙ+Ιλ 0 1n01n dx)x()x(c 1n,dx)x(c 0 n 1k 1knk1 ≥Ιαλ+ ∫ ∑ ∞ = +− (7) )0(Vn = 0n,dx)x()x(W 0 n ≥µθ ∫ ∞ (8) From the equations (2) – (8) we have, )x,z(Ι = )]x(A1[e)0,z( x1 −Ι λα− (9) )x,z(W = )]x(B1[e)0,z(W x))z(c1(2 −−λα− (10) )x,z(V = )]x(V1[e)0,z(V x))z(c1(3 −−λα− (11) )0,(zΙ = ∫ ∞ β 0 dx)x()x,z(V 0 0 dx)x()x,z(W)1( Ιλ−µθ−+ ∫ ∞ (12) )0,z(W = ))](A1)(z(c)(A[)0,z( 11 λα−+λαΙ ∗∗ )z(c0Ιλ+ (13) )0,z(V = )))z(c1((B)0,z(W 2 −λαθ ∗ (14) Substituting the expressions of )x,z(V and )x,z(W in terms of )0,z(W in equation (12), we get )0,z(Ι = )))z(c1((V)))z(c1((B)0,z(W 32 −λα−λαθ ∗∗ 02 )))z(c1((B)0,z(W)1( Ιλ−−λαθ−+ ∗ = )))z(c1((B)0,z(W 2 −λα∗ 03 )))]z(c1((V1[ Ιλ−−λαθ+θ− ∗ (15) Using the expression )0,z(Ι in equation (13) and simplifying we obtain )0,z(W = )z(D/)]z(c1[)(A 10 −λαΙλ ∗ (16) Where D(z) = )))]z(c1((V1[)))z(c1((B 32 −λαθ+θ−−λα ∗∗ z))](A1)(z(c)(A[ 11 −λα−+λα ∗∗ (17) Now equations (15) and (14) become )0,(zΙ = )))z(c1((B)z(cz{ 20 −λα−Ιλ ∗ )z(D/)))]}z(c1((V1[ 3 −λαθ+θ− ∗ (18) )0,z(V = )))z(c1((B)]z(c1[)(A 210 −λαθ−λαΙλ ∗∗ )z(D/ (19) Theorem 2 Using equilibrium state, the joint distribution of the server has the following partial generating functions )z(Ι = )](A1[)))z(c1((B)z(cz[ 120 λα−−λα−Ι ∗∗ )]z(D/[)))]}z(c1((V1[ 13 α−λαθ+θ− ∗ (20) )z(W = )]z(D/[)))]}z(c1((B1[)(A 2210 α−λα−λαΙ ∗∗ (21)
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 377 )z(V = )))z(c1((B)(A 210 −λαθλαΙ ∗∗ )]z(D/[)))]}z(c1((V1[ 33 α−λα− ∗ (22) 0Ι = 211 T/Tα (23) Where T1 = ]v[C)](A1[C1 1312111 θα+µαλ−λα−− ∗ T2 = )TC)(A)((A1(T 111111 −λαλα−+α ∗∗ ]v[C)(A 11111 θ+µλλαα+ ∗ Proof Substituting for )0,z(W),0,z(Ι and )x,z(V given by equations (9), (10) and (11) and integrating with respect to x from 0 to ∞ we get the results given in equations (20) – (22). Now, the unknown constant 0Ι given in equation (23) can be determined by using the normalizing condition .1)1(V)1(W)1(0 =++Ι+Ι 6. MEAN ORBIT SIZE AND MEAN SYSTEM SIZE Theorem 3 The probability generating function of the number of customer in the orbit is )z(Pq = )))z(c1((B)(A)1([ 213210 −λαλαα−ααθΙ ∗∗ )))]z(c1((V1[ 3 −λα− ∗ 321 )1( αα−α− )(A)))z(c1((B 12 λα−λα ∗∗ )z(c)](A1[)1( 1321 λα−ααα−− ∗ )))]z(c1((V1)))[z(c1((B 32 −λαθ+θ−−λα ∗∗ )(A 131 λααα+ ∗ )]z(D/[))}(A1(z 3211132 αααλα−α−αα+ ∗ (24) The probability generating function of number of customer in the system is )z(Pq = )))z(c1((B)(A)1([ 213210 −λαλαα−ααθΙ ∗∗ )))]z(c1((V1[ 3 −λα− ∗ )))z(c1((B)(A 21321 −λαλαααα− ∗∗ ))(A1()1( 1321 λα−ααα−− ∗ )))z(c1((B)z(c 2 −λα∗ )))]z(c1((V1[ 3 −λαθ+θ− ∗ )(Az)1( 1321 λαααα−+ ∗ ))))}z(c1((B( 2121 −λαα−α−α ∗ )]z(D/[ 321 ααα (25) Proof The probability generating function for the number of customer in the orbit is )z(Pq = )z(V)z(W)z(0 ++Ι+Ι and The probability generating function for the number of customer in the system is )z(Ps = )z(V)z(zW)z(0 ++Ι+Ι Substituting the expressions of )z(W),z(Ι and ),z(V we get the equations as in (24) and (25). Corollary 1 The mean number of customer in the orbit is qL = )TT/(TNT/N 213122 + (26) The mean number of customer in the system is sL = 21111q T/C)(AL µλαλα+ ∗ (27) Where 3T = ))(A1(CvC 112 2 11132 2 1 2 λα−µαλ+µθααλ ∗ ))(A1(vC 113 2 1 λα−θαλ+ ∗ 2 2 1 2 2 2 C[ µαλ+ 2/))](A1(CvC 122 2 1 22 3 λα−+λαθ+ ∗ 1N = 112111 CC[))(A1()1( µλα+λα−α− ∗ ))(A1(]vC 11113 λα−α−−θλα+ ∗ ])1(v)1([)(AC 1213111 µα−+α−θλαλα+ ∗ 2N = 11 2 1 2 2131 vC)(A)1( µλαλαθα−α ∗ 2 2 1 2 1331 vC)(A)1({ λλαθα−αα+ ∗ 2 2 1 2 1221 C)(A)1( µλλαα−αα+ ∗ 2 2 1 22 2211 CC))[(A1)(1( µλα+λα−α−+ ∗ ))(A1)(1(2/]}vC 112 2 1 22 3 λα−α−+λαθ+ ∗
  • 5. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 378 1 2 131 2 12 vCC[ θλα+µλα ]vC 11 2 1 2 23 µλααθ+ Proof Differentiating )z(Pq and )z(Ps with respect to z and taking limit 1z → by using L′Hospital rule the expressions for qL and sL can be obtained. 7. OPERATING CHARACTERISTICS Some performance measures for the system are given below. 1. The steady state probability that the server is idle in the empty system is 2110 T/Tα=Ι 2. The steady state probability that the server is idle in the non-empty system is 211131121 T/]1CvCC)][(A1[ −+λαθ+µλαλα−=Ι ∗ 3. The steady state probability that the server is busy is 21111 T/C)(AW µλλαα= ∗ 4. The steady state probability that the server is on vacation is 21111 T/vC)(AV λθλαα= ∗ 5. The probability that the orbit is empty while the server is busy is )]}(V1[)(BT{/)](B1[TW 32222110 λαθ+θ−λααλα−α= ∗∗∗ 6. The probability that the orbit is empty while the server is on vacation is )]}(V1[T{/)](V1[TV 3233110 λαθ+θ−αλα−αθ= ∗∗ 7. The probability of orbit being empty is E = 000 VW ++Ι = )](V1)[p(B{T 323211 λαθ+θ−λααα ∗∗ )](B1[ 23 λα−α+ ∗ )}(V1)[(B 322 λα−λααθ+ ∗∗ 8. NUMERICAL ILLUSTRATION Numerical results are obtained when the service, retrial and vacation times follow exponential distribution. Table shows the dependence of the performance measures V,W,,0 ΙΙ and qL for the fixed values of )c,c,,,,,( 21321 αααβθ = (5, 5, 0.8, 0.5, 0.5, 0.5, 0.5). Figures show the effect of 21 , αα and 3α (joining probability during the period of idle, busy and vacation) on the performance measures. qL the mean number of customer in the orbit for the parameters )c,c,,,,,,,,( 21321 αααβθµηλ = (2, 15, 5, 5, 5, 0.8, 0.5, 0.5, 0.5, 0.5). Table1. Performance measures for the various values of µµµµλλλλ, and ηηηη λ µ η 0Ι Ι W V qL 1 10 20 0.7125 0.0281 0.1297 0.1297 0.0895 30 0.7213 0.0188 0.1299 0.1299 0.0748 40 0.7258 0.0141 0.1301 0.1301 0.0675 50 0.7284 0.0113 0.1301 0.1301 0.0632 30 20 0.7920 0.0271 0.0452 0.1356 0.0644 30 0.8007 0.0181 0.0453 0.1359 0.0520 40 0.8051 0.0136 0.0453 0.1360 0.0459 50 0.8077 0.0109 0.0454 0.1361 0.0423 50 20 0.8088 0.0269 0.0274 0.1369 0.0608 30 0.8175 0.0180 0.0274 0.1371 0.0489 40 0.8218 0.0135 0.0274 0.1372 0.0429 50 0.8244 0.0108 0.0275 0.1373 0.0394 2 10 20 0.4833 0.0608 0.2280 0.2280 0.3565 30 0.5015 0.0407 0.2289 0.2289 0.3005 40 0.5107 0.0306 0.2294 0.2294 0.2738 50 0.5162 0.0245 0.2296 0.2296 0.2581 30 20 0.6129 0.0577 0.0824 0.2471 0.2253 30 0.6307 0.0386 0.0827 0.2481 0.1868 40 0.6396 0.0290 0.0829 0.2486 0.1682 50 0.6450 0.0232 0.0829 0.2488 0.1572 50 20 0.6414 0.0570 0.0503 0.2513 0.2075 30 0.6591 0.0381 0.0505 0.2523 0.1717 40 0.6680 0.0286 0.0506 0.2528 0.1543 50 0.6734 0.0229 0.0506 0.2531 0.1441 3 10 20 0.2949 0.0964 0.3044 0.3044 1.0085 30 0.3227 0.0647 0.3063 0.3063 0.8163 40 0.3367 0.0487 0.3073 0.3073 0.7308 50 0.3451 0.0390 0.3079 0.3079 0.6824 30 20 0.4562 0.0906 0.1133 0.3399 0.5360 30 0.4833 0.0608 0.1140 0.3419 0.4400 40 0.4970 0.0457 0.1143 0.3430 0.3952 50 0.5052 0.0367 0.1145 0.3436 0.3693 50 20 0.4931 0.0893 0.0696 0.3480 0.4808 30 0.5200 0.0599 0.0700 0.3501 0.3956
  • 6. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 10 | Oct-2013, Available @ http://www.ijret.org 379 40 0.5336 0.0451 0.0702 0.3511 0.3556 50 0.5418 0.0361 0.0704 0.3518 0.3324 CONCLUSIONS Retrial queue with batch arrival admission control and Bernoulli vacation has been investigated in this paper. The necessary and sufficient condition for the system to be stable is obtained. The inputs of the parameters on the performance measures are illustrated. REFERENCES [1] Aissani A 2011 An MX /G/1 Energetic retrial queue with vacation and control IMA Journal of Management Mathematics22 13-32. [2] Altman E, Avrachenkov K, Barakat C and Nunez-Queija R 2002 State-dependent M/G/1 type queuing analysis for congestion in control in data networks Comp. Networks39(6) 789-808. [3] Arivudainambi D and Godhandaraman P 2012 A batch arrival retrial queue with two phase of service, feedback and K optional vacations Applied Mathematical Sciences6(22) 1071-1087. [4] Artalejo J R and Li Q 2011 Performance analysis of a block – structured discrete – time retrial queue with state – dependent arrivals Discrete Event Dynamic Systems 20(3) 325-347. [5] EbenesarAnnabagyam J and UdayaChandrika K 2012 Performance analysis of single server retrial queuing system with Bernoulli and phase type vacations International Journal of Computer Applications54 (7) 30-35. [6] EbenesarAnnabagyam J and UdayaChandrika K 2010 Single server retrial queuing system with two different vacation policies Int. J. Contemp. Math. Sciences5(32) 1591-1598. [7] Khalaf R F, Madan K C and Lukas C A 2011 An M[X] /G/1 queue with Bernoulli schedule, general vacation times, random breakdown, general delay times and general repair times Applied Mathematical Sciences5 (1) 35-51. [8] Madan K C and Abu-Dayyeh W 2002 Restricted admissibility of batches into an MX /G/1 type bulk queue with modified Bernoulli schedule server vacations ESSAIM : Probability and Statistics6, 113-125. [9] Madan K C and Choudhury G 2004 Steady state analysis of an M/(G1, G2)/1 queue with restricted admissibility of arriving batches and modified Bernoulli server vacations under a single vacation policy Journal of Probability and Statistical Sciences2 (2) 167-185. [10] Prakash Rani K, Srinivasan A and UdayaChandrika K 2008 An M/G/1 retrial queue with additional optional service and server vacation ActaCienciaIndicaXXXIVM (4) 1807-1813. [11] Srinivasan A, Prakash Rani K and UdayaChandrika K 2007 Retrial queuing system with two-phase service and vacation ActaCienciaIndicaXXXIII M (2) 365-370. [12] Sumitha D and UdayaChandrika K 2012 Performance analysis of repairable M/G/1 retrial queue with Bernoulli vacation and orbital search International Journal of Mathematica Archive3 (2). [13] Sumitha D, EbenesarAnnabagyam J, UdayaChandrika K and Prakash Rani K 2012 Bulk arrival two phase retrial queuing system with orbital search, impatient customers and different types of server vacations International Research Journal1.3 977-987. [14] UdayaChandrika K, Yasodha D and EbenesarAnnabagyam J 2008 Two phase service retrial queue with emergency and multiple vacations ActaCienciaIndicaXXXIV M (1) 161-168. α1 α2 α3 0 1 2 3 4 5 0 0.5 1 1.5 Lq Probability values α1 α2 α3