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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume 5 Issue 5, July-August 2021 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470
@ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 72
The Queue Length of a GI/M/1 Queue with Set-Up
Period and Bernoulli Working Vacation Interruption
Li Tao
School of Mathematics and Statistics, Shandong University of Technology, Zibo, China
ABSTRACT
Consider a GI/M/1 queue with set-up period and working vacations.
During the working vacation period, customers can be served at a
lower rate, if there are customers at a service completion instant, the
vacation can be interrupted and the server will come back to a set-up
period with probability (0 1)
p p
≤ ≤ or continue the working vacation
with probability1 p
− , and when the set-up period ends, the server will
switch to the normal working level. Using the matrix analytic
method, we obtain the steady-state distributions for the queue length
at arrival epochs.
KEYWORDS: GI/M/1; set-up period; working vacation; vacation
interruption; Bernoulli
How to cite this paper: Li Tao "The
Queue Length of a GI/M/1 Queue with
Set-Up Period and Bernoulli Working
Vacation
Interruption"
Published in
International Journal
of Trend in
Scientific Research
and Development
(ijtsrd), ISSN: 2456-
6470, Volume-5 | Issue-5, August 2021,
pp.72-76, URL:
www.ijtsrd.com/papers/ijtsrd43743.pdf
Copyright © 2021 by author (s) and
International Journal of Trend in
Scientific Research and Development
Journal. This is an
Open Access article
distributed under the
terms of the Creative Commons
Attribution License (CC BY 4.0)
(http://creativecommons.org/licenses/by/4.0)
1. INTRODUCTION
Servi and Finn [1] first introduced the working
vacation models and studied an M/M/1 queue, the
server commits a lower service rate rather than
completely stopping the service during a vacation.
Baba [2] considered a GI/M/1 queue with working
vacations by the matrix-analytic method. For the
vacation interruption models, Li and Tian [3] first
introduced and studied an M/M/1 queue with working
vacations and vacation interruption. Then, Li et al. [4]
analyzed the GI/M/1 queue with working vacations
and vacation interruption by the matrix-analytic
method. Meanwhile, in some practical situations, it
needs some times to switch the lower rate to the
normal working level, which we call set-up times.
Zhao et al. [5] considered a GI/M/1 queue with set-up
period and working vacation and vacation
interruption. Bai et al. [6] studied a GI/M/1 queue
with set-up period and working vacations.
In this paper, based on the Bernoulli schedule rule we
analyze a GI/M/1 queue with set-up period and
working vacation and vacation interruption at the
same time. Zhang and Shi [7] first studied an M/M/1
queue with vacation and vacation interruption under
the Bernoulli rule. In our model, during the working
vacation period, if there are customers at a service
completion instant, the server can come back to a set-
up period with probability (0 1)
p p
≤ ≤ , not with
probability 1, or continue the working vacation with
probability1 p
− , which is different from the situation
many authors considered before, and when the set-up
period ends, the server will switch to the normal busy
period. Clearly, the models in [5,6] will be the special
cases of the model we consider.
2. Model description and embedded Markov
chain
Consider a GI/M/1 queue such that the arrival process
is a general distribution process. The server begins a
vacation each time when the queue becomes empty
and if there are customers arriving in a vacation
period, the server continues to work at a lower rate,
i.e., the working vacation period is an operation
period in lower speed. At a service completion
instant, if there are customers in the vacation period,
the vacation can be interrupted and the server is
resumed to a set-up period with probability
(0 1)
p p
≤ ≤ , or continues the vacation with probability
IJTSRD43743
International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 73
p ( 1
p p
= − ), and when the set-up period ends, the
server will switch to the normal working level.
Otherwise, the server continues the vacation.
Meanwhile, if there is no customer when a vacation
ends, the server begins another vacation, otherwise,
he switches to the set-up period, and after the set-up
period, the server switches to the normal busy period.
Suppose n
τ be the arrival epoch of nth customers with
0 0
τ = . The inter-arrival times { , 1
n n
τ ≥ } are
independent and identically distributed with a general
distribution function, denoted by ( )
A t with a mean
1/ λ and a Laplace Stieltjes transform (LST), denoted
by *
( )
A s . The service times during a normal service
period, the service times during a working vacation
period, the set-up times and the working vacation
times are exponentially distributed with rate µ ,η ,
β andθ , respectively.
Let ( )
L t be the number of customers in the system at
time t and ( 0)
n n
L L τ
= − be the number of the customers
before the nth arrival. Define 0
n
J = , the nth arrival
occurs during a working vacation period; 1
n
J = , the
nth arrival occurs during a set-up period; 2
n
J = , the
nth arrival occurs during a normal service period.
Then, the process {( , ), 1}
n n
L J n ≥ is an embedded
Markov chain with state space
{0,0} {( , ), 1, 0,1,2}.
k j k j
Ω = ∪ ≥ =
In order to express the transition matrix of ( , )
n n
L J , let
( , ),( , ) 1 1
( , , ).
i j k l n n n n
p P L k J l L i J j
+ +
= = = = =
∣
Meanwhile, we introduce the expressions below
0
( )
( ), 0,
!
k
t
k
t
a e dA t k
k
µ
µ
∞
−
= ≥
∫
( )
0 0
( ( ))
( ), 0,
!
k
t
x t x
k
t x
b e e dxdA t k
k
β µ
µ
β
∞
− − −
−
= ≥
∫ ∫
0
( )
( ), 0,
!
k
k t t
k
t
c p e e dA t k
k
η θ
η
∞
− −
= ≥
∫
( )
0 0
0
( )
( )
!
( ( ))
( ), 0,
( )!
l
k t t
l x x y x
k x
l
k l
t y
x
d p e e e
l
t y
e dydxdA t k
k l
η θ β
µ
η
θ β
µ
∞
− − − −
=
−
− −
=
−
≥
×
−
∑
∫ ∫ ∫
1
1 ( )
0 0
1
( )
( )
( 1)!
( ( ))
( ), 1,
( )!
l
k t t
l x x y x
k x
l
k l
t y
x
e p p e e e
l
t y
e dydxdA t k
k l
η θ β
µ
η η
β
µ
−
∞
− − − − −
=
−
− −
=
−
−
−
× ≥
∑
∫ ∫ ∫
( )
0 0
( )
( ), 0,
!
k
t
k x x t x
k
x
f p e e e dxdA t k
k
η θ β
η
θ
∞
− − − −
= ≥
∫ ∫
1
1 ( )
0 0
( )
( ), 1.
( 1)!
k
t
k x x t x
k
x
g p p e e e dxdA t k
k
η θ β
η η −
∞
− − − − −
= ≥
−
∫ ∫
Using the lexicographic sequence for the states, the
transition probability matrix of ( , )
n n
L J can be written
as the Block-Jacobi matrix
00 01
1 1 0
2 2 1 0
3 3 2 1 0
,
B A
B A A
P B A A A
B A A A A
 
 
 
 
=
 
 
 
 
M M M M M O
where
00 0 0 0 01 0 0 0
1 ; ( , , );
B c d f A c f d
= − − − =
0 0 0
*
0 0
0
0 ( ) ;
0 0
c f d
A A b
a
β
 
 
=  
 
 
0 0 ,
0 0
k k k k k
k k
k
c f g d e
A b
a
+ +
 
 
=  
 
 
0 0 0
1
*
0
0
1 ( )
1 ( ) , 1.
1
k
i i i i i
i
k
k i
i
k
i
i
c d e f g c d f
B b A k
a
β
=
=
=
 
− + + + + − − −
 
 
 
= − − ≥
 
 
 
−
 
 
∑
∑
∑
3. Steady-state distribution at arrival epochs
We first define
0 0 0
0 1 0 1
( ) , ( ) , ( ) ,
( ) , ( ) , ( ) , ( .
)
k k k
k k k
k k k
k k k k
k k k k
k k k k
A z a z B z b z C z c z
D z d z E z e z F z f z G z g z
∞ ∞ ∞
= = =
∞ ∞ ∞ ∞
= = = =
= = =
= = = =
∑ ∑ ∑
∑ ∑ ∑ ∑
In this section, we derive the steady-state distribution
for ( , )
n n
L J at arrival epochs using matrix-geometric
approach. In order to derive the steady-state
distribution, we need the following three lemmas.
Lemma 3.1.
*
( ) ( ),
A z A z
µ µ
= −
* *
[ ( ) ( )]
( ) ,
(1 )
A z A
B z
z
β µ µ β
β µ
− −
=
− −
*
( ) ( ),
C z A p z
θ η η
= + −
* *
* *
[ ( ) ( )]
( )
(1 )
[ ( ) ( )]
,
(1 ) ( )(1 )
A p z A
D z
z p z
A p z A z
z p z z
θβ θ η η β
β µ θ η η β
θβ θ η η µ µ
β µ θ η µ η
+ − −
=
− − + − −
+ − − −
−
− − + − − −
* *
* *
[ ( ) ( )]
( )
(1 )
[ ( ) ( )]
,
(1 ) ( )(1 )
p z A p z A
E z
z p z
p z A p z A z
z p z z
η β θ η η β
β µ θ η η β
η β θ η η µ µ
β µ θ η µ η
+ − −
=
− − + − −
+ − − −
−
− − + − − −
International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 74
* *
[ ( ) ( )]
( ) ,
A A p z
F z
p z
θ β θ η η
θ η η β
− + −
=
+ − −
* *
[ ( ) ( )]
( ) .
p z A A p z
G z
p z
η β θ η η
θ η η β
− + −
=
+ − −
Lemma 3.2. If 0
θ > , the
equation *
( )
z A p z
θ η η
= + − has a unique root in the
range 0<z<1.
Lemma 3.3. If 0
θ > , 0
β > and / 1
ρ λ µ
= < , then the
matrix equation
0
k
k
k
R R A
∞
=
= ∑ has the minimal
nonnegative solution
1 2 1 3 2 3 1
2 3 2
3
( ) ( ) ( )
0 ( ) ,
0 0
r r r r r r r
R r r r
r
δ δ γδ
− ∆ − − −
 
 
= ∆ −
 
 
 
where *
2 ( )
r A β
= , 1
r and 3
r are the unique roots in the
range 0<z<1 of equations
*
( )
z A p z
θ η η
= + − and *
( )
z A z
µ µ
= − , respectively, and
1 1
( ) / ( )
p r p r
δ θ η θ η η β
= + + − − , 2
/[ (1 )]
r
β β µ
∆ = − − ,
1 1
/[ ( )(1 )]
p r r
γ β θ η µ η
= + − − − .
Moreover, we can easily verify that the Markov
chain P is positive recurrent if and only if
0
θ > , 0
β > and 1
ρ < . And the matrix
00 01
1 1
1 1
0 0 0 0 0 0
0 0 0 0
2 1 2 1
1 1 1 1 1
0 3 2 0 0 3 2 0
2 3 2 2 3 2
0 0
3 3
[ ]
1
( ) ( )
1
( ) ( )
1 0 0
0 0 1
k k
k k
k k
B A
B R
R B R A
c d f c f d
c f c f
r r r r
r r r r r
a r r b a r r b
r r r r r r
a a
r r
δ δ
ω ω
∞ ∞
− −
= =
 
 
=  
 
 
− − −
 
 
+ − −
 
− − − −
 
 
= ∆ − ∆ −
 
− + −
 
 
 
−
 
 
∑ ∑
with 3 2 3 1 0
2 1
0 0
2 3 1 3 1 2 1
( ) ( ) ( )
[ ]
r r r r d
r r
a b
r r r r r r r
δ γδ δ
ω
∆ − − −
= − + − has a
positive left invariant vector
1 2 1 3 2 3 1
(1, , ( ), ( ) ( ))
K r r r r r r r
δ δ γδ
− ∆ − − − (1)
where K ia a random positive real number.
Let ( , )
L J be the stationary limit of the process ( , )
n n
L J ,
and denote
0 00 0 1 2
; ( , , ), 1,
k k k k k
π π π π π π
= = ≥
{ , } lim { , }, ( , ) .
kj n n
n
P L k J j P L k J j k j
π
→∞
= = = = = = ∈Ω
Theorem 3.4. If 0
θ > , 0
β > and 1
ρ < , the stationary
probability distribution of ( , )
L J is given by
0 3 1
1 3 2 1
2 3 3 2 3 1
(1 ) , 0,
(1 ) ( ), 0,
(1 ) [ ( ) ( )], 1,
k
k
k k
k
k k k k
k
r r k
r r r k
r r r r r k
π σ
π σδ
π σ δ γδ
 = − ≥

= − − ≥

 = − ∆ − − − ≥

where
1 2
3 2 2 1 1 3 2 2 3 1
(1 )(1 )
.
(1 )[(1 ) ( )] (1 )( ) (1 )( )
r r
r r r r r r r r r r
σ
δ δ γδ
− −
=
− − + − + ∆ − − − − −
Proof. With the Theorem 1.5.1 in [8],
00 10 11 12
( , , , )
π π π π is given by the positive left invariant
vector Eq. (1), and satisfies the normalizing condition
1
00 10 11 12
( , , )( ) 1,
I R e
π π π π −
+ − =
where e is a column vector with all elements equal to
one. Substituting R into the above relationship, we
can get
1 2 3
3
3 2 2 1 1 3 2 2 3 1
(1 )(1 )(1 )
(1 ) .
(1 )[(1 ) ( )] (1 )( ) (1 )( )
r r r
K r
r r r r r r r r r r
σ
δ δ γδ
− − −
= = −
− − + − + ∆ − − − − −
Therefore, we have
10 11 12 3 1 2 1 3 2 3 1
( , , ) (1 ) ( , ( ), ( ) ( ))
r r r r r r r r
π π π σ δ δ γδ
= − − ∆ − − − .
Using the Theorem 1.5.1 of Neuts [8], we can obtain
1
0 1 2 10 11 12
( , , ) ( , , ) , 1.
k
k k k k R k
π π π π π π π −
= = ≥ (2)
Taking 10 11 12
( , , )
π π π and 1
k
R −
into Eq. (2), the theorem
can be derived.
Then, we discuss the distribution of the queue length
L at the arrival epochs. From Theorem 3.4, we have
0 00 3
{ 0} (1 ) ,
P L r
π π σ
= = = = −
0 1 2
3 1 2 3 2 3 1
{ }
(1 ) [(1 ) ( ) ( )], 1.
k k k k
k k k k k k
P L k
r r r r r r r k
π π π π
σ δ δ δ γδ
= = = + +
= − − + + ∆ − − − ≥
The state probability of a server in the steady-state is
given by
3
0
0 1
(1 )
{ 0} ,
1
k
k
r
P J
r
σ
π
∞
=
−
= = =
−
∑
3 2 1
1
1 1 2
(1 )( )
{ 1} ,
(1 )(1 )
k
k
r r r
P J
r r
σδ
π
∞
=
− −
= = =
− −
∑
1 3 2 2 3 1
2
1 1 2
(1 )( ) (1 )( )
{ 2} .
(1 )(1 )
k
k
r r r r r r
P J
r r
σ δ σγδ
π
∞
=
∆ − − − − −
= = =
− −
∑
Theorem 3.5. If 0
θ > , 0
β > and 1
ρ < , the stationary
queue length L can be decomposed as 0 d
L L L
= + ,
where 0
L is the stationary queue length of a classical
GI/M/1 queue without vacation, and follows a
geometric distribution with parameter 3
r . Additional
queue length d
L has a distribution
{ 0} ,
d
P L σ
= =
1
3 1 1
1
3 2 2
{ } ( 1 )( )
( 1)( ) 1
, .
k
d
k
P L k r r r
r r r k
σ δ γδ
σδ
−
−
= = − −
+ ∆ − ≥
−
−
Proof. The probability generating function of L is as
follows:
International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 75
0 1 2
0 1 1
( ) k k k
k k k
k k k
L z z z z
π π π
∞ ∞ ∞
= = =
= + +
∑ ∑ ∑
3 2 3 1
2 1
3
1 1 2 2 3 1 3
( ) ( )
( )
1
(1 ) [ ]
1 (1 )(1 ) (1 )(1 ) (1 )(1 )
r r z r r z
r r z
r
rz rz r z r z r z rz r z
σ δ δ γδ
− −
−
= − + +∆ −
− − − − − − −
3 3 2 1 3 3 2 3 1
3 1 1 2 2 1
1 1 ( )(1 ) ( ) ( )
[ ]
1 1 (1 )(1 ) 1 1
r r z r r r z z r r z r r z
r z r z r z r z r z r z
σ δ δ γδ
− − − − − −
= + + ∆ −
− − − − − −
3 3 1 3 1 3 2 3 2 3 1
3 1 1 2 2 1
1 ( ) ( ) ( ) ( ) ( )
[1 ]
1 1 1 1 1 1
r r r z r r z r r z r r z r r z
r z rz rz r z r z rz
σ δ δ δ γδ
− − − − − −
= − + − +∆ −
− − − − − −
3 3 1 3 2
3 1 2
1 ( ) ( )
[ ( 1 ) ( 1) ]
1 1 1
r r r z r r z
r z r z r z
σ σ δ γδ σδ
− − −
= + − − + ∆ −
− − −
0 ( ) ( ).
d
L z L z
=
which completes the proof.
Thus, the mean queue length at the arrival epoch is
given by
3 3 1 3 2
2 2
3 1 2
( 1 )( ) ( 1)( )
[ ] .
1 (1 ) (1 )
r r r r r
E L
r r r
σ δ γδ σδ
− − − ∆ − −
= + +
− − −
4. Steady-state distribution at arbitrary epochs
Now we consider the steady-state distribution for the
queue length at arbitrary epochs. And, denote the
limiting distribution of ( )
L t : lim { ( ) }
k
t
p P L t k
→∞
= = .
Theorem 4.1. If 0
θ > , 0
β > and 1
ρ < , the limiting
distribution of ( )
L t exists. And, we obtain
3 3
0
1
1 1 1
2 1
3 3 2 1
1
(1 ) (1 ) (1 )(1 )
1 [ ],
(1 ) (1 ) (1 )(1 )
(1 ) [ ], 1.
k k k
k
r r
p
p r
r r
p r r r r k
p r
δ δ γδ
δ γδ
σλ
µ β θ η η
δ δ γδ
δ γδ
σλ
µ β θ η η
− − −
− ∆ − − + −
∆ −

= − + +
 + −



 − ∆ − − + −
∆ −
 = − + + ≥
+ −


Proof. From the theory of SMP, the limiting
distribution of ( )
L t has the following expression (see
[9]):
1
2 0
1
( )
(1 ( ))
( 1 )!
i k
t
k i
i k
t
p e A t dt
i k
µ
µ
π λ
+ −
∞ ∞
−
= −
= −
+ −
∑ ∫
1
( )
1 0 0
1
( ( ))
(1 ( ))
( 1 )!
i k
t
x t x
i
i k
t x
e e dx A t dt
i k
β µ
µ
π β λ
+ −
∞ ∞
− − −
= −
−
+ −
+ −
∑ ∫ ∫
1,1 0
(1 ( ))
t
k e A t dt
β
π λ
∞
−
−
+ −
∫
1
1
0 0
1
( )
(1 ( ))
( 1 )!
i k
i k t t
i
i k
t
p e e A t dt
i k
η θ
η
π λ
+ −
∞ ∞
+ − − −
= −
+ −
+ −
∑ ∫
1
( )
0 0 0
1 0
1
( )
( )
!
( ( ))
(1 ( ))
( 1 )!
l
i k t t
l x x y x
i x
i k l
i k l
t y
x
p e e e
l
t y
e dydx A t dt
i k l
η θ β
µ
η
π θ β
µ
λ
∞ + −
∞
− − − −
= − =
+ − −
− −
+
−
−
+
×
− −
∑ ∑
∫ ∫ ∫
1
1
1 ( )
0 0 0
1
1
( )
( )
( 1)!
( ( ))
(1 ( ))
( 1 )!
l
i k t t
l x x y x
i x
i k l
i k l
t y
x
p p e e e
l
t y
e dydx A t dt
i k l
η θ β
µ
η η
π β
µ
λ
−
∞ + −
∞
− − − − −
= =
+ − −
− −
+
−
×
−
−
+ − −
∑ ∑
∫ ∫ ∫
1
1 ( )
0 0 0
1
( )
(1 ( ))
( 1 )!
i k
t
i k x x t x
i
i k
x
p e e e dx A t dt
i k
η θ β
η
π θ λ
+ −
∞ ∞
+ − − − − −
= −
+ −
+ −
∑ ∫ ∫
( )
0 0 0
( )
(1 ( ))
( )!
i k
t
i k x x t x
i
i k
x
p p e e e dx A t dt
i k
η θ β
η η
π λ
−
∞ ∞
− − − − −
=
+ −
−
∑ ∫ ∫
1 2 3 4 5 6 7 8.
b b b b b b b b
= + + + + + + +
We compute each part of the equation and have
*
1 1
2
3 3 2
2
*
1
1
1
1
1 ( )
1 (1 ) [
(1 )
1 ( )
],
(1 )
k k
k
A r
b r r r
r
A r
r
r
µ µ
δ γδ
σλ δ
µ µ
µ µ
γδ
µ
− −
−
− −
∆ −
= − − ∆
−
− −
+
−
*
1 1
2 2
3 2 2
2
*
1 1
1 2
1 1
1 1 1
1 ( ) 1
2 (1 ) [
(1 )
(1 ( )) (1 )
],
(1 )
k k
k k
A r r
b r r r
r
A r r
r r
r r r
µ µ
σλ δ δ
µ β
µ µ δ
βδ
β µ µ µ β µ µ
− −
− −
− − −
= − ∆ − ∆
−
− − −
− +
− + − − +
1 1
2 2
3 2 1
(1 ) (1 )
3 (1 ) [ ],
k k
r r
b r r r
δ δ
σλ
β β
− −
− −
= − −
1
1
3 1
1
1
4 (1 ) ,
k
r
b r r
p r
σλ
θ η η
−
−
= −
+ −
1
3 1 1 2
3
1 1 1
1 *
3 1 1 1
1 1 1
(1 ) 1 1
5 (1 ) ( )
(1 ) 1 1 ( )
[ ],
(1 )
k
k
r r r r
b r
r p r p r
r r r A r
r p r r
σλ θβ
σ
β µ µ θ η η β θ η η β
σλθγ µ µ
β µ µ θ η η µ
−
−
− − −
= − −
− + + − − + −
− − − −
− −
− + + − −
3 1 1 2
1 1 1
*
3 1 1 1
1 1 1
(1 ) 1 1
6 ( )
(1 ) 1 1 ( )
[ ],
(1 )
k
k
r p r r r
b
r p r p r
r p r r A r
r p r r
σλ ηβ
β µ µ θ η η β θ η η β
σλ ηγ µ µ
β µ µ θ η η µ
− − −
= −
− + + − − + −
− − − −
− −
− + + − −
1
3 1 2 1
1 1
(1 ) 1 1
7 ( ),
k
r r r r
b
p r p r
σλθ
θ η η β β θ η η
−
− − −
= −
+ − − + −
Then, using these expressions, the theorem can be
obtained by some computation.
Let L denote the steady-state system size at an
arbitrary epoch, the mean of L can be given by
3 2
0 2 1 1
3
(1 ) 1
[ ] (1 ) [ ].
(1 ) (1 )( )
(1 )
k
k
E L kp r
r r p r
r
δ γδ δ δ γδ
σλ
β θ η η
µ
∞
=
∆ − − ∆ − +
= = − + +
− − + −
−
∑
Remark 4.2. If 1
p = , the system reduces to the model
described in [4], and if 0
p = , the system becomes a
GI/M/1 queue with set-up period and multiple
working vacations [6].
References
[1] L. Servi and S. Finn, “M/M/1 queue with
working vacations (M/M/1/WV)’’,
Performance Evaluation, vol. 50, pp. 41-52,
2002.
[2] Y. Baba, “Analysis of a GI/M/1 queue with
multiple working vacations’’, Operations
Research Letters, vol. 33, pp. 201-209, 2005.
International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 76
[3] J. Li and N. Tian, “The M/M/1 queue with
working vacations and vacation interruption’’,
Journal of Systems Science and Systems
Engineering, vol. 16, pp. 121-127, 2007.
[4] J. Li, N. Tian, and Z. Ma, “Performance
analysis of GI/M/1 queue with working
vacations and vacation interruption’’, Applied
Mathematical Modelling, vol. 32, pp. 2715-
2730, 2008.
[5] G. Zhao, X. Du, and N. Tian, “GI/M/1 queue
with set-up period and working vacation and
vacation interruption’’, International Journal of
Information and Management Sciences, vol. 20,
pp. 351-363, 2009.
[6] X. Bai, X. Wang, and N. Tian, “GI/M/1 queue
with set-up period and working vacations’’,
Journal of Information and Computational
Science, vol. 9, pp. 2313-2325, 2012.
[7] H. Zhang and D. Shi, “The M/M/1 queue with
Bernoulli-schedule-controlled vacation and
vacation interruption’’, International Journal of
Information and Management Sciences, vol. 20,
pp. 579-587, 2009.
[8] M. Neuts, “Matrix-Geometric Solutions in
Stochastic Models’’, Johns Hopkins University
Press, Baltimore, 1981.
[9] D. Gross, C. Harris, “Fundamentals of
Queueing Theory’’, 3rd Edition, Wiley, New
York, 1998.

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The Queue Length of a GI M 1 Queue with Set Up Period and Bernoulli Working Vacation Interruption

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume 5 Issue 5, July-August 2021 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470 @ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 72 The Queue Length of a GI/M/1 Queue with Set-Up Period and Bernoulli Working Vacation Interruption Li Tao School of Mathematics and Statistics, Shandong University of Technology, Zibo, China ABSTRACT Consider a GI/M/1 queue with set-up period and working vacations. During the working vacation period, customers can be served at a lower rate, if there are customers at a service completion instant, the vacation can be interrupted and the server will come back to a set-up period with probability (0 1) p p ≤ ≤ or continue the working vacation with probability1 p − , and when the set-up period ends, the server will switch to the normal working level. Using the matrix analytic method, we obtain the steady-state distributions for the queue length at arrival epochs. KEYWORDS: GI/M/1; set-up period; working vacation; vacation interruption; Bernoulli How to cite this paper: Li Tao "The Queue Length of a GI/M/1 Queue with Set-Up Period and Bernoulli Working Vacation Interruption" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456- 6470, Volume-5 | Issue-5, August 2021, pp.72-76, URL: www.ijtsrd.com/papers/ijtsrd43743.pdf Copyright © 2021 by author (s) and International Journal of Trend in Scientific Research and Development Journal. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (CC BY 4.0) (http://creativecommons.org/licenses/by/4.0) 1. INTRODUCTION Servi and Finn [1] first introduced the working vacation models and studied an M/M/1 queue, the server commits a lower service rate rather than completely stopping the service during a vacation. Baba [2] considered a GI/M/1 queue with working vacations by the matrix-analytic method. For the vacation interruption models, Li and Tian [3] first introduced and studied an M/M/1 queue with working vacations and vacation interruption. Then, Li et al. [4] analyzed the GI/M/1 queue with working vacations and vacation interruption by the matrix-analytic method. Meanwhile, in some practical situations, it needs some times to switch the lower rate to the normal working level, which we call set-up times. Zhao et al. [5] considered a GI/M/1 queue with set-up period and working vacation and vacation interruption. Bai et al. [6] studied a GI/M/1 queue with set-up period and working vacations. In this paper, based on the Bernoulli schedule rule we analyze a GI/M/1 queue with set-up period and working vacation and vacation interruption at the same time. Zhang and Shi [7] first studied an M/M/1 queue with vacation and vacation interruption under the Bernoulli rule. In our model, during the working vacation period, if there are customers at a service completion instant, the server can come back to a set- up period with probability (0 1) p p ≤ ≤ , not with probability 1, or continue the working vacation with probability1 p − , which is different from the situation many authors considered before, and when the set-up period ends, the server will switch to the normal busy period. Clearly, the models in [5,6] will be the special cases of the model we consider. 2. Model description and embedded Markov chain Consider a GI/M/1 queue such that the arrival process is a general distribution process. The server begins a vacation each time when the queue becomes empty and if there are customers arriving in a vacation period, the server continues to work at a lower rate, i.e., the working vacation period is an operation period in lower speed. At a service completion instant, if there are customers in the vacation period, the vacation can be interrupted and the server is resumed to a set-up period with probability (0 1) p p ≤ ≤ , or continues the vacation with probability IJTSRD43743
  • 2. International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 73 p ( 1 p p = − ), and when the set-up period ends, the server will switch to the normal working level. Otherwise, the server continues the vacation. Meanwhile, if there is no customer when a vacation ends, the server begins another vacation, otherwise, he switches to the set-up period, and after the set-up period, the server switches to the normal busy period. Suppose n τ be the arrival epoch of nth customers with 0 0 τ = . The inter-arrival times { , 1 n n τ ≥ } are independent and identically distributed with a general distribution function, denoted by ( ) A t with a mean 1/ λ and a Laplace Stieltjes transform (LST), denoted by * ( ) A s . The service times during a normal service period, the service times during a working vacation period, the set-up times and the working vacation times are exponentially distributed with rate µ ,η , β andθ , respectively. Let ( ) L t be the number of customers in the system at time t and ( 0) n n L L τ = − be the number of the customers before the nth arrival. Define 0 n J = , the nth arrival occurs during a working vacation period; 1 n J = , the nth arrival occurs during a set-up period; 2 n J = , the nth arrival occurs during a normal service period. Then, the process {( , ), 1} n n L J n ≥ is an embedded Markov chain with state space {0,0} {( , ), 1, 0,1,2}. k j k j Ω = ∪ ≥ = In order to express the transition matrix of ( , ) n n L J , let ( , ),( , ) 1 1 ( , , ). i j k l n n n n p P L k J l L i J j + + = = = = = ∣ Meanwhile, we introduce the expressions below 0 ( ) ( ), 0, ! k t k t a e dA t k k µ µ ∞ − = ≥ ∫ ( ) 0 0 ( ( )) ( ), 0, ! k t x t x k t x b e e dxdA t k k β µ µ β ∞ − − − − = ≥ ∫ ∫ 0 ( ) ( ), 0, ! k k t t k t c p e e dA t k k η θ η ∞ − − = ≥ ∫ ( ) 0 0 0 ( ) ( ) ! ( ( )) ( ), 0, ( )! l k t t l x x y x k x l k l t y x d p e e e l t y e dydxdA t k k l η θ β µ η θ β µ ∞ − − − − = − − − = − ≥ × − ∑ ∫ ∫ ∫ 1 1 ( ) 0 0 1 ( ) ( ) ( 1)! ( ( )) ( ), 1, ( )! l k t t l x x y x k x l k l t y x e p p e e e l t y e dydxdA t k k l η θ β µ η η β µ − ∞ − − − − − = − − − = − − − × ≥ ∑ ∫ ∫ ∫ ( ) 0 0 ( ) ( ), 0, ! k t k x x t x k x f p e e e dxdA t k k η θ β η θ ∞ − − − − = ≥ ∫ ∫ 1 1 ( ) 0 0 ( ) ( ), 1. ( 1)! k t k x x t x k x g p p e e e dxdA t k k η θ β η η − ∞ − − − − − = ≥ − ∫ ∫ Using the lexicographic sequence for the states, the transition probability matrix of ( , ) n n L J can be written as the Block-Jacobi matrix 00 01 1 1 0 2 2 1 0 3 3 2 1 0 , B A B A A P B A A A B A A A A         =         M M M M M O where 00 0 0 0 01 0 0 0 1 ; ( , , ); B c d f A c f d = − − − = 0 0 0 * 0 0 0 0 ( ) ; 0 0 c f d A A b a β     =       0 0 , 0 0 k k k k k k k k c f g d e A b a + +     =       0 0 0 1 * 0 0 1 ( ) 1 ( ) , 1. 1 k i i i i i i k k i i k i i c d e f g c d f B b A k a β = = =   − + + + + − − −       = − − ≥       −     ∑ ∑ ∑ 3. Steady-state distribution at arrival epochs We first define 0 0 0 0 1 0 1 ( ) , ( ) , ( ) , ( ) , ( ) , ( ) , ( . ) k k k k k k k k k k k k k k k k k k k k k A z a z B z b z C z c z D z d z E z e z F z f z G z g z ∞ ∞ ∞ = = = ∞ ∞ ∞ ∞ = = = = = = = = = = = ∑ ∑ ∑ ∑ ∑ ∑ ∑ In this section, we derive the steady-state distribution for ( , ) n n L J at arrival epochs using matrix-geometric approach. In order to derive the steady-state distribution, we need the following three lemmas. Lemma 3.1. * ( ) ( ), A z A z µ µ = − * * [ ( ) ( )] ( ) , (1 ) A z A B z z β µ µ β β µ − − = − − * ( ) ( ), C z A p z θ η η = + − * * * * [ ( ) ( )] ( ) (1 ) [ ( ) ( )] , (1 ) ( )(1 ) A p z A D z z p z A p z A z z p z z θβ θ η η β β µ θ η η β θβ θ η η µ µ β µ θ η µ η + − − = − − + − − + − − − − − − + − − − * * * * [ ( ) ( )] ( ) (1 ) [ ( ) ( )] , (1 ) ( )(1 ) p z A p z A E z z p z p z A p z A z z p z z η β θ η η β β µ θ η η β η β θ η η µ µ β µ θ η µ η + − − = − − + − − + − − − − − − + − − −
  • 3. International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 74 * * [ ( ) ( )] ( ) , A A p z F z p z θ β θ η η θ η η β − + − = + − − * * [ ( ) ( )] ( ) . p z A A p z G z p z η β θ η η θ η η β − + − = + − − Lemma 3.2. If 0 θ > , the equation * ( ) z A p z θ η η = + − has a unique root in the range 0<z<1. Lemma 3.3. If 0 θ > , 0 β > and / 1 ρ λ µ = < , then the matrix equation 0 k k k R R A ∞ = = ∑ has the minimal nonnegative solution 1 2 1 3 2 3 1 2 3 2 3 ( ) ( ) ( ) 0 ( ) , 0 0 r r r r r r r R r r r r δ δ γδ − ∆ − − −     = ∆ −       where * 2 ( ) r A β = , 1 r and 3 r are the unique roots in the range 0<z<1 of equations * ( ) z A p z θ η η = + − and * ( ) z A z µ µ = − , respectively, and 1 1 ( ) / ( ) p r p r δ θ η θ η η β = + + − − , 2 /[ (1 )] r β β µ ∆ = − − , 1 1 /[ ( )(1 )] p r r γ β θ η µ η = + − − − . Moreover, we can easily verify that the Markov chain P is positive recurrent if and only if 0 θ > , 0 β > and 1 ρ < . And the matrix 00 01 1 1 1 1 0 0 0 0 0 0 0 0 0 0 2 1 2 1 1 1 1 1 1 0 3 2 0 0 3 2 0 2 3 2 2 3 2 0 0 3 3 [ ] 1 ( ) ( ) 1 ( ) ( ) 1 0 0 0 0 1 k k k k k k B A B R R B R A c d f c f d c f c f r r r r r r r r r a r r b a r r b r r r r r r a a r r δ δ ω ω ∞ ∞ − − = =     =       − − −     + − −   − − − −     = ∆ − ∆ −   − + −       −     ∑ ∑ with 3 2 3 1 0 2 1 0 0 2 3 1 3 1 2 1 ( ) ( ) ( ) [ ] r r r r d r r a b r r r r r r r δ γδ δ ω ∆ − − − = − + − has a positive left invariant vector 1 2 1 3 2 3 1 (1, , ( ), ( ) ( )) K r r r r r r r δ δ γδ − ∆ − − − (1) where K ia a random positive real number. Let ( , ) L J be the stationary limit of the process ( , ) n n L J , and denote 0 00 0 1 2 ; ( , , ), 1, k k k k k π π π π π π = = ≥ { , } lim { , }, ( , ) . kj n n n P L k J j P L k J j k j π →∞ = = = = = = ∈Ω Theorem 3.4. If 0 θ > , 0 β > and 1 ρ < , the stationary probability distribution of ( , ) L J is given by 0 3 1 1 3 2 1 2 3 3 2 3 1 (1 ) , 0, (1 ) ( ), 0, (1 ) [ ( ) ( )], 1, k k k k k k k k k k r r k r r r k r r r r r k π σ π σδ π σ δ γδ  = − ≥  = − − ≥   = − ∆ − − − ≥  where 1 2 3 2 2 1 1 3 2 2 3 1 (1 )(1 ) . (1 )[(1 ) ( )] (1 )( ) (1 )( ) r r r r r r r r r r r r σ δ δ γδ − − = − − + − + ∆ − − − − − Proof. With the Theorem 1.5.1 in [8], 00 10 11 12 ( , , , ) π π π π is given by the positive left invariant vector Eq. (1), and satisfies the normalizing condition 1 00 10 11 12 ( , , )( ) 1, I R e π π π π − + − = where e is a column vector with all elements equal to one. Substituting R into the above relationship, we can get 1 2 3 3 3 2 2 1 1 3 2 2 3 1 (1 )(1 )(1 ) (1 ) . (1 )[(1 ) ( )] (1 )( ) (1 )( ) r r r K r r r r r r r r r r r σ δ δ γδ − − − = = − − − + − + ∆ − − − − − Therefore, we have 10 11 12 3 1 2 1 3 2 3 1 ( , , ) (1 ) ( , ( ), ( ) ( )) r r r r r r r r π π π σ δ δ γδ = − − ∆ − − − . Using the Theorem 1.5.1 of Neuts [8], we can obtain 1 0 1 2 10 11 12 ( , , ) ( , , ) , 1. k k k k k R k π π π π π π π − = = ≥ (2) Taking 10 11 12 ( , , ) π π π and 1 k R − into Eq. (2), the theorem can be derived. Then, we discuss the distribution of the queue length L at the arrival epochs. From Theorem 3.4, we have 0 00 3 { 0} (1 ) , P L r π π σ = = = = − 0 1 2 3 1 2 3 2 3 1 { } (1 ) [(1 ) ( ) ( )], 1. k k k k k k k k k k P L k r r r r r r r k π π π π σ δ δ δ γδ = = = + + = − − + + ∆ − − − ≥ The state probability of a server in the steady-state is given by 3 0 0 1 (1 ) { 0} , 1 k k r P J r σ π ∞ = − = = = − ∑ 3 2 1 1 1 1 2 (1 )( ) { 1} , (1 )(1 ) k k r r r P J r r σδ π ∞ = − − = = = − − ∑ 1 3 2 2 3 1 2 1 1 2 (1 )( ) (1 )( ) { 2} . (1 )(1 ) k k r r r r r r P J r r σ δ σγδ π ∞ = ∆ − − − − − = = = − − ∑ Theorem 3.5. If 0 θ > , 0 β > and 1 ρ < , the stationary queue length L can be decomposed as 0 d L L L = + , where 0 L is the stationary queue length of a classical GI/M/1 queue without vacation, and follows a geometric distribution with parameter 3 r . Additional queue length d L has a distribution { 0} , d P L σ = = 1 3 1 1 1 3 2 2 { } ( 1 )( ) ( 1)( ) 1 , . k d k P L k r r r r r r k σ δ γδ σδ − − = = − − + ∆ − ≥ − − Proof. The probability generating function of L is as follows:
  • 4. International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 75 0 1 2 0 1 1 ( ) k k k k k k k k k L z z z z π π π ∞ ∞ ∞ = = = = + + ∑ ∑ ∑ 3 2 3 1 2 1 3 1 1 2 2 3 1 3 ( ) ( ) ( ) 1 (1 ) [ ] 1 (1 )(1 ) (1 )(1 ) (1 )(1 ) r r z r r z r r z r rz rz r z r z r z rz r z σ δ δ γδ − − − = − + +∆ − − − − − − − − 3 3 2 1 3 3 2 3 1 3 1 1 2 2 1 1 1 ( )(1 ) ( ) ( ) [ ] 1 1 (1 )(1 ) 1 1 r r z r r r z z r r z r r z r z r z r z r z r z r z σ δ δ γδ − − − − − − = + + ∆ − − − − − − − 3 3 1 3 1 3 2 3 2 3 1 3 1 1 2 2 1 1 ( ) ( ) ( ) ( ) ( ) [1 ] 1 1 1 1 1 1 r r r z r r z r r z r r z r r z r z rz rz r z r z rz σ δ δ δ γδ − − − − − − = − + − +∆ − − − − − − − 3 3 1 3 2 3 1 2 1 ( ) ( ) [ ( 1 ) ( 1) ] 1 1 1 r r r z r r z r z r z r z σ σ δ γδ σδ − − − = + − − + ∆ − − − − 0 ( ) ( ). d L z L z = which completes the proof. Thus, the mean queue length at the arrival epoch is given by 3 3 1 3 2 2 2 3 1 2 ( 1 )( ) ( 1)( ) [ ] . 1 (1 ) (1 ) r r r r r E L r r r σ δ γδ σδ − − − ∆ − − = + + − − − 4. Steady-state distribution at arbitrary epochs Now we consider the steady-state distribution for the queue length at arbitrary epochs. And, denote the limiting distribution of ( ) L t : lim { ( ) } k t p P L t k →∞ = = . Theorem 4.1. If 0 θ > , 0 β > and 1 ρ < , the limiting distribution of ( ) L t exists. And, we obtain 3 3 0 1 1 1 1 2 1 3 3 2 1 1 (1 ) (1 ) (1 )(1 ) 1 [ ], (1 ) (1 ) (1 )(1 ) (1 ) [ ], 1. k k k k r r p p r r r p r r r r k p r δ δ γδ δ γδ σλ µ β θ η η δ δ γδ δ γδ σλ µ β θ η η − − − − ∆ − − + − ∆ −  = − + +  + −     − ∆ − − + − ∆ −  = − + + ≥ + −   Proof. From the theory of SMP, the limiting distribution of ( ) L t has the following expression (see [9]): 1 2 0 1 ( ) (1 ( )) ( 1 )! i k t k i i k t p e A t dt i k µ µ π λ + − ∞ ∞ − = − = − + − ∑ ∫ 1 ( ) 1 0 0 1 ( ( )) (1 ( )) ( 1 )! i k t x t x i i k t x e e dx A t dt i k β µ µ π β λ + − ∞ ∞ − − − = − − + − + − ∑ ∫ ∫ 1,1 0 (1 ( )) t k e A t dt β π λ ∞ − − + − ∫ 1 1 0 0 1 ( ) (1 ( )) ( 1 )! i k i k t t i i k t p e e A t dt i k η θ η π λ + − ∞ ∞ + − − − = − + − + − ∑ ∫ 1 ( ) 0 0 0 1 0 1 ( ) ( ) ! ( ( )) (1 ( )) ( 1 )! l i k t t l x x y x i x i k l i k l t y x p e e e l t y e dydx A t dt i k l η θ β µ η π θ β µ λ ∞ + − ∞ − − − − = − = + − − − − + − − + × − − ∑ ∑ ∫ ∫ ∫ 1 1 1 ( ) 0 0 0 1 1 ( ) ( ) ( 1)! ( ( )) (1 ( )) ( 1 )! l i k t t l x x y x i x i k l i k l t y x p p e e e l t y e dydx A t dt i k l η θ β µ η η π β µ λ − ∞ + − ∞ − − − − − = = + − − − − + − × − − + − − ∑ ∑ ∫ ∫ ∫ 1 1 ( ) 0 0 0 1 ( ) (1 ( )) ( 1 )! i k t i k x x t x i i k x p e e e dx A t dt i k η θ β η π θ λ + − ∞ ∞ + − − − − − = − + − + − ∑ ∫ ∫ ( ) 0 0 0 ( ) (1 ( )) ( )! i k t i k x x t x i i k x p p e e e dx A t dt i k η θ β η η π λ − ∞ ∞ − − − − − = + − − ∑ ∫ ∫ 1 2 3 4 5 6 7 8. b b b b b b b b = + + + + + + + We compute each part of the equation and have * 1 1 2 3 3 2 2 * 1 1 1 1 1 ( ) 1 (1 ) [ (1 ) 1 ( ) ], (1 ) k k k A r b r r r r A r r r µ µ δ γδ σλ δ µ µ µ µ γδ µ − − − − − ∆ − = − − ∆ − − − + − * 1 1 2 2 3 2 2 2 * 1 1 1 2 1 1 1 1 1 1 ( ) 1 2 (1 ) [ (1 ) (1 ( )) (1 ) ], (1 ) k k k k A r r b r r r r A r r r r r r r µ µ σλ δ δ µ β µ µ δ βδ β µ µ µ β µ µ − − − − − − − = − ∆ − ∆ − − − − − + − + − − + 1 1 2 2 3 2 1 (1 ) (1 ) 3 (1 ) [ ], k k r r b r r r δ δ σλ β β − − − − = − − 1 1 3 1 1 1 4 (1 ) , k r b r r p r σλ θ η η − − = − + − 1 3 1 1 2 3 1 1 1 1 * 3 1 1 1 1 1 1 (1 ) 1 1 5 (1 ) ( ) (1 ) 1 1 ( ) [ ], (1 ) k k r r r r b r r p r p r r r r A r r p r r σλ θβ σ β µ µ θ η η β θ η η β σλθγ µ µ β µ µ θ η η µ − − − − − = − − − + + − − + − − − − − − − − + + − − 3 1 1 2 1 1 1 * 3 1 1 1 1 1 1 (1 ) 1 1 6 ( ) (1 ) 1 1 ( ) [ ], (1 ) k k r p r r r b r p r p r r p r r A r r p r r σλ ηβ β µ µ θ η η β θ η η β σλ ηγ µ µ β µ µ θ η η µ − − − = − − + + − − + − − − − − − − − + + − − 1 3 1 2 1 1 1 (1 ) 1 1 7 ( ), k r r r r b p r p r σλθ θ η η β β θ η η − − − − = − + − − + − Then, using these expressions, the theorem can be obtained by some computation. Let L denote the steady-state system size at an arbitrary epoch, the mean of L can be given by 3 2 0 2 1 1 3 (1 ) 1 [ ] (1 ) [ ]. (1 ) (1 )( ) (1 ) k k E L kp r r r p r r δ γδ δ δ γδ σλ β θ η η µ ∞ = ∆ − − ∆ − + = = − + + − − + − − ∑ Remark 4.2. If 1 p = , the system reduces to the model described in [4], and if 0 p = , the system becomes a GI/M/1 queue with set-up period and multiple working vacations [6]. References [1] L. Servi and S. Finn, “M/M/1 queue with working vacations (M/M/1/WV)’’, Performance Evaluation, vol. 50, pp. 41-52, 2002. [2] Y. Baba, “Analysis of a GI/M/1 queue with multiple working vacations’’, Operations Research Letters, vol. 33, pp. 201-209, 2005.
  • 5. International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD43743 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 76 [3] J. Li and N. Tian, “The M/M/1 queue with working vacations and vacation interruption’’, Journal of Systems Science and Systems Engineering, vol. 16, pp. 121-127, 2007. [4] J. Li, N. Tian, and Z. Ma, “Performance analysis of GI/M/1 queue with working vacations and vacation interruption’’, Applied Mathematical Modelling, vol. 32, pp. 2715- 2730, 2008. [5] G. Zhao, X. Du, and N. Tian, “GI/M/1 queue with set-up period and working vacation and vacation interruption’’, International Journal of Information and Management Sciences, vol. 20, pp. 351-363, 2009. [6] X. Bai, X. Wang, and N. Tian, “GI/M/1 queue with set-up period and working vacations’’, Journal of Information and Computational Science, vol. 9, pp. 2313-2325, 2012. [7] H. Zhang and D. Shi, “The M/M/1 queue with Bernoulli-schedule-controlled vacation and vacation interruption’’, International Journal of Information and Management Sciences, vol. 20, pp. 579-587, 2009. [8] M. Neuts, “Matrix-Geometric Solutions in Stochastic Models’’, Johns Hopkins University Press, Baltimore, 1981. [9] D. Gross, C. Harris, “Fundamentals of Queueing Theory’’, 3rd Edition, Wiley, New York, 1998.