1. INTRODUCTION
Brauer[2] studied the asymptotic behavior of solutions of nonlinear systems and perturbations of nonlinear systems by means of analogue of the variation of constants formula for nonlinear systems due to V.M. Alekseev[1]. Elaydi and Farran[9] introduced the notion of exponential asymptotic stability(EAS) which is a stronger notion than that of ULS, which is introduced by Dannan and Elaydi[8]. They investigated some analytic criteria for an autonomous differential system and its perturbed systems to be EAS. Pachpatte[15,16] investigated the stability and asymptotic behavior of solutions of the functional differential equation. Gonzalez and Pinto[10] proved theorems which relate the asymptotic behavior and boundedness of the solutions of nonlinear differential systems. Choi et al.[6,7] examined Lipschitz and exponential asymptotic stability for nonlinear functional systems. Goo[11] and Choi et al.[3,5] investigated Lipschitz and asymptotic stability for perturbed differential systems. Also, Im and Goo[13] investigated asymptotic property for solutions of the perturbed functional differential systems.
In this paper we will obtain some results on ULS and asymptotic property for perturbed nonlinear differential systems. We will employ the theory of integral inequalities to study ULS and asymptotic property for solutions of perturbed nonlinear differential systems.
2. PRELIMINARIES
We consider the nonautonomous differential system
where f ∈ C(ℝ+ × ℝn, ℝn), ℝ+ = [0, ∞) and ℝn is the Euclidean n-space. We assume that the Jacobian matrix fx = ∂f / ∂x exists and is continuous on ℝ+ × ℝn and f(t, 0) = 0. Also, we consider the perturbed differential system of (2.1)
where g ∈ C(ℝ+ × ℝn × ℝn, ℝn), h ∈ C(ℝ+ × ℝn, ℝn) , g(t, 0, 0) = 0, h(t, 0) = 0, and T : C(ℝ+, ℝn) → C(ℝ+, ℝn) is a continuous operator .
The symbol | · | will be used to denote any convenient vector norm in ℝn. For an n × n matrix A, define the norm |A| of A by |A| = sup|x|≤1 |Ax|.
Let x(t, t0, x0) denote the unique solution of (2.1) with x(t0, t0, x0) = x0, existing on [t0, ∞). Then we can consider the associated variational systems around the zero solution of (2.1) and around x(t), respectively,
and
The fundamental matrix Φ(t, t0, x0) of (2.4) is given by
and Φ(t, t0, 0) is the fundamental matrix of (2.3).
Before giving further details, we give some of the main definitions that we need in the sequel[9].
Definition 2.1. The system (2.1) (the zero solution x = 0 of (2.1)) is called (ULS) uniformly Lipschitz stable if there exist M > 0 and δ > 0 such that |x(t)| ≤ M|x0| whenever |x0| ≤ δ and t ≥ t0 ≥ 0,
(ULSV)uniformly Lipschitz stable in variation if there exist M > 0 and δ > 0 such that |Φ(t, t0, x0) ≤ M for |x0| ≤ δ and t ≥ t0 ≥ 0.
(EAS) exponentially asymptotically stable if there exist constants K > 0 , c > 0, and δ > 0 such that
|x(t)| ≤ K |x0|e−c(t−t0), 0 ≤ t0 ≤ t
provided that |x0| < δ,
(EASV) exponentially asymptotically stable in variation if there exist constants K > 0 and c > 0 such that
|Φ(t, t0, x0)| ≤ K e−c(t−t0), 0 ≤ t0 ≤ t
provided that |x0| < ∞
Remark 2.2 ([10]). The last definition implies that for |x0| ≤ δ
|x(t)| ≤ K |x0|e−c(t−t0), 0 ≤ t0 ≤ t.
For the proof we prepare some related properties. We need Alekseev formula to compare between the solutions of (2.1) and the solutions of perturbed nonlinear system
where g ∈ C(ℝ+ × ℝn, ℝn) and g(t, 0) = 0. Let y(t) = y(t, t0, y0) denote the solution of (2.5) passing through the point (t0, y0) in ℝ+ × ℝn.
The following is a generalization to nonlinear system of the variation of constants formula due to Alekseev [1].
Lemma 2.3 ([2]). Let x and y be a solution of (2.1) and (2.5), respectively. If y0 ∈ ℝn, then for all t ≥ t0 such that x(t, t0, y0) ∈ ℝn, y(t, t0, y0) ∈ ℝn,
Lemma 2.4. (Bihari−type Inequality) Let u, λ ∈ C(ℝ+), w ∈ C((0, ∞)) and w(u) be nondecreasing in u. Suppose that, for some c > 0,
Then
where t0 ≤ t < b1, , W−1(u) is the inverse of W(u), and
Lemma 2.5 ([4]). Let u, λ1, λ2, λ3, λ4, λ5, λ6 ∈ C(ℝ+), w ∈ C((0, ∞)) and w(u) be nondecreasing in u, u ≤ w(u). Suppose that for some c > 0,
Then
, where t0 ≤ t < b1, W, W−1 are the same functions as in Lemma 2.4, and
For the proof we need the following two corollaries from Lemma 2.5.
Corollary 2.6. Let u, λ1, λ2, λ3, λ4 ∈ C(ℝ+), w ∈ C((0, ∞)) and w(u) be nondecreasing in u, u ≤ w(u). Suppose that for some c > 0 and 0 ≤ t0 ≤ t,
.
Then
where t0 ≤ t < b1, W, W−1 are the same functions as in Lemma 2.4, and
.
Corollary 2.7. Let u, λ1, λ2, λ3 ∈ C(ℝ+), w ∈ C((0,∞)) and w(u) be nondecreasing in u, u ≤ w(u). Suppose that for some c > 0 and 0 ≤ t0 ≤ t,
Then
where t0 ≤ t < b1, W, W−1 are the same functions as in Lemma 2.4, and
Lemma 2.8 ([12]). Let u, λ1, λ2, λ3, λ4, λ5 ∈ C(ℝ+), w ∈ C((0, ∞)), and w(u) be nondecreasing in u, u ≤ w(u). Suppose that for some c > 0 and 0 ≤ t0 ≤ t,
Then
where t0 ≤ t < b1, W, W−1 are the same functions as in Lemma 2.4, and
For the proof we need the following corollary.
Corollary 2.9. Let u, λ1, λ2, λ3, λ4 ∈ C(ℝ+), w ∈ C((0, ∞)), and w(u) be nondecreasing in u, u ≤ w(u). Suppose that for some c > 0 and 0 ≤ t0 ≤ t,
Then
where t0 ≤ t < b1, W, W−1 are the same functions as in Lemma 2.4, and
.
3. MAIN RESULTS
In this section, we investigate ULS and asymptotic property for solutions of the perturbed nonlinear differential systems
To obtain ULS and asymptotic property, the following assumptions are needed:
(H1) The solution x = 0 of (1.1) is EASV. (H2) w(u) is nondecreasing in u, u ≤ w(u).
Theorem 3.1. Suppose that (H1), (H2), and the perturbing term g(t, y, Ty) satisfies
and
where α > 0, a, b, c, k, u, w ∈ C(ℝ+), a, b, c, k ∈ L1(ℝ+). If
where t ≥ t0 and c = |y0|Meαt0, then all solutions of (2.2) approach zero as t → ∞
Proof. Let x(t) = x(t, t0, y0) and y(t) = y(t, t0, y0) be solutions of (2.1) and (2.2), respectively. By the assumption (H1), the solution x = 0 of (2.1) is EASV. Therefore, it is EAS by remark 2.2. Using Lemma 2.3, together with (3.1) and (3.2), we have
It follows from (H2) that
Set u(t) = |y(t)|eαt. By Lemma 2.8 and (3.3) we obtain
where t ≥ t0 and c = M|y0|eαt0. The above estimation yields the desired result. □
Remark 3.2. Letting c(s) = 0 for t0 ≤ s ≤ t in Theorem 3.1, we obtain the same result as that of Theorem 3.1 in [13].
Theorem 3.3. Suppose that (H1), (H2), and the perturbing term g(t, y, Ty) satisfies
and
where α > 0, a, b, c, k, u, w ∈ C(ℝ+), a, b, c, k ∈ L1(ℝ+). If
where c = |y0|Meαt0, then all solutions of (2.2) approach zero as t → ∞
Proof. Let x(t) = x(t, t0, y0) and y(t) = y(t, t0, y0) be solutions of (2.1) and (2.2), respectively. By the assumption (H1), the solution x = 0 of (2.1) is EASV, and so it is EAS by remark 2.2. Applying Lemma 2.3, together with (3.4) and (3.5), we have
From (H2) , we obtain
Defining u(t) = |y(t)|eαt, then by corollary 2.9 and (3.6) we obtain
where t ≥ t0 and c = M|y0|eαt0. From the above estimation, we obtain the desired result. □
Remark 3.4. Letting c(s) = 0 for t0 ≤ s ≤ t in Theorem 3.3, we obtain the same result as that of Theorem 3.1 in [13].
Theorem 3.5. Suppose that (H1), (H2), and the perturbed term g(t, y, Ty) satisfies
and
where α > 0, a, b, c, k, u, w ∈ C(R+), a, b, c, k ∈ L1(ℝ+). If
where b1 = ∞ and c = M|y0|eαt0, then all solutions of (2.2) approach zero as t → ∞
Proof. Let x(t) = x(t, t0, y0) and y(t) = y(t, t0, y0) be solutions of (2.1) and (2.2), respectively. From (H1), the solution x = 0 of (2.1) is EASV. Therefore, it is EAS. Using Lemma 2.3, together with (3.7) and (3.8), we have
Applying (H2) , we obtain
Set u(t) = |y(t)|eαt. Then, it follows from Corollary 2.6 and (3.9) that
where t ≥ t0 and c = M|y0|eαt0. The above estimation yields the desired result. □
Remark 3.6. Letting b(s) = c(s) = 0 for t0 ≤ s ≤ t in Theorem 3.5, we obtain the same result as that of Corollary 3.8 in [5].
Theorem 3.7. Suppose that (H1), (H2), and the perturbed term g(t, y, Ty) satisfies
and
where α > 0, a, b, c, k, u, w ∈ C(ℝ+), a, b, c, k ∈ L1(ℝ+). If
where b1 = ∞ and c = M|y0|eαt0, then all solutions of (2.2) approach zero as t → ∞
Proof. Let x(t) = x(t, t0, y0) and y(t) = y(t, t0, y0) be solutions of (2.1) and (2.2), respectively. From the assumption (H1), the solution x = 0 of (2.1) is EASV, and so it is EAS. Using Lemma 2.3, together with (3.10) and (3.11), we have
By the assumption (H2) , we obtain
Set u(t) = |y(t)|eαt. Then, it follows from Corollary 2.7 and (3.12) that
where t ≥ t0 and c = M|y0|eαt0. From the above estimation, we obtain the desired result. □
Remark 3.8. Letting c(s) = 0 for t0 ≤ s ≤ t in Theorem 3.7, we obtain the same result as that of Theorem 3.3 in [13].
Theorem 3.9. For the perturbed (2.2), we suppose that (H2),
and
where a, b, c, d, k, q, u ∈ C(ℝ+), a, b, c, d, k, q ∈ L1(ℝ+), w ∈ C((0, ∞), for some v > 0, and
where M(t0) < ∞ and b1 = ∞. If the zero solution of (2.1) is ULSV, then the zero solution of (2.2) is ULS.
Proof. Let x(t) = x(t, t0, y0) and y(t) = y(t, t0, y0) be solutions of (2.1) and (2.2), respectively. Since x = 0 of (2.1) is ULSV, it is ULS by Theorem 3.3[8]. In view of Lemma 2.3, together with ULSV condition of x = 0 of (2.1), (3.13) and (3.14), we obtain
Set u(t) = |y(t)||y0|−1. Then, by Lemma 2.5, we have
.
The above estimation and (3.15) yield the desired result. Hence the proof is complete. □
Remark 3.10. Letting b(s) = c(s) = d(s) = 0 for t0 ≤ s ≤ t in Theorem 3.9, we obtain the same result as that of Corollary 3.4 in [5].
Theorem 3.11. For the perturbed (2.2), we suppose that (H2),
and
where a, b, c, k, q, u ∈ C(ℝ+), a, b, c, k, q ∈ L1(ℝ+) , w ∈ C((0, ∞), for some v > 0, and
where M(t0) < ∞ and b1 = ∞. If the zero solution of (2.1) is ULSV, then the zero solution of (2.2) ULS.
Proof. Let x(t) = x(t, t0, y0) and y(t) = y(t, t0, y0) be solutions of (2.1) and (2.2), respectively. Since x = 0 of (2.1) is ULSV, it is ULS. Using Lemma 2.3, together with ULSV condition of x = 0 of (2.1), (3.16), and (3.17) , we obtain
Set u(t) = |y(t)||y0|−1. Then, an application of Lemma 2.8 yields
.
Thus, by (3.18), we have |y(t)| ≤ M(t0)|y0| for some M(t0) > 0 whenever |y0| < δ. This completes the proof. □
Remark 3.12. Letting b(s) = c(s) = q(s) = 0 for t0 ≤ s ≤ t in Theorem 3.11, we obtain the same result as that of Corollary 3.2 in [5].
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- Lyapunov Functions and Lipschitz Stability for Riemann-Liouville Non-Instantaneous Impulsive Fractional Differential Equations vol.13, pp.4, 2016, https://doi.org/10.3390/sym13040730
- Lipschitz Stability in Time for Riemann-Liouville Fractional Differential Equations vol.5, pp.2, 2021, https://doi.org/10.3390/fractalfract5020037