POSITIVE PERIODIC SOLUTIONS OF A CLASS OF SECOND-ORDER DIFFERENTIAL EQUATIONS
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Submitted 1967-01-01 | SovietRxiv: ru-196701.41355 | Translated from Russian

Abstract Generated abstract

The paper studies positive periodic solutions of a nonlinear second-order differential equation with periodic coefficients, nonnegative nonlinearity, and a nonoscillation assumption on the associated linear equation. Using cone-theoretic methods, it gives sufficient conditions for the existence of nonnegative and positive periodic solutions in terms of upper and lower linear bounds on the nonlinearity and stability or instability of related linear equations. Additional results address Lyapunov stability and instability of positive periodic solutions under quasi-concavity or quasi-convexity assumptions, as well as uniqueness and exclusion of sign-changing periodic solutions under an integral condition. The paper also provides necessary and sufficient criteria, with an application-oriented corollary, for asymptotic stability and instability of the underlying linear periodic equation.

Full Text

UDC 517.917

Yu. S. KOLESOV

POSITIVE PERIODIC SOLUTIONS OF A CLASS OF SECOND-ORDER DIFFERENTIAL EQUATIONS

(Presented by Academician I. G. Petrovskii on 11 III 1966)

The article considers the question of the existence of positive \(\omega\)-periodic solutions of the nonlinear second-order equation

\[ \ddot{x}+p(t)\dot{x}+q(t)x=f(t,x), \tag{1} \]

where \(p(t)\) and \(q(t)\) are continuous \(\omega\)-periodic functions. With respect to the function \(f(t,x)\), it is assumed that it is continuous for \(-\infty<t<\infty\), \(x\ge 0\), \(\omega\)-periodic in \(t\), and nonnegative for nonnegative \(x\). In addition, throughout the article it is assumed that the solutions of the linear equation

\[ \ddot{x}+p(t)\dot{x}+q(t)x=0 \tag{2} \]

do not oscillate on \((t_0,\infty)\) (see \((^1,^2)\)) and that

\[ \int_0^\omega p(\tau)\,d\tau>0. \]

In the theorems formulated below, the linear equations

\[ \ddot{x}+p(t)\dot{x}+q(t)x-c_i(t)x=0 \quad (i=1,2,3,4). \tag{3} \]

will appear. Without specifying this each time, we shall assume that the functions \(c_i(t)\) \((i=1,2,3,4)\) are continuous, nonnegative, and \(\omega\)-periodic.

  1. Theorem 1. Suppose the inequality

\[ f(t,x)\le c_1(t)x+a \quad (x\ge 0,\ 0\le t\le \omega) \tag{4} \]

is satisfied.

Suppose the zero solution of equation (3) \((i=1)\) is asymptotically stable.

Then equation (1) has at least one nonnegative \(\omega\)-periodic solution.

  1. In the remainder of the article it is assumed that \(f(t,0)\equiv 0\) \((0\le t\le \omega)\), and the question of the existence of nonzero periodic solutions is considered.

Theorem 2. Suppose condition (4) is satisfied, and suppose that for small nonnegative \(x\)

\[ f(t,x)\ge c_2(t)x \quad (0\le t\le \omega). \]

Finally, suppose the zero solution of equation (3) \((i=2)\) is unstable.

Then equation (1) has at least one positive \(\omega\)-periodic solution.

Theorem 3. Suppose that, for small nonnegative \(x\), the inequality

\[ f(t,x)\le c_3(t)x \quad (0\le t\le \omega), \]

and for all nonnegative \(x\)

\[ f(t,x)\geq c_4(t)x-b \qquad (0\leq t\leq \omega). \]

Finally, suppose that the zero solution of equation (3) \((i=3)\) is asymptotically stable, while the zero solution of equation (3) \((i=4)\) is unstable. Then equation (1) has at least one positive \(\omega\)-periodic solution.

  1. Following M. A. Krasnosel’skii \((^3)\), we shall call a function \(f(t,x)\) quasi-concave if

\[ f(t,\tau x)\geq \tau f(t,x) \qquad (0\leq t\leq \omega,\ x\geq 0,\ 0<\tau<1). \]

Similarly, if

\[ f(t,\tau x)\leq \tau f(t,x) \qquad (0\leq t\leq \omega,\ x\geq 0,\ 0<\tau<1), \]

then we shall call the function \(f(t,x)\) quasi-convex.

Theorem 4. Suppose that the function \(f(t,x)\) is quasi-concave and that it is nondecreasing in the second variable for \(x\geq 0\). Further, suppose that for some \(0\leq t_1\leq \omega\) and \(x>0\)

\[ f(t_1,\tau x)>\tau f(t_1,x) \qquad (0<\tau<1). \]

Then, under the conditions of Theorems 1 and 2, equation (1) has a positive \(\omega\)-periodic solution asymptotically stable in the sense of Lyapunov.

Theorem 5. Suppose that the function \(f(t,x)\) is quasi-convex. Suppose that for some \(0\leq t_2\leq \omega\) and \(x>0\)

\[ f(t_2,\tau x)<\tau f(t_2,x) \qquad (0<\tau<1). \]

Then, under the conditions of Theorem 3, equation (1) has an unstable positive \(\omega\)-periodic solution.

  1. A natural question arises about the number of \(\omega\)-periodic solutions of equation (1). We give one result.

Theorem 6. Suppose that for all \(0\leq t\leq \omega\) the inequality

\[ \int_t^{t+\omega}\exp\left[\int_0^s p(\tau)\,d\tau\right]q(s)\,ds\geq 0 \]

is satisfied.

Then, under the conditions of Theorems 4 and 5, equation (1) has a unique positive \(\omega\)-periodic solution and has no sign-changing \(\omega\)-periodic solutions.

All the theorems formulated above are obtained by methods of cone theory (see \((^{3-5})\)).

  1. The question of the stability of solutions of the linear equation (2) under various assumptions has been studied by many authors (see, for example, \((^{6-8})\)). Here we shall give criteria for stability and instability of solutions of equation (2) which, as it seems to us, are convenient for applications of the theorems of the preceding sections.

Theorem 7. In order that the zero solution of equation (2) be asymptotically stable, it is necessary and sufficient that there exist a continuously differentiable function \(\varphi_1(t)\) \((t_0\leq t\leq t_0+\omega)\) such that

\[ \varphi_1(t_0)\leq \varphi_1(t_0+\omega),\qquad \int_0^\omega p(\tau)\,d\tau \geq 2\int_{t_0}^{t_0+\omega}\varphi_1(\tau)\,d\tau \geq 0, \]

\[ \varphi_1'(t)\leq \varphi_1^2(t)-p(t)\varphi_1(t)+q(t), \]

moreover, if

\[ \int_{t_0}^{t_0+\omega}\varphi_1(\tau)\,d\tau=0, \]

then

\[ \dot{\varphi}_1(t^*)<\varphi_1^2(t^*)-p(t^*)\varphi_1(t^*)+q(t^*) \]

for some \(t_0\leqslant t^*\leqslant t_0+\omega\).

We present one corollary of Theorem 7.

Theorem 8. Suppose that the function \(q(t)\ne 0\). Suppose that the inequality

\[ \int_0^\omega dt\int_t^{t+\omega}\exp\left[-\int_s^t p(\tau)\,d\tau\right]q(s)\,ds\geqslant 0 \]

is satisfied. Then the zero solution of equation (2) is asymptotically stable.

Theorem 9. In order that the zero solution of equation (2) be unstable, it is necessary and sufficient that there exist a continuously differentiable function \(\varphi_2(t)\) \((t_0\leqslant t\leqslant t_0+\omega)\) such that

\[ \varphi_2(t_0)\geqslant \varphi_2(t_0+\omega), \]

\[ \int_{t_0}^{t_0+\omega}\varphi_2(\tau)\,d\tau\leqslant 0, \]

\[ \dot{\varphi}_2(t)\geqslant \varphi_2^2(t)-p(t)\varphi_2(t)+q(t), \]

moreover, if

\[ \int_{t_0}^{t_0+\omega}\varphi_2(\tau)\,d\tau=0, \]

then

\[ \dot{\varphi}_2(t^*)>\varphi_2^2(t^*)-p(t^*)\varphi_2(t^*)+q(t^*) \]

for some \(t_0\leqslant t^*\leqslant t_0+\omega\).

In conclusion the author expresses his gratitude to M. A. Krasnosel’skii and A. Yu. Levin for discussion of the results of the present article.

Voronezh State
University

Received
4 III 1966

REFERENCES

  1. R. Bellman, Stability Theory of Differential Equations, Moscow, 1954.
  2. A. Yu. Levin, UMN, 20, issue 2 (122) (1965).
  3. M. A. Krasnosel’skii, Operator of translation along the trajectories of differential equations, “Nauka,” 1966.
  4. M. A. Krasnosel’skii, Positive Solutions of Operator Equations, Moscow, 1962.
  5. Yu. S. Kolesov, M. A. Krasnosel’skii, DAN, 145, No. 6 (1962).
  6. V. M. Starzhinskii, Prikl. matem. i mekh., 18, 469 (1954).
  7. V. M. Starjinsky, Bul. Inst. Politechn. Iași, 4, No. 3–4, 19 (1958).
  8. V. A. Yakubovich, DAN, 87, No. 3 (1952).

Submission history

POSITIVE PERIODIC SOLUTIONS OF A CLASS OF SECOND-ORDER DIFFERENTIAL EQUATIONS