ON THE QUESTION OF ESTIMATING THE INTERVAL OF APPLICABILITY OF CHAPLYGIN’S THEOREM
V. S. BEZDOMNIKOV, Yu. V. KOMLENKO
Submitted 1966-01-01 | SovietRxiv: ru-196601.18889 | Translated from Russian

Full Text

UDC 517.934.9

ON THE QUESTION OF ESTIMATING THE INTERVAL OF APPLICABILITY OF CHAPLYGIN’S THEOREM

V. S. BEZDOMNIKOV, Yu. V. KOMLENKO

Consider the problem

\[ L[y]\equiv y^{(n)}+\sum_{k=0}^{n-1} g_k(t)y^{(k)}=0, \tag{1} \]

\[ y^{(i)}(a)=y^{(m)}(b)=0 \quad (i=0,1,\ldots,n-2;\; m\leq n-1). \tag{2} \]

We shall assume the coefficients of the operation \(L[y]\) to be continuous. We shall call \([0,R)\) a subcritical interval of the problem (1), (2) if, for any \(a,b\in[0,R)\) (\(a<b\)), the problem (1), (2) has a unique solution. An interval \([0,T)\) on which every solution of equation (1) has no more than \(n-1\) zeros, counting a multiple zero as many times as its multiplicity, will be called an interval of nonoscillation of equation (1).

Below we propose methods, based on the ideas of [1, 2], for obtaining estimates of the subcritical interval of the problem (1), (2).

  1. Let \(u_0(t),u_1(t),\ldots,u_{n-1}(t)\) be a fundamental system of equation (1), and let \(W(t)\) be the Wronskian of this system,

\[ C(t,s)=\frac{1}{W(s)} \begin{vmatrix} u_0(s) & u_1(s) & \cdots & u_{n-1}(s)\\ u'_0(s) & u'_1(s) & \cdots & u'_{n-1}(s)\\ \cdots & \cdots & \cdots & \cdots\\ u_0^{(n-2)}(s) & u_1^{(n-2)}(s) & \cdots & u_{n-1}^{(n-2)}(s)\\ u_0(t) & u_1(t) & \cdots & u_{n-1}(t) \end{vmatrix} \]

is called the Cauchy function of equation (1). It is not difficult to verify that

\[ K(t,s)=\frac{(t-s)^{\,n-1}}{(n-1)!} \]

is the Cauchy function of the equation \(y^{(n)}=f(t)\), and the Green’s function for this equation with boundary conditions (2) has the form

\[ G(t,s)= \begin{cases} K(t,s)-\dfrac{K^{(m)}(b,s)K(t,a)}{K^{(m)}(b,a)}, & (t>s),\\[1.2em] -\dfrac{K^{(m)}(b,s)K(t,a)}{K^{(m)}(b,a)}, & (t\leq s). \end{cases} \]

Let \(H_k\) be numbers such that ...

\[ H_k \geq \sup_{t,s\in [a,b]}\left|\frac{K^{(k)}(s,a)}{K^{(i)}(t,a)}\,G^{(i)}(t,s)\right| \tag{3} \]

\[ (i,\ k=0,\ 1,\ \ldots,\ n-1) \]

for any \(a,\ b\in [0,R)\). A direct calculation shows that

\[ H_k=\frac{(n-m-1)^{\,n-m-1}(n-k-1)^{\,n-k-1}} {(n-k-1)!(2n-m-k-2)^{\,2n-m-k-2}}\,R^{\,n-k-1} \tag{4} \]

satisfy inequality (3) for any \(a,\ b\in [0,R)\).

Consider the operation

\[ L_1[y]\equiv y^{(n)}+\sum_{k=0}^{n-1}p_k(t)y^{(k)}, \]

where \(p_k(t)=g_k(t)\) \((k=1,\ 2,\ldots,\ n-1)\), \(p_0(t)=\max_{t\in[a,b]}[0,g_0(t)]\). By the comparison theorem (see [5]), the subcritical interval for the equation \(L_1[y]=0\) with boundary conditions (2) is contained in the subcritical interval of problem (1), (2). Taking this into account, we shall prove the following assertion.

Theorem 1. If

\[ \sum_{k=0}^{n-1} H_k \int_0^R |p_k(t)|\,dt <1, \]

then \([0,R)\) is a subcritical interval of problem (1), (2).

Proof. Rewrite the equation \(L_1[y]=0\) in the form

\[ y^{(n)}=-\sum_{k=0}^{n-1}p_k(t)y^{(k)}. \tag{5} \]

Then problem (5), (2) is equivalent to the equation

\[ y(t)=-\sum_{k=0}^{n-1}\int_a^b G(t,s)p_k(s)y^{(k)}(s)\,ds \]

or, if we put \(y^{(k)}(t)=x_k(t)\), to the system

\[ x_i(t)=-\sum_{k=0}^{n-1}\int_a^b G^{(i)}(t,s)p_k(s)x_k(s)\,ds \tag{6} \]

\[ (i=0,\ 1,\ldots,\ n-1). \]

By virtue of Theorem 4 of [1], this system has a unique solution if there exist continuous functions \(z_i(t)>0\) such that

\[ z_i(t)>\sum_{k=0}^{n-1}\int_a^b |G^{(i)}(t,s)p_k(s)|z_k(s)\,ds \]

\[ (i=0,\ 1,\ldots,\ n-1). \]

We shall show that such functions exist for any \(a, b \in [0, R)\). From the condition of the theorem and (4) it follows that the root of the equation

\[ \left| \begin{array}{cccc} H_0\displaystyle\int_0^R |p_0(s)|\,ds-\lambda & \cdots & H_{n-1}\displaystyle\int_0^R |p_{n-1}(s)|\,ds \\ \cdot & \cdot & \cdot \\ H_0\displaystyle\int_0^R |p_0(s)|\,ds & \cdots & H_{n-1}\displaystyle\int_0^R |p_{n-1}(s)|\,ds-\lambda \end{array} \right| = \]

\[ =(-\lambda)^{n-1} \left\{ \lambda-\sum_{k=0}^{n-1} H_k\int_0^R |p_k(s)|\,ds \right\} =0 \]

is less than unity. And this means that, for the system

\[ \xi_i=\sum_{k=0}^{n-1} a_k \xi_k+\eta_i \qquad (i=0,1,\ldots,n-1), \tag{7} \]

where

\[ a_k=H_k\int_0^R |p_k(s)|\,ds, \tag{8} \]

Chaplygin’s theorem is valid, i.e., for \(\eta_i>0\) we have \(\xi_i>0\)\(^*\). Let \(c_i>0\) be a solution of system (7); then

\[ c_i>\sum_{k=0}^{n-1} a_k c_k \qquad (i=0,1,\ldots,n-1). \]

Using (3) and (8), we strengthen the last inequalities:

\[ c_i> \sum_{k=0}^{n-1}\int_a^b |G^{(i)}(t,s)p_k(s)| \frac{c_k K^{(k)}(s,a)}{K^{(i)}(t,a)}\,ds. \]

It follows from this that \(z_k(t)=c_k K^{(k)}(t,a)\) satisfy inequalities (6) for any \(a,b\in[0,R)\).
The theorem is proved.

Remark. It is not difficult to see that \([0,R)\) is a subcritical interval of problem (1), (2) if and only if in the triangle \(0\le s<t<R\) the inequality \(K^{(m)}(t,s)>0\) holds. Thus, the subcritical interval of problem (1), (2) is the interval of applicability of Chaplygin’s theorem for the equation \(L[y]=f(t)\) (see [4, 5]).

We note that the estimate of the interval of applicability of Chaplygin’s theorem [6, 8] is obtained as a special case of our theorem when \(m=r\), \(p_k(t)\equiv 0\) \((k=r+1,r+2,\ldots,n-1)\).

  1. In the case \(p_k(t)\ge 0\) \((k=1,2,\ldots,n-1)\), one may propose the following supplement to the results of [4].

\(^*\) This follows directly from the fact that, under the indicated conditions, the method of successive approximations for system (7) converges.

Theorem 2. If

\[ \sum_{k=0}^{n-1}\frac{(n-m-1)!\,R^{\,n-k}}{(2n-m-k-1)!}\,P_k<1, \]

where

\[ P_k=\max_{[a,b]\in[0,R)}[p_k(t)], \]

then \([0,R)\) is a precritical interval for problem (1), (2).

Proof. From the remark to Theorem 1 it is clear that the question of estimating the precritical interval for problem (1), (2) is equivalent to the question of the conditions for positivity of \(C^{(m)}(t,s)\), where \(C(t,s)\) is the Cauchy function of equation (5). For a lower estimate of \(C^{(m)}(t,s)\), define the sequence \(\{W_i(t,s)\}\) as follows:

\[ W_0(t,s)=\frac{(t-s)^{n-1}}{(n-1)!}, \]

\[ W_{i+1}(t,s)=W_i(t,s)-\int_s^t W_i(t,\tau)L_1[W_i(\tau,s)]\,d\tau . \tag{9} \]

By Theorem 2 of [3], if \(L_1[W_0(\tau,s)]\ge 0\) in the triangle \(0\le s<t<R\), then \(W_i^{(m)}(t,s)\le W_{i+1}^{(m)}(t,s)\le C^{(m)}(t,s)\) in this triangle. Restricting ourselves to the first step of the iterative process (9), we have: if \(W_1^{(m)}(t,s)>0\) in the triangle \(0<s<t<R\), then also \(C^{(m)}(t,s)>0\) in this triangle. The inequality

\[ W_1^{(m)}(t,s)= \frac{(t-s)^{n-m-1}}{(n-m-1)!} - \int_s^t \frac{(t-\tau)^{n-m-1}}{(n-m-1)!} \times \]

\[ \times \left[ \sum_{k=0}^{n-1} p_k(\tau)\frac{(\tau-s)^{n-k-m-1}}{(n-k-m-1)!} \right]\,d\tau>0 \]

will hold if

\[ \sum_{k=0}^{n-1} \frac{(t-s)^{2n-m-k-1}(n-m-1)!}{(2n-m-k-1)!}\,p_k < (t-s)^{n-m-1}. \]

The last inequality is valid if

\[ \sum_{k=0}^{n-1} \frac{(n-m-1)!\,R^{n-k}}{(2n-m-k-1)!}\,p_k<1. \]

The theorem is proved.

3. Consider the equation

\[ y'''+p(t)y'+g(t)y=0. \tag{10} \]

We shall assume that \(p(t)\) has a continuous derivative. Denote

\[ h(t)=\frac{1}{2}\{|g(t)|+g(t)\}. \]

\[ h_1(t)=\frac{1}{2}\{|p'(t)-g(t)|+|p'(t)-g(t)|\}, \]

\[ H=\max_{t\in[0,T]}[h(t)],\qquad H_1=\max_{t\in[0,T]}[h_1(t)]. \]

Taking into account theorem 2 of [2], we obtain the following consequences of theorems 1 and 2.

Corollary 1. If the inequalities

\[ \frac{4T}{27}\int_0^T |p(t)|\,dt+\frac{T^2}{32}\int_0^T h(t)\,dt<1, \]

\[ \frac{4T}{27}\int_0^T |p(t)|\,dt+\frac{T^2}{32}\int_0^T h_1(t)\,dt<1, \]

are satisfied, then \([0,T)\) is an interval of nonoscillation of equation (10).

Corollary 2. Let \(P\geq p(t)\geq 0\) and let the inequalities

\[ \frac{T^2}{12}\,P+\frac{T^3}{60}\,H<1,\qquad \frac{T^2}{12}\,P+\frac{T^3}{60}\,H_1<1, \]

be satisfied; then \([0,T)\) is an interval of nonoscillation of equation (10).

  1. Let us consider some consequences of the above theorems for an equation of the special form

\[ y^{(n)}+g(t)y=0. \tag{11} \]

As is known (see, for example, [7]), when \(g(t)\geq 0\), the subcritical interval of problem (11), (2) for \(m=0\) is an interval of nonoscillation for equation (11). On the basis of what has been said and theorems 1 and 2, we have

Corollary 3. If \(g(t)\geq 0\) on \([0,T)\) and one of the inequalities

\[ \frac{T^{n-1}}{4^{\,n-1}(n-1)!}\int_0^T g(t)\,dt<1 \quad\text{or}\quad g(t)<\frac{(2n-1)!}{(n-1)!\,T^n}, \]

is satisfied, then \([0,T)\) is an interval of nonoscillation of equation (11).

For odd \(n\), the equations

\[ y^{(n)}+g(t)y=0 \quad\text{and}\quad y^{(n)}-g(t)y=0 \]

are adjoint. Since for adjoint equations the intervals of nonoscillation coincide, one may formulate

Corollary 4. If \(g(t)\leq 0\) on \([0,T)\) and one of the inequalities

\[ \frac{T^{n-1}}{4^{\,n-1}(n-1)!}\int_0^T |g(t)|\,dt<1 \quad\text{or}\quad |g(t)|<\frac{(2n-1)!}{(n-1)!\,T^n}, \]

is satisfied, then \([0,T)\) is an interval of nonoscillation of equation (11) for odd \(n\).

References

  1. N. V. Azbelev, Z. B. Tsalyuk. Dokl. Akad. Nauk SSSR, 156, No. 2, 239—242, 1964.
  2. N. V. Azbelev, Z. B. Tsalyuk. Matem. sb., 51, No. 4, 1960, pp. 475—486.
  3. N. V. Azbelev, I. M. Smolin, Z. B. Tsalyuk. Dokl. Akad. Nauk SSSR, 135, No. 3, 511—514, 1960.
  4. Yu. V. Komlenko. Dokl. Akad. Nauk SSSR, 164, No. 2, 270—272, 1965.
  5. N. V. Azbelev, Z. B. Tsalyuk. Ukrainian Mathematical Journal, 10, No. 1, 3—12, 1958.
  6. N. V. Azbelev, Z. B. Tsalyuk. Differential Equations, 1, No. 4, 1965.
  7. J. Mikusinski. Ann. polon. math., 1, No. 2, 1955.
  8. Yu. V. Komlenko. Reports of the Third Siberian Conference on Mathematics and Mechanics. Tomsk, 1964, pp. 119—120.

Received by the editors
April 30, 1965

Izhevsk Mechanical
Institute

Submission history

ON THE QUESTION OF ESTIMATING THE INTERVAL OF APPLICABILITY OF CHAPLYGIN’S THEOREM