<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2019.712210</article-id><article-id pub-id-type="publisher-id">JAMP-96972</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Double Lipschitz Stability for Nonlinearly Perturbed Differential Systems with Multiple Delay
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ran</surname><given-names>Huo</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xiaoli</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Science, Inner Mongolia Agricultural University, Huhhot, China</addr-line></aff><aff id="aff2"><addr-line>College of Statistics and Mathematics, Inner Mongolia University of Finance and Economics, Huhhot, China</addr-line></aff><pub-date pub-type="epub"><day>02</day><month>12</month><year>2019</year></pub-date><volume>07</volume><issue>12</issue><fpage>3003</fpage><lpage>3011</lpage><history><date date-type="received"><day>6,</day>	<month>November</month>	<year>2019</year></date><date date-type="rev-recd"><day>6,</day>	<month>December</month>	<year>2019</year>	</date><date date-type="accepted"><day>9,</day>	<month>December</month>	<year>2019</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, firstly a new class of time-delay differential inequality is proved. Then as an application, the nonlinearly perturbed differential systems with multiple delay are considered and it is obtained that the trivial solution of the nonlinear systems with multiple delay has uniform stability and uniform exponential Lipschitz asymptotic stability with respect to partial variables. It is obvious that the above system is a generalization of the traditional differential systems. The aim of this paper is to investigate the double stability of time-delay differential equations, including Uniform stability and Uniform Lipschitz stability. The author uses the method of differential inequalities with time-delay and integral inequalities to establish double stability criteria. As a result, the partial stability of differential equations is widely used both in theory and in practice such as dynamic systems and control systems.
 
</p></abstract><kwd-group><kwd>Time-Delay</kwd><kwd> Nonlinear Systems</kwd><kwd> Double Stability</kwd><kwd> Differential Inequality</kwd><kwd> Integral Inequality</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In 1892, Lyapunov, a Russian mathematician, mechanician and physicist, proposed the notion of the stability of motion. He gave the general research methods in his doctoral dissertation “The general problem of the stability of motion” [<xref ref-type="bibr" rid="scirp.96972-ref1">1</xref>], in which he established the foundation of the stability theory. When studying nonlinear systems, especially studying dynamic systems or control systems, we cannot study the stability of all variables because of the technology difficulties, the limitation of practical conditions, or it is not necessary to study all variables considering the actual need. As a result, studying the partial stability of differential equations becomes more important. In addition, the partial stability is widely used in science and technology. For instance, the absolute stability of famous Lurie adjusting systems can be changed into a problem of partial stability. In a word, it is of practical significance to study the partial stability of differential equations.</p><p>In 1986, Dannan and Elaydi ( [<xref ref-type="bibr" rid="scirp.96972-ref2">2</xref>] ) introduced a new notion of stability, which is called uniform Lipschitz stability (ULS), for systems of differential equations</p><p>d x d t = f ( t , x ) , (1)</p><p>where f ∈ C [ J &#215; R n , R n ] , J = [ 0 , ∞ ) , f ( t , 0 ) = 0 , and x ( t , t 0 , x 0 ) ≡ x ( t ) is the solution of (1) with x ( t 0 , t 0 , x 0 ) = x 0 , where t 0 ≥ 0 .</p><p>This notion of ULS lies somewhere between uniform stability (US) on one side and the notions of asymptotic stability in variation (ASV) and uniform stability in variation (USV) on the other side. An important feature of ULS is that the linearized system inherits the property of ULS from the original nonlinear system.</p><p>YU-LI Fu ( [<xref ref-type="bibr" rid="scirp.96972-ref3">3</xref>] ) considers the system with time-delay</p><p>d x d t = f ( t , x t ) , (2)</p><p>where x ∈ R n , f : R &#215; C ( [ − r , 0 ] , R n ) ↦ R n , f ( t , 0 ) = 0 , f is continuous, x t = x ( t + θ ) , θ ∈ [ − r , 0 ] , r &gt; 0 .</p><p>Sung Kyu Choi, Ki Shik Koo and Keonhee Lee ( [<xref ref-type="bibr" rid="scirp.96972-ref4">4</xref>] ) investigated the problems of ULS, EAS and GEASV for the following various perturbed differential systems of the nonlinear differential system (1) and</p><p>d x d t = A ( t ) x + g ( t , x ) , (3)</p><p>d x d t = f ( t , x ) + g ( t , x ) , (4)</p><p>where A ( t ) is a continuous n &#215; n matrix defined on R + , g ( t , x ) ∈ C ( R + &#215; R n , R n ) with g ( t , 0 ) = 0 .</p><p>Vorotnikov, V. I. ( [<xref ref-type="bibr" rid="scirp.96972-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.96972-ref6">6</xref>] ) considered the following system</p><p>{ d y d t = A ( t ) y + B ( t ) z + Y ( t , y , z ) d z d t = C ( t ) y + D ( t ) z + Z ( t , y , z ) , (5)</p><p>and studied the double stability as ‖ y ‖ + ‖ z ‖ → 0 and ‖ Y ( t , y , z ) ‖ + ‖ Z ( t , y , z ) ‖ ‖ y ‖ + ‖ z ‖ → 0 .</p><p>In this paper, the author considers a new class of the nonlinearly perturbed differential systems with time-delay</p><p>d x d t = A ( t ) x + f ( t , x ( t ) , x ( t − τ ) , ∫ 0 t h ( s , x ( s ) , x ( s − τ ) ) d s ) , (6)</p><p>where x ∈ R n , y = c o l ( x 1 , x 2 , ⋯ , x m ) , z = c o l ( x m + 1 , x m + 2 , ⋯ , x n ) , x = c o l ( y , z ) , f : R &#215; R n &#215; C ( [ − r , 0 ] , R n ) &#215; R n ↦ R n , f ( t , 0 , 0 , 0 ) ≡ 0 , h : R &#215; R n &#215; C ( [ − r , 0 ] , R n ) ↦ R n , τ is a non-negative constant.</p><p>It is obvious that the above system is a generalization of the systems in [<xref ref-type="bibr" rid="scirp.96972-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.96972-ref6">6</xref>]. The aim of this paper is to investigate the double stability of time-delay differential equations, including Uniform stability and Uniform Lipschitz stability. The author uses the method of differential inequalities with time-delay and integral inequalities to establish double stability criteria.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>1) Definitions and lemmas</p><p>Consider the following system:</p><p>d x d t = f ( t , x , x ( t − τ ) ) , (7)</p><p>where x ∈ R n , y = c o l ( x 1 , x 2 , ⋯ , x m ) , z = c o l ( x m + 1 , x m + 2 , ⋯ , x n ) , x = c o l ( y , z ) , f ( t , 0 , 0 ) ≡ 0 , τ is a non-negative constant. Let ϕ ( t ) be a continuous function, for ∀ t ∈ E t 0 = [ t 0 − τ , t 0 ] .</p><p>Definition 1: The trivial solution of system (7) has uniform stability and exponential asymptotic stability with respect to y if, for ∀ ε &gt; 0 , ∀ t 0 ∈ I , ∃ δ ( ε ) &gt; 0 and λ &gt; 0 , when ‖ ϕ ‖ &lt; δ (for ∀ t ∈ E t 0 ), such that ‖ x ( t ; t 0 , ϕ ) ‖ &lt; ε , ‖ y ( t ; t 0 , ϕ ) ‖ &lt; ε exp ( − λ ( t − t 0 ) ) , for all t ≥ t 0 .</p><p>Definition 2: The trivial solution of system (7) has Lipschitz stability with respect to y if, there exist constants M ( t 0 ) &gt; 0 and δ ( t 0 ) &gt; 0 , when ‖ ϕ ‖ &lt; δ (for ∀ t ∈ E t 0 ), such that ‖ y ( t ; t 0 , ϕ ) ‖ ≤ M ( t 0 ) ‖ ϕ ‖ , for all t ≥ t 0 ≥ 0 .</p><p>Definition 3: The trivial solution of system (7) has equi-exponential Lipschitz asymptotic stability with respect to y if, there exist constants λ &gt; 0 , K ( t 0 ) &gt; 0 and δ ( t 0 ) &gt; 0 , when ‖ ϕ ‖ &lt; δ (for ∀ t ∈ E t 0 ), such that ‖ y ( t ; t 0 , ϕ ) ‖ ≤ K ( t 0 ) ‖ ϕ ‖ exp ( − λ ( t − t 0 ) ) , for all t ≥ t 0 ≥ 0 .</p><p>Definition 4: The trivial solution of system (7) has uniform exponential Lipschitz asymptotic stability with respect to y if, K and δ in Definition3 are unrelated to t 0 .</p><p>Lemma 1. [<xref ref-type="bibr" rid="scirp.96972-ref7">7</xref>] Consider the homogeneous system</p><p>{ d y d x = B ( t ) y + C ( t ) z d z d x = D ( t ) y + E ( t ) z , (8)</p><p>if the trivial solution of system (8) has uniform stability, and has exponential asymptotic stability with respect to y, then there exists a Lyapunov-function V ( t , x ) satisfied the following conditions:</p><p>‖ y ‖ ≤ V ( t , x ) ≤ M ‖ x ‖ ,     V ˙ | ( 8 ) ≤ − α V ( t , x ) ,</p><p>where M &gt; 0 .</p><p>Consider the following inequality:</p><p>x ˙ i ( t ) ≤ f i ( t ) [ − r i x i ( t ) + h i ( 1 ) ( x t ) x t α i + ∫ − ∞ t h i ( 2 ) ( t − s , x ( s ) ) x β i ( t ) e − ε ( t − s ) d s ] , (9)</p><p>where f i ( t ) ∈ C [ R , R + ] and f i ( t ) ≥ β = c o n s t &gt; 0 , r i = c o n s t &gt; 0 , ( i = 1 , 2 , ⋯ , m ) , h i ( 1 ) ( ⋅ ) , h i ( 2 ) ( t − θ , ⋅ ) are nonnegative and not monotone decreasing for “ ⋅ ”, α i , β i ≥ 1 , x ( θ ) ≜ max 1 ≤ j ≤ n ( x j ( θ ) ) , x t ≜ max 1 ≤ j ≤ n ( sup t − τ ≤ θ ≤ t x j ( θ ) ) , τ = c o n s t &gt; 0 , α ≜ max ( α i , β i ) .</p><p>Lemma 2. [<xref ref-type="bibr" rid="scirp.96972-ref8">8</xref>] Suppose x i ( t ) be nonnegative continuous on R + , for all t ≥ t 0 (3) is satisfied, if ∃ K = c o n s t the following inequality holds:</p><p>h i ( 1 ) ( K ) + ∫ 0 + ∞ h i ( 2 ) ( s , K ) d s &lt; r i , α K 1 − 1 α &lt; 1 ,</p><p>when M α ≜ max 1 ≤ j ≤ n ( sup t 0 − τ ≤ θ ≤ t 0 x j ( θ ) ) &lt; K , we have following result:</p><p>x i ( t ) ≤ M exp ( − λ ( t − t 0 ) ) ,</p><p>holds true, where t ≥ t 0 , and λ &gt; 0 .</p><p>2) Differential Inequalities with Time-Delay</p><p>Consider the following inequality</p><p>x ˙ i ( t ) ≤ f i ( t ) [ − r i x i ( t ) + h i ( 1 ) ( x t ) x t α i + ∫ − ∞ t h i ( 2 ) ( t − s , x ( s ) ) x β i ( t ) e − ε ( t − s ) d s ] , (10)</p><p>where f i ( t ) ∈ C [ R , R + ] and f i ( t ) ≥ γ = c o n s t &gt; 0 , r i = c o n s t &gt; 0 , h i ( 1 ) ( ⋅ ) , h i ( 2 ) ( t − θ , ⋅ ) ( i = 1 , 2 , ⋯ , n ) are nonnegative and not monotone ecreasing for “ ⋅ ”, α i , β i ≥ 1 , x ( θ ) = max 1 ≤ i ≤ n ( x i ( θ ) ) , x t = max 1 ≤ i ≤ n ( sup t − τ &lt; θ &lt; t x i ( θ ) ) , τ = c o n s t &gt; 0 , α = max ( α i , β i ) .</p><p>Lemma 3. Assume x i ( t ) be nonnegative continuous on R + , (10) is satisfied for all t ≥ t 0 , there exists a constant K satisfied the following inequality:</p><p>h i ( 1 ) ( K ) + ∫ 0 + ∞ h i ( 2 ) ( s , K ) d s &lt; r i , (11)</p><p>and</p><p>α K 1 − 1 α &lt; 1 ,</p><p>then if<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x113.png" xlink:type="simple"/></inline-formula>, the following inequality:</p><p>x i ( t ) ≤ M exp ( − λ ( t − t 0 ) )   ( i = 1 , 2 , ⋯ , n )</p><p>holds true, where t ≥ t 0 and λ &gt; 0 .</p><p>Proof</p><p>According to (10), for ∀ ε &gt; 0 , ∃ λ (let λ &lt; ε α ) we can get</p><p>− r i + α λ γ + e α λ τ h i ( 1 ) ( K ) + ∫ 0 + ∞ h i ( 2 ) ( s , K ) d s &lt; 0.</p><p>Now define</p><p>P i ( t ) ≜ { x i α ( t ) e α λ ( t − t 0 ) , t ≥ t 0 ;   ( 12 ) x i α ( t ) ,     t ∈ [ t 0 − τ , t 0 ] ,   ( i = 1 , 2 , ⋯ , n )</p><p>thus, we can have</p><p>x i ( t ) = P i 1 α ( t ) e − λ ( t − t 0 ) ,</p><p>furthermore</p><p>x ˙ i ( t ) = ( 1 α P i 1 α − 1 ( t ) P ˙ i ( t ) − λ P i 1 α ( t ) ) e − λ ( t − t 0 ) . (13)</p><p>Let</p><p>P t = max 1 ≤ i ≤ n ( sup t − τ &lt; θ &lt; t P i ( θ ) ) ,   P ( θ ) = max 1 ≤ i ≤ n ( P i ( θ ) ) ,</p><p>obviously</p><p>P t ≥ x t α ,     P ( θ ) ≥ x α ( θ ) ,</p><p>hence</p><p>x ˙ i ( t ) = ( 1 α P i 1 α − 1 ( t ) P ˙ i ( t ) − λ P i 1 α ( t ) ) e − λ ( t − t 0 ) ≤ f i ( t ) [ − r i x i ( t ) + h i ( 1 ) ( x t ) x t α i + ∫ − ∞ t h i ( 2 ) ( t − s , x ( s ) ) x β i ( t ) e − ε ( t − s ) d s ] .</p><p>Notice that</p><p>x t α = max 1 ≤ i ≤ n ( sup t − τ &lt; θ &lt; t x i α ( θ ) ) = max 1 ≤ i ≤ n ( sup t − τ &lt; θ &lt; t x i α ( θ ) ) = max 1 ≤ i ≤ n ( sup t − τ &lt; θ &lt; t P i ( θ ) e − α λ ( θ − t 0 ) ) = max 1 ≤ i ≤ n ( sup t − τ &lt; θ &lt; t P i ( θ ) ) e − α λ ( t − τ − t 0 ) = P t e − α λ ( t − t 0 ) e α λ τ ,</p><p>and</p><p>x α ( θ ) = max 1 ≤ i ≤ n ( x i α ( θ ) ) = max 1 ≤ i ≤ n ( P i ( θ ) e − α λ ( θ − t 0 ) ) = max 1 ≤ i ≤ n ( P i ( θ ) e − α λ ( θ − t 0 ) ) = max 1 ≤ i ≤ n ( P i ( θ ) ) e − α λ ( θ − t 0 ) = P ( θ ) e − α λ ( θ − t 0 ) .</p><p>Applying (12) into (10), we have</p><p>P ˙ i ( t ) ≤ f i ( t ) [ − ( r i − α λ γ ) P i ( t ) + ( h i ( 1 ) ( x t ) P t e α λ τ     + ∫ 0 + ∞ h i ( 2 ) ( t − s , x ( s ) ) P ( s ) d s ) α P i 1 − 1 α ( t ) ] . (14)</p><p>For any scaler l ∈ ( 1 , K M α ) , we can get</p><p>P i ( t ) ≤ l M α ≜ N .</p><p>If not, then P i ( t ) &lt; N , thus there exists a certain i in ( − ∞ , t 0 ] and t 1 &gt; t 0 , we have</p><p>P i ( t 1 ) = N ,   P j ( t ) { &lt; N ,     j = i ,     t ∈ ( − ∞ , t 1 ) ; ≤ N ,     j ≠ i ,     t ∈ ( − ∞ , t 1 ] ,</p><p>thus we can get P ˙ i ( t 1 ) ≥ 0 . Using it in (14), we get</p><p>P ˙ i ( t 1 ) ≤ f i ( t 1 ) [ − ( r i − α λ β ) P i ( t 1 ) + ( h i ( 1 ) ( x t 1 ) P t 1 e α λ τ     + ∫ − ∞ t 1 h i ( 2 ) ( t 1 − s , x ( s ) ) P ( s ) d s ) α P i 1 − 1 α ( t 1 ) ] ≤ f i ( t 1 ) [ − ( r i − α λ β ) K + ( h i ( 1 ) ( K ) K e α λ τ + ∫ 0 + ∞ h i ( 2 ) ( s , K ) K d s ) α K 1 − 1 α ] ≤ f i ( t 1 ) [ − ( r i − α λ β ) + ( h i ( 1 ) ( K ) e α λ τ + ∫ 0 + ∞ h i ( 2 ) ( s , K ) d s ) ] K &lt; 0.</p><p>It is a contradictory, thus P i ( t ) ≤ l M α , let l → 1 , we can get</p><p>P i ( t ) ≤ M α .</p><p>Notice (12), the following is obtained</p><p>x i ( t ) ≤ M exp ( − λ ( t − t 0 ) ) , for all t ≥ t 0 .</p><p>Remark It is obvious that when α i = 1 , β i = 1 lemma 2 can be deduced by lemma 3.</p></sec><sec id="s3"><title>3. Main Results</title><p>Consider the following system which is equivalent with system (1)</p><p>{ d y d t = B ( t ) y + C ( t ) z + Y ( t , y ( t ) , z ( t ) , ∫ 0 t h 1 ( s , y ( s ) , z ( s ) , y ( s − τ ) , z ( s − τ ) ) d s ) d x d t = D ( t ) y + E ( t ) z + Z ( t , y ( t ) , z ( t ) , ∫ 0 t h 2 ( s , y ( s ) , z ( s ) , y ( s − τ ) , z ( s − τ ) ) d s ) (15)</p><p>where x = ( y , z ) T , τ ≥ 0 is a constant, initial condition is:</p><p>x ( t ) = φ ( t ) , t 0 − τ ≤ t ≤ t 0 ,</p><p><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x149.png" xlink:type="simple"/></inline-formula>is an <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x150.png" xlink:type="simple"/></inline-formula> matrix, <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x151.png" xlink:type="simple"/></inline-formula> is an <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x152.png" xlink:type="simple"/></inline-formula> matrix, <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x153.png" xlink:type="simple"/></inline-formula>is an <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x154.png" xlink:type="simple"/></inline-formula> matrix, they are all continuous for <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x155.png" xlink:type="simple"/></inline-formula> and satisfy the condition of existence and uniqueness theorem.</p><p>The homogeneous system of (15) is</p><p><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x156.png" xlink:type="simple"/></inline-formula>. (15)*</p><p>Theorem: If (15) satisfies the following conditions:</p><p>1)<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x157.png" xlink:type="simple"/></inline-formula>.</p><p>2)<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x158.png" xlink:type="simple"/></inline-formula>.</p><p>3)<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x159.png" xlink:type="simple"/></inline-formula>.</p><p>where<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x160.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x161.png" xlink:type="simple"/></inline-formula>are nonnegative and not monotone decreasing for “<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x162.png" xlink:type="simple"/></inline-formula>”, <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x163.png" xlink:type="simple"/></inline-formula>, and</p><p><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x164.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/7-1721753x165.png" xlink:type="simple"/></inline-formula>,</p><p>then the trivial solution of system (15) has uniform exponential Lipschitz asymptotic stability with respect to y, when the trivial solution of system (15)* has uniform stability and exponential asymptotic stability with respect to y.</p><p>Proof The V-Ляпунов function of (15)*, which is obtained under the condition of theorem, satisfies following conditions:</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x166.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x167.png" xlink:type="simple"/></inline-formula>, (16)</p><p><img data-original="//html.scirp.org/file/7-1721753x168.png" />, (<img data-original="//html.scirp.org/file/7-1721753x169.png" />), (17)</p><p>for<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x170.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x171.png" xlink:type="simple"/></inline-formula>.</p><p>Derivative the V-Ляпунов function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x172.png" xlink:type="simple"/></inline-formula> along (15), we get</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x173.png" xlink:type="simple"/></inline-formula>,</p><p>where</p><disp-formula id="scirp.96972-formula3"><graphic  xlink:href="//html.scirp.org/file/7-1721753x174.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.96972-formula4"><graphic  xlink:href="//html.scirp.org/file/7-1721753x175.png"  xlink:type="simple"/></disp-formula><p>here <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x176.png" xlink:type="simple"/></inline-formula> the notation of inner product.</p><p>From condition of theorem and (17), when <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x177.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.96972-formula5"><graphic  xlink:href="//html.scirp.org/file/7-1721753x178.png"  xlink:type="simple"/></disp-formula><p>By the first inequality of (16), the above can be expressed as follow:</p><disp-formula id="scirp.96972-formula6"><graphic  xlink:href="//html.scirp.org/file/7-1721753x179.png"  xlink:type="simple"/></disp-formula><p>then there exists <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x180.png" xlink:type="simple"/></inline-formula> such that when <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x181.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x182.png" xlink:type="simple"/></inline-formula>, we get</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x183.png" xlink:type="simple"/></inline-formula>,</p><p>here select the appropriate small constant r such that</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x184.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x185.png" xlink:type="simple"/></inline-formula>,</p><p>hence by the lemma [<xref ref-type="bibr" rid="scirp.96972-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.96972-ref10">10</xref>], there exists <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x186.png" xlink:type="simple"/></inline-formula> such that for all <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x187.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.96972-formula7"><label>. (18)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/7-1721753x188.png"  xlink:type="simple"/></disp-formula><p>For any solution of (15), from the inequality (18) and the first inequality of (16) we obtain</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x189.png" xlink:type="simple"/></inline-formula>.</p><p>According to the proof of the theorem in [<xref ref-type="bibr" rid="scirp.96972-ref11">11</xref>], we get<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/7-1721753x190.png" xlink:type="simple"/></inline-formula>, hence we obtain that the trivial solution of system (15) has uniform stability and uniform exponential Lipschitz asymptotic stability with respect to y.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, we use the method of differential inequalities with time-delay and integral inequalities to establish double stability criteria. As a result, studying the partial stability of differential equations becomes more important. In addition, the partial stability of differential equations is widely used in science and technology.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors are grateful to Professor Si Ligeng and the referee for several helpful comments.</p></sec><sec id="s6"><title>Supported</title><p>Supported by Inner Mongolia Autonomous Region Higher Education Research Project (No.NJZY17064, NJZY16141).</p></sec><sec id="s7"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Huo, R. and Wang, X.L. (2019) Double Lipschitz Stability for Nonlinearly Perturbed Differential Systems with Multiple Delay. Journal of Applied Mathematics and Physics, 7, 3003-3011. https://doi.org/10.4236/jamp.2019.712210</p></sec></body><back><ref-list><title>References</title><ref id="scirp.96972-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Lyapunov, A.M. (1892) The General Problem of the Stability of Motion. Doctor Dissertation, University of Moscow, Moscow.</mixed-citation></ref><ref id="scirp.96972-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Dannan, F.M. and Elaydi, S. (1986) Lipschitz Stability of Nonlinear Differential Equations. Journal of Mathematical Analysis and Applications, 113, 562-577. https://doi.org/10.1016/0022-247X(86)90325-2</mixed-citation></ref><ref id="scirp.96972-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Fu, Y.L. (1991) On Lipschitz Stablity for F.D.E. 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