2019 International Conference on Artificial Intelligence, Control and Automation Engineering (AICAE 2019) ISBN: 978-1-60595-643-5
The Well-posedness and Regularity of a Batch Arrival Poisson
Queue with Generalized Vacation
Xiao-hua WANG
*College of Humanities, Shaoxing University, Zhejiang Shaoxing, 312000, P. R. China
*Corresponding author
Keywords: Well-posedness, Regularity, Poisson queue, 𝐶0-semigroup, Dissipative operator, Dispersive operator.
Abstract. In this paper the solution of a batch arrival Poisson queue with generalized vacation is investigated. By using the method of functional analysis, especially, the linear operator theory and the 𝐶0 semigroup theory on Banach space, we prove the well-posedness of the system, and show the
existence of positive solution.
The Well-posedness of Solution
The system of differential equations associated with this model is the following([1]):
{
𝑑𝑄(𝑡)
𝑑𝑡 = −𝜆𝑄(𝑡) + 𝜇𝑅0(𝑡) + ∫ 𝑣 +∞
0 (𝑥)𝑃0(𝑥, 𝑡)𝑑𝑥, 𝑑𝑅0(𝑡)
𝑑𝑡 = −(𝜆 + 𝜇)𝑅0(𝑡) + 𝜇𝑅1(𝑡) + ∫ 𝑣 +∞
0 (𝑥)𝑃1(𝑥, 𝑡)𝑑𝑥, 𝑑𝑅𝑛(𝑡)
𝑑𝑡 = −(𝜆 + 𝜇)𝑅𝑛(𝑡) + 𝜇𝑅𝑛+1(𝑡) + 𝜆 ∑ 𝑎𝑖 𝑛
𝑖=1 𝑅𝑛−𝑖(𝑡) + ∫0+∞𝑣(𝑥)𝑃𝑛+1(𝑥, 𝑡)𝑑𝑥, 𝑛 ≥ 1, 𝜕𝑃0(𝑥,𝑡)
𝜕𝑡 +
𝜕𝑃0(𝑥,𝑡)
𝜕𝑥 = −[𝜆 + 𝑣(𝑥)]𝑃0(𝑥, 𝑡), 𝜕𝑃𝑛(𝑥,𝑡)
𝜕𝑡 +
𝜕𝑃𝑛(𝑥,𝑡)
𝜕𝑥 = −[𝜆 + 𝑣(𝑥)]𝑃𝑛(𝑥, 𝑡) + 𝜆 ∑ 𝑎𝑖 𝑛
𝑖=1 𝑃𝑛−𝑖(𝑥, 𝑡), 𝑛 ≥ 1.
(1)
where the following notations are defined:
𝜆: group arrival rate; 𝜇: service rate; 𝑋: arrival size random variable; 𝑎𝑘: 𝑃𝑟𝑜𝑏(𝑋 = 𝑘); 𝑉: vacation time random variable; 𝑉(𝑥): the distribution function of 𝑉.
The above set of equations is to be solved under the following boundary conditions:
𝑃0(0, 𝑡) = 𝜆𝑄(𝑡), 𝑃𝑛(0, 𝑡) = 0, 𝑛 ≥ 1. (2)
Equations (1)(2) should be solved together with the normalizing condition
𝑄(𝑡) + ∑ 𝑅𝑛 ∞
𝑛=0
(𝑡) + ∑ ∫ 𝑃𝑛 +∞
0 ∞
𝑛=0
(𝑥, 𝑡)𝑑𝑥 = 1,
and an initial conditions 𝑄(0) = 1, 𝑅𝑛(0) = 0, 𝑃𝑛(𝑥, 0) = 0, 𝑛 ≥ 0.
𝒜1
( 𝑄 𝑅0 𝑅𝑛
𝑃0(𝑥)
𝑃𝑛(𝑥)) =
(
−𝜆𝑄 + 𝜇𝑅0+ ∫ 𝑣 +∞
0
(𝑥)𝑃0(𝑥)𝑑𝑥
−(𝜆 + 𝜇)𝑅0+ ∫ 𝑣+∞
0
(𝑥)𝑃1(𝑥)𝑑𝑥
−(𝜆 + 𝜇)𝑅𝑛+ ∫+∞𝑣
0
(𝑥)𝑃𝑛+1(𝑥)𝑑𝑥
−𝑃0′(𝑥) − [𝜆 + 𝑣(𝑥)]𝑃0(𝑥)
−𝑃𝑛′(𝑥) − [𝜆 + 𝑣(𝑥)]𝑃𝑛(𝑥), 𝑛 ≥ 1 )
ℬ
( 𝑄 𝑅0 𝑅𝑛
𝑃0(𝑥)
𝑃𝑛(𝑥)) =
( 0 𝜇𝑅1
𝜇𝑅𝑛+1 + 𝜆 ∑ 𝑎𝑖 𝑛
𝑖=1
𝑅𝑛−𝑖, 𝑛 ≥ 1
0
𝜆 ∑ 𝑎𝑖 𝑛
𝑖=1
𝑃𝑛−𝑖(𝑥), 𝑛 ≥ 1
) ,
with the domain 𝐷(ℬ) = 𝑋, 𝐷(𝒜) = 𝐷(𝒜1), and
𝐷(𝒜) = {(𝑄, 𝑅𝑛, 𝑃𝑛(𝑥)) ∈ 𝑋: 𝑃𝑛′(𝑥) ∈ 𝐿1(ℝ+), 𝑛 ≥ 0; 𝑃
0(0) = 𝜆𝑄, 𝑃𝑛(0) = 0, 𝑛 ≥ 1. }
Then the equation system (1.1)(1.2) can be rewritten as an abstract Cauchy problem on 𝑋:
{𝑑𝑃(𝑡)𝑑𝑡 = 𝒜𝑃(𝑡), 𝑡 > 0, 𝑃(0) = 𝑃̃0.𝑃(𝑡) = (𝑄, 𝑅𝑛, 𝑃𝑛(𝑥)), 𝑃̃0 = (1,0,0, ⋯ ). (3)
Theorem 1.1𝒜1 is a linear closed and densely defined operator on 𝑋. Proof of Theorem 1.1 is a direct verification, so we omit the details.
Let 𝑋∗ be the dual space of 𝑋, and 𝒜1∗ be the dual operator of 𝒜1, then 𝑋∗ = ℝ × 𝑙∞(ℝ) × 𝐿∞(ℝ+× ℕ). From (𝒜
1𝑃, 𝑊) = (𝑃, 𝒜1∗𝑊), we can obtain
𝒜1∗
( 𝑞 𝑟0
𝑟𝑛
𝑝0(𝑥)
𝑝𝑛(𝑥)) =
(
𝜆[𝑝0(0) − 𝑞] 𝜇𝑞 − (𝜆 + 𝜇)𝑟0 −(𝜆 + 𝜇)𝑟𝑛, 𝑛 ≥ 1
𝑝0′(𝑥) − [𝜆 + 𝑣(𝑥)]𝑝0(𝑥) +𝑞𝑣(𝑥)
𝑝𝑛′(𝑥) − [𝜆 + 𝑣(𝑥)]𝑝𝑛(𝑥) +𝑟𝑛−1𝑣(𝑥), 𝑛 ≥ 1 )
,
with the domain 𝐷(𝒜1∗) = {(𝑞, 𝑟𝑛, 𝑝𝑛(𝑥)) ∈ 𝑋∗: 𝑝𝑛′(𝑥), 𝑣(𝑥)𝑝𝑛(𝑥) ∈ 𝐿∞(𝑅+), 𝑛 ≥ 0. }
Theorem 1.2 1 is not a eigenvalue of 𝒜1∗.
Proof Let 𝑊 = (𝑞, 𝑟𝑛, 𝑝𝑛(𝑥)) ∈ 𝑋∗, 𝒜1∗𝑊 = 𝑊, i.e.,
0 0 0
[p (0) q] q, q ( )r r, ( )rn r nn, 1
(4)
0'( ) [ ( )] 0( ) ( ) 0( )
p x v x p x qv x p x (5)
1
'( ) [ ( )] ( ) ( ) ( ), 1
n n n n
𝑝0(𝑥) = 𝑒∫ [
𝑥
0 1+𝜆+𝑣(𝑠)]𝑑𝑠{𝑝0(0) − ∫ 𝑞
𝑥
0
𝑣(𝑢)𝑒− ∫ [0𝑢1+𝜆+𝑣(𝑠)]𝑑𝑠𝑑𝑢},
𝑝𝑛(𝑥) = 𝑒∫ [0𝑥1+𝜆+𝑣(𝑠)]𝑑𝑠{𝑝
𝑛(0) − ∫ 𝑟𝑛−1 𝑥
0
𝑣(𝑢)𝑒− ∫ [0𝑢1+𝜆+𝑣(𝑠)]𝑑𝑠𝑑𝑢}, 𝑛 ≥ 1.
Let 𝑥 → +∞ , observing 𝑝0(𝑥), 𝑝𝑛(𝑥) ∈ 𝐿∞, we get
𝑝0(0) = ∫ 𝑞 +∞
0
𝑣(𝑢)𝑒− ∫ [0𝑢1+𝜆+𝑣(𝑠)]𝑑𝑠𝑑𝑢, 𝑝𝑛(0) = ∫ 𝑟𝑛−1
+∞
0
𝑣(𝑢)𝑒− ∫ [0𝑢1+𝜆+𝑣(𝑠)]𝑑𝑠𝑑𝑢, 𝑛 ≥ 1.
Let ∫0+∞𝑣(𝑢)𝑒− ∫ [
𝑢
0 1+𝜆+𝑣(𝑠)]𝑑𝑠𝑑𝑢 = 𝑎, then 0 < 𝑎 < 1, and we obtain 𝑝0(0) = 𝑎𝑞, 𝑝𝑛(0) =
𝑎𝑟𝑛−1, 𝑛 ≥ 1. It is combined with (4), we get 𝑞 = 0. Furthermore, we also get 𝑟𝑛 = 0, 𝑛 ≥ 0,
therefore, 𝑝𝑛(0) = 0, 𝑛 ≥ 0. Thus we get 𝑝𝑛(𝑥) ≡ 0, 𝑛 ≥ 0. Hence 𝑊 = 0 and 1 is not a
eigenvalue of 𝒜1∗.
We can use the Lumer-Phillips Theorem(Ref.[2]) to show the well-posedness of the system (3).
Theorem 1.3. (1)𝒜 is a dissipative operator on 𝑋.
(2) The operator 𝒜1 generates a 𝐶0 semigroup of contraction.
Proof Firstly, 𝒜 is a dissipative operator on 𝑋. In fact, for any 𝑃 = (𝑄, 𝑅𝑛, 𝑃𝑛(𝑥)) ∈ 𝐷(𝒜), we
define 𝑊 = (𝑞, 𝑟𝑛, 𝑝𝑛(𝑥)) ∈ 𝑋∗ , where 𝑞 =∥ 𝑃 ∥ 𝑠𝑔𝑛(𝑄), 𝑟𝑛 =∥ 𝑃 ∥ 𝑠𝑔𝑛(𝑅𝑛), 𝑝𝑛(𝑥) =∥ 𝑃 ∥ 𝑠𝑔𝑛(𝑃𝑛(𝑥)), then (𝑃, 𝑊) =∥ 𝑃 ∥∥ 𝑊 ∥. In addition, we have
(𝒜𝑃, 𝑊) =∥ 𝑃 ∥ {[−𝜆𝑄 + 𝜇𝑅0+ ∫ 𝑣 +∞
0
(𝑥)𝑃0(𝑥)𝑑𝑥]𝑠𝑔𝑛(𝑄) + [−(𝜆 + 𝜇)𝑅0
+ ∫ 𝑣
+∞
0
(𝑥)𝑃1(𝑥)𝑑𝑥 + 𝜇𝑅1]𝑠𝑔𝑛(𝑅0) − ∑[ ∞
𝑛=1
(𝜆 + 𝜇)𝑅𝑛− ∫ 𝑣 +∞
0
(𝑥)𝑃𝑛+1(𝑥)𝑑𝑥 − 𝜇𝑅𝑛+1
−𝜆 ∑ 𝑎𝑖 𝑛
𝑖=1
𝑅𝑛−𝑖]𝑠𝑔𝑛(𝑅𝑛) − ∫ [ +∞
0
𝑃0′(𝑥) + (𝜆 + 𝑣(𝑥))𝑃0(𝑥)]𝑠𝑔𝑛(𝑃0(𝑥))𝑑𝑥
− ∑ ∫ [+∞
0 ∞
𝑛=1
𝑃𝑛′(𝑥) + (𝜆 + 𝑣(𝑥))𝑃𝑛(𝑥) − 𝜆 ∑ 𝑎𝑖
𝑛
𝑖=1
𝑃𝑛−𝑖(𝑥)]𝑠𝑔𝑛(𝑃𝑛(𝑥))𝑑𝑥} ≤∥ 𝑃
∥ {−𝜆|𝑄| + 𝜇|𝑅0| + ∫ 𝑣
+∞
0
(𝑥)|𝑃0(𝑥)|𝑑𝑥 − (𝜆 + 𝜇)|𝑅0| + ∫ 𝑣
+∞
0
(𝑥)|𝑃1(𝑥)|𝑑𝑥 + 𝜇|𝑅1|
− ∑[
∞
𝑛=1
(𝜆 + 𝜇)|𝑅𝑛| − ∫ 𝑣+∞
0
(𝑥)|𝑃𝑛+1(𝑥)|𝑑𝑥 − 𝜇|𝑅𝑛+1| − 𝜆 ∑ 𝑎𝑖
𝑛
𝑖=1
|𝑅𝑛−𝑖|] + 𝜆|𝑄|
− ∫ [
+∞
0
𝜆 + 𝑣(𝑥)]|𝑃0(𝑥)|𝑑𝑥 − ∑ ∫ [ +∞
0 ∞
𝑛=1
(𝜆 + 𝑣(𝑥))|𝑃𝑛(𝑥)| − 𝜆 ∑ 𝑎𝑖 𝑛
𝑖=1
|𝑃𝑛−𝑖(𝑥)|]𝑑𝑥} = 0.
Therefore, 𝒜 is dissipative. Observing (𝒜1𝑃, 𝑊) ≤ (𝒜𝑃, 𝑊), we known that 𝒜1 is dissipative
and hence 𝑅(𝐼 − 𝒜1) is a closed subspace of 𝑋.
Furthermore, we have 𝑅(𝐼 − 𝒜1) = 𝑋. If it is not true, then there exists a 𝑊 ∈ 𝑋∗, such that for any 𝐹 ∈ 𝑅(𝐼 − 𝒜1), (𝐹, 𝑊) = 0. Hence, for any 𝑃 ∈ 𝐷(𝒜1), ((𝐼 − 𝒜1)𝑃, 𝑊) = 0, i.e., for any
Theorem 1.4. The operator 𝒜 generates a 𝐶0 semigroup on 𝑋. The system (3) is well-posed.
Proof Obviously, ℬ is a bounded linear operator on 𝑋, using the perturbation theory of semigroup ([2]), we know that the operator 𝒜 generates a 𝐶0 semigroup on 𝑋. Therefore, the system (3) is well-possed.
The Regularity of Solution
For a practical physical state, an important problem is the existence of positive solution.
Definition 2.1. ([3]) Let 𝑌 be a Banach lattice, 𝑌+ be a positive cone of 𝑌 and 𝒯 be a linear operator on 𝑌. Denote 𝐺(𝑥) = {𝜑 ∈ 𝑌+∗: ∥ 𝜑 ∥≤ 1, (𝑥, 𝜑) =∥ 𝑥+ ∥2}. If, for any 𝑥 ∈ 𝐷(𝒯), there exists a 𝜑 ∈ 𝐺(𝑥), such that (𝒯𝑥, 𝜑) ≤ 0, then 𝒯 is called a dispersive operator.
Theorem 2.1. (1)𝒜 is a dispersive operator on 𝑋.
(2) The operator 𝒜 generates a positive 𝐶0 contractive semigroup on 𝑋.
Proof It is well known that 𝑋 is a Banach lattice. According to Ref. [3], it is sufficient to prove that 𝒜 is a dispersive operator. For any 𝑃 = (𝑄, 𝑅𝑛, 𝑃𝑛(𝑥)) ∈ 𝐷(𝒜), we choose 𝑊 = (𝑞, 𝑟𝑛, 𝑝𝑛(𝑥)) ∈ 𝑋∗ , where 𝑞 =∥ 𝑃 ∥ 𝑠𝑔𝑛
+(𝑄), 𝑟𝑛 =∥ 𝑃 ∥ 𝑠𝑔𝑛+(𝑅𝑛), 𝑝𝑛(𝑥) =∥ 𝑃 ∥
𝑠𝑔𝑛+(𝑃𝑛(𝑥)), and if 𝑎 > 0, then 𝑠𝑔𝑛+𝑎 = 1; if 𝑎 ≤ 0, then 𝑠𝑔𝑛+𝑎 = 0.
Similar to the proof of Theorem 1.3, a direct verification can show that (𝒜𝑃, 𝑊) ≤ 0. Observing 𝑊 ∈ 𝐺(𝑃), the desired result is obtained.
The following result studies the regularity of the system.
Theorem 2.2. Let 𝑇(𝑡) be a positive contractive semigroup with generator 𝒜, then 𝑇(𝑡) satisfies positive conserve property, i.e., for any 𝐻0 ∈ 𝐷(𝒜) and 𝐻0 > 0, ∥ 𝑇(𝑡)𝐻0 ∥=∥ 𝐻0 ∥, 𝑡 ≥ 0.
Proof Since 𝐻0 ∈ 𝐷(𝒜) and 𝐻0 > 0, then 𝑇(𝑡)𝐻0 ∈ 𝐷(𝒜) is a classical solution of the system (3). Let 𝑃(𝑡) = (𝑄(𝑡), 𝑅𝑛(𝑡), 𝑃𝑛(𝑥, 𝑡)) = 𝑇(𝑡)𝐻0 > 0, then 𝑃(𝑡) satisfies (1)(2). Note that
𝑑
𝑑𝑡∥ 𝑃(𝑡) ∥= 𝑑
𝑑𝑡∥ 𝑇(𝑡)𝐻0 ∥=
𝑑𝑄(𝑡) 𝑑𝑡 + ∑
𝑑𝑅𝑛(𝑡) 𝑑𝑡
∞
𝑛=0
+ ∑ ∫ 𝜕𝑃𝑛(𝑥, 𝑡) 𝜕𝑡
+∞
0 ∞
𝑛=0
𝑑𝑥,
we get
𝑑
𝑑𝑡∥ 𝑃(𝑡) ∥ = −𝜆𝑄(𝑡) + 𝜇𝑅0(𝑡) + ∫ 𝑣
+∞
0
(𝑥)𝑃0(𝑥, 𝑡)𝑑𝑥 − (𝜆 + 𝜇)𝑅0(𝑡) + 𝜇𝑅1(𝑡) + ∫ 𝑣 +∞
0
(𝑥)𝑃1(𝑥, 𝑡)𝑑𝑥
− ∑[
∞
𝑛=1
(𝜆 + 𝜇)𝑅𝑛(𝑡) − 𝜇𝑅𝑛+1(𝑡) − 𝜆 ∑ 𝑎𝑖
𝑛
𝑖=1
𝑅𝑛−𝑖(𝑡) − ∫ 𝑣
+∞
0
(𝑥)𝑃𝑛+1(𝑥, 𝑡)𝑑𝑥]
− ∫ {
+∞
0
𝜕𝑃0(𝑥, 𝑡)
𝜕𝑥 + [𝜆 + 𝑣(𝑥)]𝑃0(𝑥, 𝑡)}𝑑𝑥 − ∑ ∫ {
+∞
0 ∞
𝑛=1
𝜕𝑃𝑛(𝑥, 𝑡)
𝜕𝑥 + [𝜆 + 𝑣(𝑥)]𝑃𝑛(𝑥, 𝑡)
− 𝜆 ∑ 𝑎𝑖 𝑛
𝑖=1
𝑃𝑛−𝑖(𝑥, 𝑡)}𝑑𝑥
= −𝜆𝑄(𝑡) + 𝜇𝑅0(𝑡) + ∫ 𝑣
+∞
0
(𝑥)𝑃0(𝑥, 𝑡)𝑑𝑥 − (𝜆 + 𝜇)𝑅0(𝑡) + 𝜇𝑅1(𝑡) + ∫ 𝑣
+∞
0
− ∑[
∞
𝑛=1
(𝜆 + 𝜇)𝑅𝑛(𝑡) − 𝜇𝑅𝑛+1(𝑡) − 𝜆 ∑ 𝑎𝑖
𝑛
𝑖=1
𝑅𝑛−𝑖(𝑡) − ∫ 𝑣
+∞
0
(𝑥)𝑃𝑛+1(𝑥, 𝑡)𝑑𝑥] + 𝜆𝑄(𝑡)
− ∫ [
+∞
0
𝜆 + 𝑣(𝑥)]𝑃0(𝑥, 𝑡)𝑑𝑥 − ∑ ∫ { +∞
0 ∞
𝑛=1
[𝜆 + 𝑣(𝑥)]𝑃𝑛(𝑥, 𝑡) − 𝜆 ∑ 𝑎𝑖 𝑛
𝑖=1
𝑃𝑛−𝑖(𝑥, 𝑡)}𝑑𝑥 = 0.
Hence ∥ 𝑃(𝑡) ∥=∥ 𝑃(0) ∥=∥ 𝐻0 ∥.
Conclusion
By using the linear operator theory and the 𝐶0 semigroup theory, we obtained the following results: (1) The operator 𝒜 generates a positive 𝐶0 contractive semigroup on 𝑋. The system (3) is well-posed. (2) Let 𝑇(𝑡) be a positive contractive semigroup with generator 𝒜, then 𝑇(𝑡) satisfies positive conserve property, i.e., for any 𝐻0 ∈ 𝐷(𝒜) and 𝐻0 > 0, ∥ 𝑇(𝑡)𝐻0 ∥=∥ 𝐻0 ∥, 𝑡 ≥ 0.
After the mathematical modeling for the problem, our task is mainly to solve the following questions:
(1) the system under consideration has a unique nonnegative time-dependent solution; (2) approximate of solution; (3) the system has a steady state, and the dynamic solution of the system converges to the steady state.
Obviously, this paper only completed the above question (1).
References
[1] Borthakur A. and Choudhury G. On a batch arrival poisson queue with generalized vacation,
Indian J. Stat., 59(1997), B: 369-383.
[2] Pazy A. Semigroup of linear operators and applications to partial differential equations,
Springer-Verlag, New York, 1983.