On the localization and numerical computation of positive radial solutions for φ-Laplace equations in the annulus

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Abstract

The paper deals with the existence and localization of positive radial solutions for stationary partial differential equations involving a general ϕ-Laplace operator in the annulus. Three sets of boundary conditions are considered: Dirichlet–Neumann, Neumann–Dirichlet and Dirichlet–Dirichlet. The results are based on the homotopy version of Krasnosel’skiıs fixed point theorem and Harnack type inequalities, first established for each one of the boundary conditions. As a consequence, the problem of multiple solutions is solved in a natural way. Numerical experiments confirming the theory, one for each of the three sets of boundary conditions, are performed by using the MATLAB object-oriented package Chebfun.

Authors

Jorge Rodríguez-López
CITMAga & Departamento de Estatística, Análise Matemática e Optimización, Universidade de
Santiago de Compostela, 15782, Facultade de Matemáticas, Campus Vida, Santiago, Spain

Radu Precup

Radu Precup

Faculty of Mathematics and Computer Science and Institute of Advanced Studies in Science and Technology, Babes-Bolyai University, Cluj-Napoca, Romania
Călin-Ioan Gheorghiu

Călin-Ioan Gheorghiu

Keywords

ϕ-Laplace operator; radial solution; positive solution; fixed point index; Harnack type inequality; numerical solution.

Paper coordinates

J. Rodriguez-Lopez, R. Precup, C.-I. Gheorghiu, On the localization and numerical computation of positive radial solutions for φ-Laplace equations in the annulus, Electronic Journal of Qualitative Theory of Differential Equations, 2022, no. 47, pp. 1-22, doi.org/10.14232/ejqtde.2022.1.47

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http://www.math.u-szeged.hu/ejqtde/p9859.pdf

About this paper

Journal

Electronic Journal of Qualitative Theory of Differential Equations

Publisher Name

University of Szeged

DOI

http://doi.org/10.14232/ejqtde.2022.1.47

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ISSN 14173875

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On the localization and numerical computation of positive radial solutions for ϕ-Laplace equations in the annulus

On the localization and numerical computation of positive radial solutions for $\phi$ -Laplace equations in the annulus

Jorge Rodríguez-López J. Rodríguez-López, Departamento de Estatística, Análise Matemática e Optimización, Instituto de Matemáticas, Universidade de Santiago de Compostela, 15782, Facultade de Matemáticas, Campus Vida, Santiago, Spain jorgerodriguez.lopez@usc.es , Radu Precup R. Precup, Faculty of Mathematics and Computer Science and Institute of Advanced Studies in Science and Technology, Babeş-Bolyai University, 400084 Cluj-Napoca, Romania & Tiberiu Popoviciu Institute of Numerical Analysis, Romanian Academy, P.O. Box 68-1, 400110 Cluj-Napoca, Romania r.precup@math.ubbcluj.ro and Călin-Ioan Gheorghiu C.-I. Gheorghiu, Tiberiu Popoviciu Institute of Numerical Analysis, Romanian Academy, P.O. Box 68-1, 400110 Cluj-Napoca, Romania ghcalin@ictp.acad.ro

Abstract.

The paper deals with the existence and localization of positive radial solutions for stationary partial differential equations involving a general $\phi$ -Laplace operator in the annulus. Three sets of boundary conditions are considered: Dirichlet-Neumann, Neumann-Dirichlet and Dirichlet-Dirichlet. The results are based on the homotopy version of Krasnosel’skiĭ’s fixed point theorem and Harnack type inequalities, first established for each one of the boundary conditions. As a consequence, the problem of multiple solutions is solved in a natural way. Numerical experiments confirming the theory, one for each of the three sets of boundary conditions, are performed by using the MATLAB object-oriented package Chebfun.

Key words and phrases:

\phi

-Laplace operator, radial solution, positive solution, fixed point index, Harnack type inequality, numerical solution

1991 Mathematics Subject Classification:

35J60, 34B18

1. Introduction

In the short but clever paper [19], Hayan Wang solved the problem of existence of positive radial solutions for the semilinear elliptic equation

\Delta w+g\left(\left|x\right|\right)f\left(w\right)=0,\ \ \ \ \ \ R_{1}<\left% |x\right|<R_{2},\ \ x\in\mathbb{R}^{N},\ \ N\geq 2,

with one of the following sets of boundary conditions,

(1.2)		$\displaystyle\begin{array}[]{ccc}w=0\ \ \text{on\ \ }\left\|x\right\|=R_{1}&% \text{and}&\left\|x\right\|=R_{2},\end{array}$
(1.4)		$\displaystyle\begin{array}[]{ccc}w=0\ \ \text{on\ \ }\left\|x\right\|=R_{1}&% \text{and}&\partial w/\partial r=0\ \ \text{on\ \ }\left\|x\right\|=R_{2},\end{array}$
(1.6)		$\displaystyle\begin{array}[]{ccc}\partial w/\partial r=0\ \ \text{on\ \ }\left% \|x\right\|=R_{1}&\text{and}&w=0\ \ \text{on\ \ }\left\|x\right\|=R_{2},\end{array}$

where $r=\left|x\right|$ and $\partial w/\partial r$ denotes differentiation in the radial direction, and $0<R_{1}<R_{2}<+\infty.$

The tools were a Krasnosel’skiĭ type fixed point theorem in cones and the property of bilateral boundedness of the corresponding Green functions. The first one is based on the fixed point index theory, while the second, as shown in [13], on Harnack type inequalities. Since then, many authors have considered the problem of radial solutions for equations and systems involving the Laplacian or some of its generalizations, various boundary conditions and domains, by using different topological or variational methods. We refer the interested reader to some of these contributions [1, 2, 3, 6, 5, 8] and the references therein.

Most of the works that followed deviated from the spirit of the original ideas. On their line, we mention our recent papers [14], [15] and [16]. It is the scope of the present paper to complement them, as close as possible to paper [19], for the case of equations with a general $\phi$ -Laplacian. Here in the absence of a Green function we are forced to produce Harnack type inequalities for each set of boundary conditions.

More exactly, in this paper, we deal with the existence, localization and multiplicity of positive radial solutions to the Dirichlet problem involving $\phi$ -Laplacian operators:

(1.7)

-\mathrm{div}\left(\psi\left(\left|\nabla w\right|\right)\nabla w\right)=g% \left(\left|x\right|\right)f\left(u\right)\quad\text{ }R_{1}<\left|x\right|<R_% {2},\ \ x\in\mathbb{R}^{N},\ \ N\geq 2,

where $0<R_{1}<R_{2}<+\infty,$ the functions $g:\left[R_{1},R_{2}\right]\rightarrow\mathbb{R}_{+},\ f:\mathbb{R}_{+}% \rightarrow\mathbb{R}_{+}$ are continuous and $\psi:\left(-a,a\right)\rightarrow\mathbb{R}$ is such that $\phi\left(s\right):=s\,\psi\left(s\right)$ is an increasing homeomorphism between two intervals $\left(-a,a\right)$ and $\left(-b,b\right)$ $(0<a,b\leq+\infty).$

The following particular cases are of much interest due to their corresponding models arising from physics:

(a) $\phi:\mathbb{R}\rightarrow\mathbb{R},\ \ \phi\left(s\right)=\left|s\right|^{p-% 2}s,$ where $p>1\$ (here $a=b=+\infty$ ), when the left side $L_{0}w$ in (1.7) is

L_{0}w=-\mathrm{div}\left(\left|\nabla w\right|^{p-2}\nabla w\right)\ \ \ % \text{(}p\text{-{Laplace operator}),}

involved in a nonlinear Darcy law for flows through porous media;

(b) (singular homeomorphism) $\phi:\left(-a,a\right)\rightarrow\mathbb{R},\ \phi\left(s\right)=\frac{s}{% \sqrt{a^{2}-s^{2}}}$ (here $0<a<+\infty$ and $b=+\infty$ ), when

L_{0}w=-\mathrm{div}\left(\frac{\nabla w}{\sqrt{a^{2}-\left|\nabla w\right|^{2% }}}\right)\ \ \ \text{({Minkowski mean curvature operator}),}

arised from the relativistic mechanics;

(c) (bounded homeomorphism) $\phi:\mathbb{R}\rightarrow\left(-b,b\right),\ \phi\left(s\right)=\frac{bs}{% \sqrt{1+s^{2}}}$ (here $a=+\infty$ and $0<b<+\infty$ ), when

L_{0}w=-b\,\mathrm{div}\left(\frac{\nabla w}{\sqrt{1+\left|\nabla w\right|^{2}% }}\right)\ \ \ \text{({Euclidian mean curvature operator}),}

associated to capillarity problems.

Looking for radial solutions of (1.7), that is, functions of the form $w(x)=v(r)$ with $r=\left|x\right|$ , (1.7) reduces to the ordinary differential equation

(1.8)

L\left(v\right):=-r^{1-N}\left(r^{N-1}\phi\left(v^{\prime}\right)\right)^{% \prime}=g\left(r\right)f(v),\qquad R_{1}<r<R_{2},

while boundary conditions (1.2) become

(1.10)		$\displaystyle\begin{array}[]{ccc}v\left(R_{1}\right)=0&\text{and}&v\left(R_{2}% \right)=0,\end{array}$
(1.12)		$\displaystyle\begin{array}[]{ccc}v\left(R_{1}\right)=0&\text{and}&v^{\prime}% \left(R_{2}\right)=0,\end{array}$
(1.14)		$\displaystyle\begin{array}[]{ccc}v^{\prime}\left(R_{1}\right)=0&\text{and}&v% \left(R_{2}\right)=0.\end{array}$

2. Harnack type inequalities

Originally, Harnack’s inequality was introduced in order to give estimates from above and from below for the ratio $u(x)/u(y)$ of two values of a positive harmonic function. It can be generically put under the form

\min_{x\in\omega}u\left(x\right)\geq k\max_{x\in\omega}u\left(x\right),

where $k$ is a positive constant depending on the subdomain $\omega.$ Next it was generalized to nonnegative solutions or supersolutions of a wide class of linear elliptic equations. For the origin of the notion and many references, we refer the reader to [11].

More general, we speak about a Harnack type inequality whenever for a given operator $L$ acting on a space of functions defined on a set $\Omega$ and endowed with a norm $\left\|\cdot\right\|,$ there is a subdomain $\omega\subset\Omega$ and a constant $k>0$ such that

\min_{x\in\omega}u\left(x\right)\geq k\left\|u\right\|

for all nonnegative functions $u$ satisfying $L\left(u\right)\geq 0$ and eventually some additional behavior properties. In [12], Harnack inequalities have been put in connexion with the compression-expansion method of Krasnosel’skiĭ for the localization of positive solutions of nonlinear problems. In case of boundary value problems for ordinary differential equations, when a Green function is known, a Harnack inequality immediately can be derived using the bilateral estimates of the Green function. However, Harnack inequalities can be obtained even for differential operators for which a Green function does not exist. This is the case of the $\phi$ -Laplace operators. Deduction of such inequalities requires a fine analysis and makes use of priority properties of solutions such as monotony and concavity (see, e.g., [9] and [10]). The analysis is even more difficult in the case of radial solutions. It is the goal of this section to obtain Harnack inequalities for $\phi$ -Laplace operators subject to each of the three boundary conditions (1.10), (1.12), (1.14).

2.1. Case of the boundary conditions (1.12)

Theorem 2.1.

If $v\in C^{1}\left[R_{1},R_{2}\right]$ is such that (1.12) are satisfied, $r^{N-1}\phi\left(v^{\prime}\right)$ is differentiable and $L\left(v\right)\left(r\right)\in[0,b\,(R_{1}/R_{2})^{N-1})$ for all $r\in\left[R_{1},R_{2}\right],$ then $v$ is nonnegative, increasing and concave. In addition, for any $c\in\left(R_{1},R_{2}\right),$ one has

(2.1)

v\left(c\right)\geq\frac{c-R_{1}}{R_{2}-R_{1}}v\left(R_{2}\right).

Proof.

Let $h:=L\left(v\right).$ Integrating from $r$ to $R_{2}$ and taking into account that $v^{\prime}\left(R_{2}\right)=0$ yields

v^{\prime}\left(r\right)=\phi^{-1}\left(r^{1-N}\int_{r}^{R_{2}}\tau^{N-1}h% \left(\tau\right)d\tau\right).

A new integration, this time from $R_{1}$ to $r$ gives the expression of the solution, namely

v\left(r\right)=\int_{R_{1}}^{r}\phi^{-1}\left(s^{1-N}\int_{s}^{R_{2}}\tau^{N-% 1}h\left(\tau\right)d\tau\right)ds

and of the associated solution operator

S\left(h\right)\left(r\right)=\int_{R_{1}}^{r}\phi^{-1}\left(s^{1-N}\int_{s}^{% R_{2}}\tau^{N-1}h\left(\tau\right)d\tau\right)ds.

Since $h\geq 0,$ these formulas show that $v$ is nonnegative and increasing. Also $v^{\prime}$ is decreasing, i.e., $v$ is concave. Finally, the concavity implies that the graph of $v$ is over the line joining the point $\left(R_{1},0\right)$ and $\left(R_{2},v\left(R_{2}\right)\right),$ whose equation is $y=\frac{v\left(R_{2}\right)}{R_{2}-R_{1}}\left(x-R_{1}\right).$ Taking $x=c$ gives (2.1). ∎

Note that under the assumptions of Theorem 2.1, in (2.1), one has $v\left(c\right)=\min_{r\in\left[c,R_{2}\right]}v\left(r\right)$ and $v\left(R_{2}\right)=\max_{r\in\left[R_{1},R_{2}\right]}v\left(r\right)=\left\|% v\right\|.$ Hence,

\min_{r\in\left[c,R_{2}\right]}v\left(r\right)\geq k_{1}\left\|v\right\|,

with $k_{1}=(c-R_{1})/(R_{2}-R_{1})$ .

2.2. Case of the boundary conditions (1.14)

Theorem 2.2.

If $v\in C^{1}\left[R_{1},R_{2}\right]$ is such that (1.14) are satisfied, $r^{N-1}\phi\left(v^{\prime}\right)$ is differentiable, $L\left(v\right)\left(r\right)\in[0,b)$ and $L\left(v\right)$ is increasing on $\left[R_{1},R_{2}\right],$ then $v$ is nonnegative, decreasing and concave. In addition, for any $c\in\left(R_{1},R_{2}\right),$ one has

(2.2)

v\left(c\right)\geq\frac{R_{2}-c}{R_{2}-R_{1}}v\left(R_{1}\right).

Proof.

If we let $h=L\left(v\right),$ then by integration we obtain

v^{\prime}\left(r\right)=\phi^{-1}\left(-r^{1-N}\int_{R_{1}}^{r}\tau^{N-1}h% \left(\tau\right)d\tau\right)

and

S\left(h\right)\left(r\right)=v\left(r\right)=-\int_{r}^{R_{2}}\phi^{-1}\left(% -s^{1-N}\int_{R_{1}}^{s}\tau^{N-1}h\left(\tau\right)d\tau\right)ds.

Since $h$ is nonnegative, these formulas immediately imply that $v$ is nonnegative and decreasing.

To show that $v$ is concave we need to prove that $v^{\prime}$ is decreasing, equivalently, that the function $\eta\left(r\right)=r^{1-N}\int_{R_{1}}^{r}\tau^{N-1}h\left(\tau\right)d\tau$ is increasing. Indeed, using the monotonicity of $h,$ one has

$\displaystyle\eta^{\prime}\left(r\right)$	$\displaystyle=$	$\displaystyle h\left(r\right)-\frac{N-1}{r^{N}}\int_{R_{1}}^{r}\tau^{N-1}h% \left(\tau\right)d\tau$
	$\displaystyle\geq$	$\displaystyle h\left(r\right)-\frac{N-1}{r^{N}}h\left(r\right)\int_{R_{1}}^{r}% \tau^{N-1}d\tau$
	$\displaystyle=$	$\displaystyle h\left(r\right)-\frac{N-1}{N}h\left(r\right)\left(1-\left(\frac{% R_{1}}{r}\right)^{N}\right)$
	$\displaystyle\geq$	$\displaystyle 0.$

Finally, since the graph of the concave function $v$ is over the line joining the points $\left(R_{1},v\left(R_{1}\right)\right)$ and $\left(R_{2},0\right),$ if $c$ is any point in $\left(R_{1},R_{2}\right),$ we have (2.2). ∎

Note that under the assumptions of Theorem 2.2, in (2.2), one has $v\left(c\right)=\min_{r\in\left[R_{1},c\right]}v\left(r\right)$ and $v\left(R_{1}\right)=\max_{r\in\left[R_{1},R_{2}\right]}v\left(r\right)=\left\|% v\right\|.$ Therefore,

\min_{r\in\left[R_{1},c\right]}v\left(r\right)\geq k_{2}\left\|v\right\|,

where $k_{2}=(R_{2}-c)/(R_{2}-R_{1})$ .

2.3. Case of the boundary conditions (1.10)

Theorem 2.3.

For each function $h\in L^{1}\left(R_{1},R_{2}\right)$ not identically zero satisfying $h\left(r\right)\geq 0$ a.e. on $\ \left(R_{1},R_{2}\right)$ and $\left\|h\right\|_{L^{1}}<b\,(R_{1}/R_{2})^{N-1}$ , the equation $L\left(v\right)=h$ endowed with the boundary conditions (1.10) has a unique nonzero nonnegative solution $v$ which is concave and such that for any $c\in[0,\left(R_{2}-R_{1}\right)/2),$ one has:

(2.3)

{\min_{r\in\left[c_{1},c_{2}\right]}}v\left(r\right){\geq{\frac{1}{R_{2}-R_{1}% }\left(\frac{R_{2}-R_{1}}{2}-c\right)}\left\|v\right\|},

where $\ c_{1}=R_{m}-c,$ $c_{2}=R_{m}+c$ and $R_{m}=\left(R_{1}+R_{2}\right)/2.$

Proof.

Let $v$ be a nonnegative solution. Since $h$ is not identically zero, $v$ is nonzero and since it vanishes at $R_{1}$ and $R_{2},$ any maximum point $R$ is interior and so $v^{\prime}\left(R\right)=0.$ Integrating from $R$ to $r$ then gives

(2.4)

v^{\prime}\left(r\right)=\phi^{-1}\left(-r^{1-N}\int_{R}^{r}\tau^{N-1}h\left(% \tau\right)d\tau\right).

This shows that $v^{\prime}$ is decreasing on $\left[R_{1},R_{2}\right].$ Hence $v$ is concave on $\left[R_{1},R_{2}\right].$ Let $R$ be such that $v\left(R\right)=\left\|v\right\|=\max_{r\in\left[R_{1},R_{2}\right]}v\left(r% \right).\$ First assume that $R\leq R_{m}.$ The concavity of $v$ implies that the graph of $v$ restricted to $\left[R,R_{2}\right]$ is over the line joining the points $\left(R,v\left(R\right)\right)$ and $\left(R_{2},0\right)$ which at its turn is over the line joining the points $\left(R_{1},v\left(R\right)\right),\ \left(R_{2},0\right),$ of equation $y=\frac{v\left(R\right)}{R_{2}-R_{1}}\left(R_{2}-x\right).$ Thus, since $c_{2}\in\left[R,R_{2}\right],$ we have

v\left(c_{2}\right)\geq\frac{v\left(R\right)}{R_{2}-R_{1}}\left(R_{2}-c_{2}% \right){=\frac{1}{R_{2}-R_{1}}\left(\frac{R_{2}-R_{1}}{2}-c\right)v\left(R% \right)}.

In addition the graph of $v$ on $\left[R_{1},R_{m}\right]$ is over the line joining the points $\left(R_{1},0\right),\ \left(R_{2},v\left(R\right)\right).$ Then

v\left(c_{1}\right)\geq\frac{v\left(R\right)}{R_{2}-R_{1}}\left(c_{1}-R_{1}% \right)=\frac{1}{R_{2}-R_{1}}\left(\frac{R_{2}-R_{1}}{2}-c\right)v\left(R% \right).

As a result

\min_{r\in\left[c_{1},c_{2}\right]}v\left(r\right)=\min\left\{v\left(c_{1}% \right),v\left(c_{2}\right)\right\}\geq{\frac{1}{R_{2}-R_{1}}\left(\frac{R_{2}% -R_{1}}{2}-c\right)}\left\|v\right\|.

The proof of the case $R\geq R_{m}$ is similar.

Next, integration in (2.4) gives the representation formulas (for the solution operator)

(2.5)

v\left(r\right)=\int_{R_{1}}^{r}\phi^{-1}\left(-s^{1-N}\int_{R}^{s}\tau^{N-1}h% \left(\tau\right)d\tau\right)ds\ \ \ \left(r\in\left[R_{1},R_{2}\right]\right),

v\left(r\right)=-\int_{r}^{R_{2}}\phi^{-1}\left(-s^{1-N}\int_{R}^{s}\tau^{N-1}% h\left(\tau\right)d\tau\right)ds\ \ \ \left(r\in\left[R_{1},R_{2}\right]\right).

To prove the existence of a solution, in virtue of (2.5) and (2.4) it is enough to prove the existence of a number $R\in\left(R_{1},R_{2}\right)$ such that

\int_{R_{1}}^{R_{2}}\phi^{-1}\left(-s^{1-N}\int_{R}^{s}\tau^{N-1}h\left(\tau% \right)d\tau\right)ds=0.

This immediately follows since the continuous function

t\longmapsto\int_{R_{1}}^{R_{2}}\phi^{-1}\left(-s^{1-N}\int_{t}^{s}\tau^{N-1}h% \left(\tau\right)d\tau\right)ds\ \ \ \left(t\in\left[R_{1},R_{2}\right]\right)

takes values of opposite sign at the ends $R_{1}$ and $R_{2}.$

To prove the uniqueness of the solution, assume that $v_{1}$ and $v_{2}$ are two nonnegative solutions and let $R^{\prime},R^{\prime\prime}$ be two of their maximum points, respectively. Using the representation formula (2.4) it is easy to see that $\left(v_{2}-v_{1}\right)^{\prime}$ preserves its sign on the whole interval $\left(R_{1},R_{2}\right),$ positive or negative depending on the ordering between $R^{\prime}$ and $R^{\prime\prime}.$ Thus $v_{2}-v_{1}$ is monotone and being zero at the ends of the interval it must be identically zero. Hence $v_{1}=v_{2}.$ ∎

3. Existence and localization

As mentioned above, the key ingredient together with Harnack inequalities to obtain positive solutions in this paper will be the fixed point index in cones. In particular, we recall the well–known homotopy version of Krasnosel’skiĭ fixed point theorem in cones.

Theorem 3.1 (Krasnosel’skiĭ).

Let $\ X$ be a Banach space, $K$ a cone of $X$ and $\Omega_{1}$ and $\Omega_{2}$ two relatively open and bounded subsets of $K$ with $0\in\Omega_{1}\subset\overline{\Omega}_{1}\subset\Omega_{2}$ . Let $N:K\rightarrow K$ be a completely continuous operator satisfying one of the following two conditions:

(i):: $\lambda u\neq N(u)$ for all $u\in\partial_{K}\Omega_{1}$ and all $\lambda\geq 1$ ; and there exists $h\in K\setminus\{0\}$ such that $u\neq N(u)+\lambda\,h$ for all $u\in\partial_{K}\Omega_{2}$ and all $\lambda\geq 0$ .
(ii):: $\lambda u\neq N(u)$ for all $u\in\partial_{K}\Omega_{2}$ and all $\lambda\geq 1$ ; and there exists $h\in K\setminus\{0\}$ such that $u\neq N(u)+\lambda\,h$ for all $u\in\partial_{K}\Omega_{1}$ and all $\lambda\geq 0$ .

Then $N$ has a fixed point $u\in K$ such that $u\in\Omega_{2}\setminus\overline{\Omega}_{1}$ .

In the sequel, consider the Banach space of continuous functions $C[R_{1},R_{2}]$ endowed with the usual maximum norm $\left\|v\right\|=\max_{r\in\left[R_{1},R_{2}\right]}\left|v\left(r\right)\right|$ and denote by $P$ the cone of nonnegative functions in $C[R_{1},R_{2}]$ .

3.1. Case of the boundary conditions (1.12)

By a solution of (1.8)–(1.12) we mean a function $v\in C^{1}[R_{1},R_{2}]$ with $v(R_{1})=0=v^{\prime}(R_{2})$ such that $v^{\prime}\in(-a,a)$ , $r^{n-1}\phi(v^{\prime})\in W^{1,1}[R_{1},R_{2}]$ and satisfies (1.8). We will look for nonnegative nontrivial solutions on $[R_{1},R_{2}]$ .

It is clear that $v$ is a nonnegative solution of (1.8)–(1.12) if and only if $v$ is a fixed point of the operator

T_{1}(v)(r)=\int_{R_{1}}^{r}\phi^{-1}\left(s^{1-N}\int_{s}^{R_{2}}\tau^{N-1}g% \left(\tau\right)f(v(\tau))d\tau\right)ds.

If $f$ is such that $f\left(s\right)\int_{R_{1}}^{R_{2}}g\left(\tau\right)d\tau<\left(\frac{R_{1}}{% R_{2}}\right)^{N-1}b$ for all $s\in\mathbb{R}_{+},$ then $T_{1}$ is defined on the whole cone $P$ and $T_{1}\left(P\right)\subset P.$ Moreover, $T_{1}$ is completely continuous as follows from the Arzelà–Ascoli theorem.

Here, for a fixed $c\in(R_{1},R_{2})$ , we will look for fixed points of the operator $T_{1}$ in a subcone of $P$ , namely,

K_{1}=\left\{v\in P:\min_{r\in\left[c,R_{2}\right]}v\left(r\right)\geq k_{1}% \left\|v\right\|\right\},

where $k_{1}=(c-R_{1})/(R_{2}-R_{1})$ . By the Harnack inequality given by Theorem 2.1, it is easy to check that the operator $T_{1}$ maps the cone $K_{1}$ into itself.

Now, for any numbers $\alpha,\beta>0$ , consider the open (in $K_{1}$ ) sets

(3.1)

V_{\alpha}:=\left\{v\in K_{1}:\left\|v\right\|<\alpha\right\}

and

(3.2)

W_{\beta}:=\left\{v\in K_{1}:\min_{r\in\left[c,R_{2}\right]}v\left(r\right)<% \beta\right\}.

Note that $V_{\beta}\subset W_{\beta}\subset V_{\beta/k_{1}}$ , so $W_{\beta}$ is bounded.

We are in the position to apply Theorem 3.1 in order to obtain existence and localization results for problem (1.8)–(1.12). In this way, we localize a solution in the set $W_{\beta}\setminus\overline{V}_{\alpha}$ if $\beta>\alpha$ and in the set $V_{\alpha}\setminus\overline{W}_{\beta}$ if $\alpha>\beta/k_{1}.$

We will use the following notations:

A:=\int_{R_{1}}^{R_{2}}g(\tau)d\tau\quad\text{and}\quad B:=\int_{c}^{R_{2}}g(% \tau)d\tau.

Also, for any $\alpha,\beta>0$ , we denote

M_{\alpha}:=\max\{f(s):s\in[0,\alpha]\}\quad\text{and}\quad m_{\beta}:=\min\{f% (s):s\in[\beta,\beta/k_{1}]\}.

Theorem 3.2.

Assume that

(3.3)

f\left(s\right)<\frac{b}{A}\left(\frac{R_{1}}{R_{2}}\right)^{N-1}\ \ \ \text{% for all }s\in\mathbb{R}_{+}.

In addition assume that there exist $\alpha,\beta>0$ such that

(3.4)		$\displaystyle(R_{2}-R_{1})\phi^{-1}\left((R_{2}/R_{1})^{N-1}A\,M_{\alpha}\right)$	$\displaystyle<\alpha,$
(3.5)		$\displaystyle(c-R_{1})\phi^{-1}\left(B\,m_{\beta}\right)$	$\displaystyle>\beta.$

(1⁰):: If $\alpha<\beta$ , then problem (1.8)–(1.12) has a positive solution $v$ such that $\alpha<\left\|v\right\|<\beta/k_{1}$ .
(2⁰):: If $\alpha>\beta/k_{1}$ , then problem (1.8)–(1.12) has a positive solution $v$ such that $\beta<\left\|v\right\|<\alpha$ .

Proof.

We shall apply Theorem 3.1. First, let us see that

\left\|T_{1}(v)\right\|<\alpha\quad\text{for all }v\in K_{1}\text{ with }\left\|v\right\|=\alpha,

which clearly implies that $\lambda v\neq T_{1}(v)$ for all $v\in\partial_{K_{1}}V_{\alpha}$ and all $\lambda\geq 1$ . Indeed, for $v\in K_{1}$ with $\left\|v\right\|=\alpha$ , we have that $f(v(s))\leq M_{\alpha}$ and so from (3.4) it follows that

	$\displaystyle\left\\|T_{1}(v)\right\\|$	$\displaystyle=\int_{R_{1}}^{R_{2}}\phi^{-1}\left(s^{1-N}\int_{s}^{R_{2}}\tau^{% N-1}g\left(\tau\right)f(v(\tau))d\tau\right)ds$
		$\displaystyle\leq\int_{R_{1}}^{R_{2}}\phi^{-1}\left(M_{\alpha}\,s^{1-N}\int_{R% _{1}}^{R_{2}}\tau^{N-1}g\left(\tau\right)d\tau\right)ds$
		$\displaystyle\leq(R_{2}-R_{1})\phi^{-1}\left(\left(R_{2}/R_{1}\right)^{N-1}AM_% {\alpha}\right)<\alpha,$

as wished.

On the other hand, let us prove that $v\neq T_{1}(v)+\lambda h$ for all $v\in\partial_{K_{1}}W_{\beta}$ and all $\lambda\geq 0$ with $h\equiv 1$ . Notice that for $v\in K_{1}$ with $\min_{r\in[c,R_{2}]}v(r)=\beta$ , we have that $\beta\leq v(r)\leq\beta/k_{1}$ for all $r\in[c,R_{2}]$ , and thus $m_{\beta}\leq f(v(r))$ for all $r\in[c,R_{2}]$ . Hence, for any $r\in[c,R_{2}]$ ,

	$\displaystyle T_{1}(v)(r)$	$\displaystyle\geq\int_{R_{1}}^{c}\phi^{-1}\left(s^{1-N}\int_{s}^{R_{2}}\tau^{N% -1}g\left(\tau\right)f(v(\tau))d\tau\right)ds$
		$\displaystyle\geq\int_{R_{1}}^{c}\phi^{-1}\left(s^{1-N}\int_{c}^{R_{2}}\tau^{N% -1}g\left(\tau\right)f(v(\tau))d\tau\right)ds$
		$\displaystyle\geq(c-R_{1})\phi^{-1}\left(B\,m_{\beta}\right).$

Now, (3.5) implies that $T_{1}(v)(r)>\beta=\min_{r\in[c,R_{2}]}v(r)$ for all $r\in[c,R_{2}]$ , which clearly ensures that $v\neq T_{1}(v)+\lambda$ for all $v\in\partial_{K_{1}}W_{\beta}$ and all $\lambda\geq 0$ .

Now, if $\alpha<\beta$ , then $\overline{V}_{\alpha}\subset W_{\beta}$ , so Theorem 3.1 guarantees that the operator $T_{1}$ has at least a fixed point in $W_{\beta}\setminus\overline{V}_{\alpha}\subset V_{\beta/k_{1}}\setminus% \overline{V}_{\alpha}$ . But if one has $\alpha>\beta/k_{1}$ , then $W_{\beta}\subset V_{\beta/k_{1}}\subset\overline{V}_{\beta/k_{1}}\subset V_{\alpha}$ and thus Theorem 3.1 implies that the operator $T_{1}$ has at least a fixed point located in $V_{\alpha}\setminus\overline{W}_{\beta}\subset V_{\alpha}\setminus\overline{V}% _{\beta}.$ ∎

Note that condition (3.3) trivially holds if $b=+\infty.$ Obviously, if $\phi$ is a classical or a bounded homeomorphism, i.e., if $a=+\infty,$ then conditions (3.4) and (3.5) can be rewritten as

\frac{M_{\alpha}}{\phi\left(C_{1}\,\alpha\right)}<C_{2}\quad\text{and}\quad% \frac{m_{\beta}}{\phi\left(C_{3}\,\beta\right)}>C_{4},

with suitable positive constants $C_{1}$ , $C_{2}$ , $C_{3}$ and $C_{4}$ as come from (3.4)-(3.5).

Hence, if we are only interested on the existence and not on the localization of the solutions, we can establish sufficient conditions for the existence of the numbers $\alpha$ and $\beta$ satisfying the inequalities above. They are given by asymptotic conditions on the ratio $f/\phi$ at $0$ and at infinity.

Theorem 3.3.

Assume that the following conditions are satisfied: $\ a=+\infty,$

(3.6)

\limsup_{x\rightarrow 0}\frac{\phi(\tau x)}{\phi(x)}<+\infty,\quad\quad\limsup% _{x\rightarrow+\infty}\frac{\phi(x)}{\phi(\tau x)}<+\infty\quad\text{for all }% \tau>0

and

f_{0}:=\lim_{x\rightarrow 0^{+}}\frac{f(x)}{\phi(x)}=+\infty,\qquad f_{\infty}% :=\lim_{x\rightarrow+\infty}\frac{f(x)}{\phi(x)}=0.

Then problem (1.8)–(1.12) has at least one positive solution.

Proof.

First we show that there exists $\beta>0$ such that

(3.7)

m_{\beta}>C_{4}\phi\left(C_{3}\,\beta\right).

By (3.6), with $\tau=C_{3}$ , there exist $L>0$ and $\rho>0$ such that

\frac{L}{C_{4}}\phi(x)>\phi(C_{3}\,x)\quad\text{for all }x\in(0,\rho).

Now, since $f_{0}=+\infty$ , there exists $\tau>0$ (we may assume $\tau<\rho$ ) such that

f(x)\geq L\phi(x)\quad\text{for all }x\in(0,\tau].

Hence, the fact that $\phi$ is increasing implies that

\min_{x\in[\tau k_{1},\tau]}f(x)\geq L\phi(\tau k_{1}).

Then, taking $\beta=\tau k_{1}$ , one has

m_{\beta}:=\min_{x\in[\beta,\beta/k_{1}]}f(x)\geq L\phi(\beta)>C_{4}\phi(C_{3}% \,\beta),

and so (3.7) holds.

Secondly, we prove that there exists $\alpha>\beta/k_{1}$ such that

(3.8)

M_{\alpha}<C_{2}\phi\left(C_{1}\,\alpha\right).

By (3.6), with $\tau=C_{1}$ , there exist $\tilde{L}>0$ and $\tilde{\rho}>0$ such that

C_{2}\,\tilde{L}\,\phi(C_{1}\,x)>\phi(x)\quad\text{for all }x\in(\tilde{\rho},% +\infty).

Since $f_{\infty}=0$ , there exists $\sigma>0$ such that

f(x)\leq\sigma+\frac{1}{2\tilde{L}}\phi(x)\quad\text{for all }x\geq 0.

Now, it follows from the fact that $\phi:\mathbb{R}\rightarrow\mathbb{R}$ is an increasing unbounded homeomorphism that there exists $\alpha>0$ such that $2\tilde{L}\,\sigma\leq\phi(\alpha)$ . Thus,

f(x)\leq\frac{1}{\tilde{L}}\phi(\alpha)\quad\text{for all }x\in[0,\alpha],

and so

M_{\alpha}:=\max_{x\in[0,\alpha]}f(x)\leq\frac{1}{\tilde{L}}\phi(\alpha)<C_{2}% \phi(C_{1}\,\alpha),

that is, (3.8) holds.

Finally, the conclusion follows from Theorem 3.2. ∎

Similarly, an existence result can be obtained if $f$ is sublinear at $0$ and superlinear at infinity with respect to $\phi$ .

Theorem 3.4.

Assume that $\phi$ is a classical homeomorphism such that

(3.9)

\limsup_{x\rightarrow 0}\frac{\phi(x)}{\phi(\tau x)}<+\infty,\quad\limsup_{x% \rightarrow+\infty}\frac{\phi(\tau x)}{\phi(x)}<+\infty\quad\text{for all }% \tau>0

and $f$ satisfies

f_{0}=0,\qquad f_{\infty}=+\infty.

Then problem (1.8)–(1.12) has at least one positive solution.

Remark 3.5.

Note that if $\phi$ is bounded, then condition $f_{\infty}=+\infty$ is not possible, since $\displaystyle\lim_{x\rightarrow+\infty}\phi(x)=b$ and $f$ must be bounded.

Note that if $\phi$ is singular (i.e., $a<+\infty$ , $b=+\infty$ ), then condition (3.4) is trivially satisfied for $\alpha$ large enough and so the existence of a positive solution for problem (1.8)–(1.12) is ensured provided that there exists a positive number $\beta$ satisfying (3.5). This holds if $f$ is superlinear at $0$ with respect to $\phi$ , i.e., $f_{0}=+\infty$ . Thus we have

Theorem 3.6.

Assume that $\phi$ is a singular homeomorphism such that

(3.10)

\limsup_{x\rightarrow 0}\frac{\phi(\tau x)}{\phi(x)}<+\infty\quad\text{for all% }\tau>0

and $f$ satisfies

f_{0}=+\infty.

Then problem (1.8)–(1.12) has at least one positive solution.

Obviously, the localization of solutions given by Theorem 3.2 allows us to derive multiplicity results provided that there exist several couples of positive numbers $(\alpha,\beta)$ satisfying assumptions (3.4)–(3.5). Some conclusions in this line are collected in the following

Theorem 3.7.

Assume that condition (3.3) holds.

(1)

Let $(\alpha_{i})_{1\leq i\leq k}$ , $(\beta_{i})_{1\leq i\leq k}$ $(k\in\mathbb{N})$ be sets of positive numbers with $\alpha_{i}<\beta_{i}\leq k_{1}\alpha_{i+1}$ for each $i$ . If the assumptions of Theorem 3.2 hold for each couple $(\alpha_{i},\beta_{i})$ , then problem (1.8)–(1.12) has $k$ different solutions $v_{i}$ such that $\alpha_{i}<\left\|v_{i}\right\|<\beta_{i}/k_{1}$ .
(2)

Let $(\alpha_{i})_{1\leq i\leq k}$ , $(\beta_{i})_{1\leq i\leq k}$ $(k\in\mathbb{N})$ be sets of positive numbers with $\alpha_{i}<\beta_{i}<k_{1}\alpha_{i+1}$ for each $i$ . If the assumptions of Theorem 3.2 hold for each couple $(\alpha_{i},\beta_{i})$ , then problem (1.8)–(1.12) has $2k-1$ different solutions $v_{i}$ , $w_{j}$ $(i=1,\ldots,k,\ j=1,\ldots,k-1)$ such that

$\alpha_{i}<\left\|v_{i}\right\|,\ \min_{r\in\left[c,R_{2}\right]}v_{i}\left(r% \right)<\beta_{i}\text{ and }\min_{r\in\left[c,R_{2}\right]}w_{j}\left(r\right% )>\beta_{j},\ \left\|w_{j}\right\|<\alpha_{j+1}.$
(3)

Let $(\alpha_{i})_{i\in\mathbb{N}}$ , $(\beta_{i})_{i\in\mathbb{N}}$ be two sequences of positive numbers with $\alpha_{i}<\beta_{i}\leq k_{1}\alpha_{i+1}$ for each $i$ . If the assumptions of Theorem 3.2 hold for each couple $(\alpha_{i},\beta_{i})$ , then problem (1.8)–(1.12) has infinitely many different solutions $v_{i}$ such that $\alpha_{i}<\left\|v_{i}\right\|<\beta_{i}/k_{1}$ .

Proof.

Let us prove cases (1) and (2).

(1)

For each $i$ , since $\alpha_{i}<\beta_{i}$ , Theorem 3.2 ensures that problem (1.8)–(1.12) has a positive solution $v_{i}$ such that $\alpha_{i}<\left\|v_{i}\right\|<\beta_{i}/k_{1}$ . Now, it suffices to remark that $\beta_{i}/k_{1}\leq\alpha_{i+1}$ implies that $\left\|v_{i}\right\|<\left\|v_{i+1}\right\|$ , so there exist at least $k$ different such solutions.
(2)

For each $i$ , since $\alpha_{i}<\beta_{i}$ , we can derive from the proof of Theorem 3.2 a better localization result: the solution $v_{i}$ belongs to the set $W_{\beta_{i}}\setminus\overline{V}_{\alpha_{i}}$ , that is,

$\alpha_{i}<\left\|v_{i}\right\|,\quad\min_{r\in\left[c,R_{2}\right]}v_{i}\left% (r\right)<\beta_{i}.$

On the other hand, for each $j\in\{1,\ldots,k-1\}$ , since $\beta_{j}<k_{1}\alpha_{j+1}$ , Theorem 3.2 also implies that problem (1.8)–(1.12) has a positive solution $w_{j}$ located in the set $V_{\alpha_{j+1}}\setminus\overline{W}_{\beta_{j}}$ . Thus,

$\min_{r\in\left[c,R_{2}\right]}w_{j}\left(r\right)>\beta_{j},\quad\left\|w_{j}% \right\|<\alpha_{j+1}.$

Since $\alpha_{j+1}<\beta_{j+1}$ , one has that $\left\|w_{j}\right\|<\left\|w_{j+1}\right\|$ . Finally, the estimations

$\min_{r\in\left[c,R_{2}\right]}v_{n}\left(r\right)<\beta_{j}<\min_{r\in\left[c% ,R_{2}\right]}w_{j}\left(r\right)\quad\text{ and }\quad\left\|w_{j}\right\|<% \alpha_{j+1}<\left\|v_{m}\right\|,$

for $n\in\{1,\dots,j\}$ and $m\in\{j+1,\dots,k\}$ , show that $w_{j}$ is also distinct from any $v_{i}$ and so problem (1.8)–(1.12) has at least $2k-1$ different solutions.

The proof of case (3) is analogous and thus we omit it. ∎

3.2. Case of the boundary conditions (1.14)

By a solution of (1.8)–(1.14) we mean a function $v\in C^{1}[R_{1},R_{2}]$ with $v^{\prime}(R_{1})=0=v(R_{2})$ such that $v^{\prime}\in(-a,a)$ , $r^{n-1}\phi(v^{\prime})\in W^{1,1}[R_{1},R_{2}]$ and satisfies (1.8). We will look for nonnegative nontrivial solutions on $[R_{1},R_{2}]$ .

It is clear that $v$ is a nonnegative solution of (1.8)–(1.14) if and only if $v$ is a fixed point of the operator $T_{2}:P\rightarrow P$ defined as

T_{2}(v)(r)=-\int_{r}^{R_{2}}\phi^{-1}\left(-s^{1-N}\int_{R_{1}}^{s}\tau^{N-1}% g\left(\tau\right)f(v(\tau))d\tau\right)ds,

which is a completely continuous operator.

Let us assume that the functions $f$ and $g$ satisfy the following monotonicity assumptions:

(H_f)

$f$ is decreasing on $\mathbb{R}_{+}$ and $0<f(0)<b\int_{R_{1}}^{R_{2}}g(\tau)d\tau$ ;
(H_g)

$r^{N-1}g(r)$ is increasing on $[R_{1},R_{2}]$ .

For a fixed $c\in(R_{1},R_{2})$ , we consider the following subcone of $P$ :

K_{2}=\left\{v\in P:\ v\text{ is decreasing and }\min_{r\in\left[R_{1},c\right% ]}v\left(r\right)\geq k_{2}\left\|v\right\|\right\},

where $k_{2}=(R_{2}-c)/(R_{2}-R_{1})$ .

Note that the operator $T_{2}$ maps the cone $K_{2}$ into itself. Indeed, take $v\in K_{2}$ and let us show that $w:=T_{2}(v)$ belongs to $K_{2}$ . Since $f$ and $g$ are nonnegative, then $w$ is nonnegative and decreasing. Moreover, the monotonicity assumptions on $f$ and $g$ given by (H_f) and (H_g) together with the fact that $v$ is decreasing imply that the function $r\mapsto r^{N-1}g(r)f(v(r))$ is increasing. Thus,

r\mapsto L(w)(r)=r^{N-1}g(r)f(v(r))

is increasing on $[R_{1},R_{2}]$ . Then Theorem 2.2 ensures that $w$ satisfies that

\min_{r\in\left[R_{1},c\right]}w\left(r\right)\geq k_{2}\left\|w\right\|,

so $w\in K_{2}$ .

For any numbers $\alpha,\beta>0$ , define the sets $V_{\alpha}$ and $W_{\beta}$ as in (3.1) and (3.2), with $K_{2}$ instead of $K_{1}$ . Then the following existence and localization result for problem (1.8)–(1.14) can be proved as an application of Theorem 3.1, which guarantees the existence of a fixed point of $T_{2}$ in $W_{\beta}\setminus\overline{V}_{\alpha}$ or in $V_{\alpha}\setminus\overline{W}_{\beta}$ .

We will use the following notation:

A:=\int_{R_{1}}^{R_{2}}g(\tau)d\tau\quad\text{and}\quad B:=\int_{R_{1}}^{c}g(% \tau)d\tau.

Moreover, for any $\alpha,\beta>0$ , denote

M_{\alpha}:=\max\{f(s):s\in[0,\alpha]\}=f(0)\quad\text{and}\quad m_{\beta}:=% \min\{f(s):s\in[\beta,\beta/k_{2}]\}=f(\beta/k_{2}).

It is obvious that the following result can be proved in a similar way to Theorem 3.2, so we omit the proof here.

Theorem 3.8.

Assume that conditions (H_f) and (H_g) hold and that there exist $\alpha,\beta>0$ such that

(3.11)		$\displaystyle-(R_{2}-R_{1})\phi^{-1}\left(-A\,M_{\alpha}\right)$	$\displaystyle<\alpha,$
(3.12)		$\displaystyle-(R_{2}-c)\phi^{-1}\left(-(R_{1}/R_{2})^{N-1}B\,m_{\beta}\right)$	$\displaystyle>\beta.$

(1⁰):: If $\alpha<\beta$ , then problem (1.8)–(1.14) has a positive solution $v$ such that $\alpha<\left\|v\right\|<\beta/k_{2}$ .
(2⁰):: If $\alpha>\beta/k_{2}$ , then problem (1.8)–(1.14) has a positive solution $v$ such that $\beta<\left\|v\right\|<\alpha$ .

Remark 3.9.

If we take into account that $f$ is decreasing, then conditions (3.11) and (3.12) can be rewritten as

(3.13)		$\displaystyle-(R_{2}-R_{1})\phi^{-1}\left(-A\,f(0)\right)$	$\displaystyle<\alpha,$
(3.14)		$\displaystyle-(R_{2}-c)\phi^{-1}\left(-(R_{1}/R_{2})^{N-1}B\,f(\beta/k_{2})\right)$	$\displaystyle>\beta.$

Note that condition (3.13) is always satisfied for $\alpha$ sufficiently large since the left-hand side in the inequality is independent of $\alpha$ . Furthermore, from the fact that $f$ is continuous with $f(0)>0$ , it follows that condition (3.14) holds for any $\beta$ close enough to $0$ .

In view of Theorem 3.8 and Remark 3.9, it is clear that problem (1.8)–(1.14) is always solvable under assumptions (H_f) and (H_g). Thus we have

Corollary 3.10.

If conditions (H_f) and (H_g) hold, then problem (1.8)–(1.14) has at least one positive solution.

Remark 3.11.

Observe that multiplicity results cannot be derived from Theorem 3.8. Indeed, since $A\geq B$ and $f$ is decreasing, one has

A\,f(0)\geq(R_{1}/R_{2})^{N-1}B\,f(\beta/k_{2}),

and so

-(R_{2}-R_{1})\phi^{-1}\left(-A\,f(0)\right)>-(R_{2}-c)\phi^{-1}\left(-(R_{1}/% R_{2})^{N-1}B\,f(\beta/k_{2})\right).

Therefore, any $\alpha$ satisfying (3.13) must be bigger than any $\beta$ for which (3.14) holds.

Remark 3.12.

Observe that the results contained in Section 3.2 remain valid for $R_{1}=0$ , i.e., in the ball.

Note that problem (1.8)–(1.14) with $R_{1}=0$ and $R_{2}=1$ , that is, in the unit ball, was considered in [16], but the results are not comparable since there $f$ was assumed to be nondecreasing.

3.3. Case of the boundary conditions (1.10)

By a solution of (1.8)–(1.10) we mean a function $v\in C^{1}[R_{1},R_{2}]$ with $v(R_{1})=0=v(R_{2})$ such that $v^{\prime}\in(-a,a)$ , $r^{n-1}\phi(v^{\prime})\in W^{1,1}[R_{1},R_{2}]$ and satisfies (1.8). We will look for nonnegative nontrivial solutions on $[R_{1},R_{2}]$ .

To construct the fixed point operator, we need the following technical result, similar to Lemma 1 in [4].

Denote

D_{b}=\left\{h\in P:\ \left\|h\right\|_{L^{1}}<b\left(\frac{R_{1}}{R_{2}}% \right)^{N-1}\right\}.

Lemma 3.13.

For each function $h\in D_{b},$ there exists $R\in\left(R_{1},R_{2}\right)$ such that

\gamma=\int_{R_{1}}^{R}\tau^{N-1}h(\tau)\,d\tau

is the unique number $\gamma$ satisfying

-s^{1-N}\left[\int_{R_{1}}^{s}\tau^{N-1}h(\tau)\,d\tau-\gamma\right]\in\left(-% b,b\right)

and

\int_{R_{1}}^{R_{2}}\phi^{-1}\left(-s^{1-N}\left[\int_{R_{1}}^{s}\tau^{N-1}h(% \tau)\,d\tau-\gamma\right]\right)ds=0.

Moreover, the function $Q_{\phi}:D_{b}\rightarrow\mathbb{R},\ Q_{\phi}\left(h\right)=\gamma$ is continuous.

Proof.

The existence of $R$ with the desired property follows from the proof of Theorem 2.3. Note that for any $h\in D_{b},$ one has

-s^{1-N}\left[\int_{R_{1}}^{s}\tau^{N-1}h(\tau)\,d\tau-\gamma\right]\in\left(-% b,b\right)\ \ \ \text{for all }s\in\left[R_{1},R_{2}\right].

Indeed

\left|-s^{1-N}\left[\int_{R_{1}}^{s}\tau^{N-1}h(\tau)\,d\tau-\gamma\right]% \right|=\left|s^{1-N}\int_{R}^{s}\tau^{N-1}h(\tau)\,d\tau\right|\leq\left(% \frac{R_{2}}{R_{1}}\right)^{N-1}\left\|h\right\|_{L^{1}}<b.

For uniqueness, assume that there exist $\gamma_{i}\in\mathbb{R}$ ( $i=1,2$ ) such that

\int_{R_{1}}^{R_{2}}\phi^{-1}\left(-s^{1-N}\left[\int_{R_{1}}^{s}\tau^{N-1}h(% \tau)\,d\tau-\gamma_{i}\right]\right)ds=0.

Now, by the mean value theorem for integration, there exists $s_{0}\in[R_{1},R_{2}]$ such that

\phi^{-1}\left(-{s_{0}}^{1-N}\left[\int_{R_{1}}^{s_{0}}\tau^{N-1}h(\tau)\,d% \tau-\gamma_{1}\right]\right)ds=\phi^{-1}\left(-{s_{0}}^{1-N}\left[\int_{R_{1}% }^{s_{0}}\tau^{N-1}h(\tau)\,d\tau-\gamma_{2}\right]\right)ds.

This clearly implies that $\gamma_{1}=\gamma_{2}$ .

Finally, for the continuity of $Q_{\phi}$ , let $\left\{h_{n}\right\}_{n\in\mathbb{N}}\subset D_{b}$ such that $h_{n}\rightarrow h_{0}\in D_{b}$ in $C[R_{1},R_{2}]$ . We may assume that $Q_{\phi}(h_{n})\rightarrow\gamma_{0}$ . Passing to limit we find that

\int_{R_{1}}^{R_{2}}\phi^{-1}\left(-s^{1-N}\left[\int_{R_{1}}^{s}\tau^{N-1}h_{% 0}(\tau)\,d\tau-\gamma_{0}\right]\right)ds=0,

and so $\gamma_{0}=Q_{\phi}(h_{0})$ , as wished. ∎

In addition, the solution operator

S:D_{b}\rightarrow C[R_{1},R_{2}],\qquad S(h)(r)=\int_{R_{1}}^{r}\phi^{-1}% \left(-s^{1-N}\left[\int_{R_{1}}^{s}\tau^{N-1}h(\tau)\,d\tau-Q_{\phi}\left(h% \right)\right]\right)ds,

is monotone as shows the next lemma. The proof follows similar ideas to those in [10].

Lemma 3.14.

Let $h_{1},h_{2}\in D_{b}$ , $h_{1}\geq h_{2}$ a.e. on $[R_{1},R_{2}]$ , and let $v_{1},v_{2}\in C^{1}[R_{1},R_{2}]$ be such that for $i=1,2$ , one has $v_{i}(R_{1})=0=v_{i}(R_{2})$ and

L(v_{i})(r)=h_{i}(r)\quad\text{for }r\in(R_{1},R_{2}).

Then $v_{1}\geq v_{2}$ on $[R_{1},R_{2}]$ .

Proof.

Assume to the contrary that $v_{1}\not\geq v_{2}$ . Then there exists an interval $[t_{1},t_{2}]$ , with $R_{1}\leq t_{1}<t_{2}\leq R_{2}$ , such that $v_{1}<v_{2}$ on $(t_{1},t_{2})$ and $v_{1}(t_{i})=v_{2}(t_{i})$ , $i=1,2$ . Hence, by the mean value theorem, there exists $R\in(t_{1},t_{2})$ such that $(v_{1}-v_{2})^{\prime}(R)=0$ . Then

\phi(v_{2}^{\prime})(r)-\phi(v_{1}^{\prime})(r)=\frac{1}{r^{N-1}}\int_{R}^{r}s% ^{N-1}\left[h_{1}(s)-h_{2}(s)\right]\,ds.

Since $h_{1}\geq h_{2}$ , we deduce that $\phi(v_{2}^{\prime})(r)-\phi(v_{1}^{\prime})(r)\geq 0$ on $(R,t_{2})$ . Thus, $v_{2}^{\prime}(r)\geq v_{1}^{\prime}(r)$ on $(R,t_{2})$ which joint with $v_{2}(t_{2})=v_{1}(t_{2})$ imply $v_{1}\geq v_{2}$ on $(R,t_{2})$ , a contradiction. ∎

If $f$ satisfies condition (3.3), then for each $v\in P,$ the function $h:=gf\left(v\right)\in D_{b}$ and since $h\geq 0,$ one has $S\left(h\right)\geq S\left(0\right)=0.$ Hence the operator

T_{3}:P\rightarrow P,\ \ \ \ T_{3}\left(v\right)=S\left(gf\left(v\right)\right)

is well-defined. In addition, thanks to the continuity of $Q_{\phi}$ and the Arzelà-Ascoli theorem, it is completely continuous.

Notice that $v$ is a nonnegative solution of (1.8)–(1.10) if and only if $v$ is a fixed point of the operator $T_{3}.$ Here, for a fixed $c\in(0,(R_{2}-R_{1})/2)$ , we shall look for fixed points of the operator $T_{3}$ in a subcone of $P$ , namely,

K_{3}=\left\{v\in P:\ \min_{r\in I_{c}}v\left(r\right)\geq k_{3}\left\|v\right% \|\right\},

where $k_{3}=\left((R_{2}-R_{1})/2-c\right)/(R_{2}-R_{1})$ and $I_{c}=\left[R_{m}-c,R_{m}+c\right]$ . By the Harnack inequality given by Theorem 2.3, it follows that the operator $T_{3}$ maps the cone $K_{3}$ into itself.

Now, for any numbers $\alpha,\beta>0$ , consider the relatively open sets

V_{\alpha}:=\left\{v\in K_{3}:\left\|v\right\|<\alpha\right\}\quad\text{and}% \quad W_{\beta}:=\left\{v\in K_{3}:\min_{r\in I_{c}}v\left(r\right)<\beta% \right\}.

We will use the following notation:

A:=\int_{R_{1}}^{R_{2}}g(\tau)d\tau\quad\text{and}\quad B:=\min\left\{\int_{R_% {m}-c}^{R_{m}}g(\tau)d\tau,\int_{R_{m}}^{R_{m}+c}g(\tau)d\tau.\right\}.

Moreover, for any $\alpha,\beta>0$ , denote

M_{\alpha}:=\max\{f(s):s\in[0,\alpha]\}\quad\text{and}\quad m_{\beta}:=\min\{f% (s):s\in[\beta,\beta/k_{3}]\}.

Theorem 3.15.

Assume that $f$ satisfies (3.3) and there exist $\alpha,\beta>0$ such that

(3.15)	$\displaystyle(R_{2}-R_{1})\phi^{-1}\left(\left(\frac{R_{2}}{R_{1}}\right)^{N-1% }A\,M_{\alpha}\right)$	$\displaystyle<\alpha,$
(3.16)	$\displaystyle k_{3}\left(R_{m}-R_{1}-c\right)\phi^{-1}\left(B\,m_{\beta}\right)$	$\displaystyle>\beta,$
(3.17)	$\displaystyle-k_{3}\left(R_{2}-R_{m}-c\right)\phi^{-1}\left(-\left(R_{m}/R_{2}% \right)^{N-1}B\,m_{\beta}\right)$	$\displaystyle>\beta.$

(1⁰):: If $\alpha<\beta$ , then problem (1.8)–(1.10) has a positive solution $v$ such that $\alpha<\left\|v\right\|<\beta/k_{3}$ .
(2⁰):: If $\alpha>\beta/k_{3}$ , then problem (1.8)–(1.10) has a positive solution $v$ such that $\beta<\left\|v\right\|<\alpha$ .

Proof.

We shall apply Theorem 3.1. First, let us show that

\left\|T_{3}(v)\right\|<\alpha\quad\text{for all }v\in K_{3}\text{ with }\left\|v\right\|=\alpha,

which clearly implies that $\lambda v\neq T_{3}(v)$ for all $v\in\partial_{K_{3}}V_{\alpha}$ and all $\lambda\geq 1$ . Indeed, for $v\in K_{3}$ with $\left\|v\right\|=\alpha$ , we have that there exists $R\in(R_{1},R_{2})$ such that $\left\|T_{3}(v)\right\|=T_{3}\left(v\right)(R)$ and $(T_{3}(v))^{\prime}(R)=0$ . Thus,

	$\displaystyle T_{3}(v)(r)$	$\displaystyle=$	$\displaystyle\int_{R_{1}}^{r}\phi^{-1}\left(-s^{1-N}\int_{R}^{s}\tau^{N-1}g(% \tau)f(v(\tau))\,d\tau\right)\,ds\ \$
		$\displaystyle=$	$\displaystyle-\int_{r}^{R_{2}}\phi^{-1}\left(-s^{1-N}\int_{R}^{s}\tau^{N-1}g(% \tau)f(v(\tau))\,d\tau\right)\,ds\ \ \ \ (r\in[R_{1},R_{2}]).$

Since $f(v(s))\leq M_{\alpha}$ for every $s\in[R_{1},R_{2}]$ and $S$ is monotone, we have

	$\displaystyle\left\\|T_{3}(v)\right\\|=T_{3}(v)(R)$	$\displaystyle=S\left(gf\left(v\right)\right)\left(R\right)\leq S\left(gM_{% \alpha}\right)\left(R\right)=\int_{R_{1}}^{R}\phi^{-1}\left(-s^{1-N}M_{\alpha}% \int_{R}^{s}\tau^{N-1}g(\tau)\,d\tau\right)\,ds$
		$\displaystyle=\int_{R_{1}}^{R}\phi^{-1}\left(s^{1-N}M_{\alpha}\int_{s}^{R}\tau% ^{N-1}g(\tau)\,d\tau\right)\,ds$
		$\displaystyle\leq(R_{2}-R_{1})\phi^{-1}\left(\left(\frac{R_{2}}{R_{1}}\right)^% {N-1}A\,M_{\alpha}\right)<\alpha,$

as wished.

On the other hand, let us prove that $v\neq T_{3}(v)+\lambda\,h$ for all $v\in\partial_{K_{3}}W_{\beta}$ and all $\lambda\geq 0$ with $h\equiv 1$ . Notice that for $v\in K_{3}$ with $\min_{r\in I_{c}}v(r)=\beta$ , we have that $\beta\leq v(r)\leq\beta/k_{3}$ for all $r\in I_{c}$ , and thus $m_{\beta}\leq f(v(r))$ for all $r\in I_{c}$ . Hence, $f(v(r))\geq m_{\beta}\chi_{I_{c}}(r)$ for all $r\in[R_{1},R_{2}]$ (where $\chi_{I_{c}}$ denotes the characteristic function of $I_{c}$ ). Then Lemma 3.14 implies that

T_{3}(v)(r)\geq S(m_{\beta}\,g\,\chi_{I_{c}})(r),\qquad(r\in[R_{1},R_{2}]).

Note that there is $R\in(R_{1},R_{2})$ such that

S(m_{\beta}\,g\,\chi_{I_{c}})(r)=\int_{R_{1}}^{r}\phi^{-1}\left(-s^{1-N}m_{% \beta}\int_{R}^{s}\tau^{N-1}g(\tau)\chi_{I_{c}}(\tau)\,d\tau\right)\,ds.

Now, suppose that $R\geq R_{m}$ . Then

	$\displaystyle T_{3}(v)(R_{m}-c)$	$\displaystyle\geq S(m_{\beta}\,g\,\chi_{I_{c}})(R_{m}-c)$
		$\displaystyle=\int_{R_{1}}^{R_{m}-c}\phi^{-1}\left(s^{1-N}m_{\beta}\int_{R_{m}% -c}^{R}\tau^{N-1}g(\tau)\chi_{I_{c}}(\tau)\,d\tau\right)\,ds$
		$\displaystyle\geq\int_{R_{1}}^{R_{m}-c}\phi^{-1}\left(s^{1-N}m_{\beta}\int_{R_% {m}-c}^{R_{m}}\tau^{N-1}g(\tau)\chi_{I_{c}}(\tau)\,d\tau\right)\,ds$
		$\displaystyle\geq(R_{m}-R_{1}-c)\phi^{-1}\left(B\,m_{\beta}\right)$
		$\displaystyle>\beta/k_{3},$

that is, $T_{3}(v)(R_{m}-c)>\beta/k_{3}\geq v(r)$ for all $r\in I_{c}$ . In particular, $T_{3}(v)(R_{m}-c)>v(R_{m}-c)$ .

Analogously, if $R\leq R_{m}$ , then

$\displaystyle T_{3}(v)(R_{m}+c)$	$\displaystyle\geq$	$\displaystyle S(m_{\beta}\,g\,\chi_{I_{c}})(R_{m}+c)$
	$\displaystyle=$	$\displaystyle-\int_{R_{m}+c}^{R_{2}}\phi^{-1}\left(-s^{1-N}m_{\beta}\int_{R}^{% s}\tau^{N-1}g(\tau)\chi_{I_{c}}(\tau)\,d\tau\right)\,ds\$
	$\displaystyle=$	$\displaystyle-\int_{R_{m}+c}^{R_{2}}\phi^{-1}\left(-s^{1-N}m_{\beta}\int_{R_{m% }}^{R_{m}+c}\tau^{N-1}g(\tau)\chi_{I_{c}}(\tau)\,d\tau\right)\,ds$
	$\displaystyle\geq$	$\displaystyle-\left(R_{2}-R_{m}-c\right)\phi^{-1}\left(-\left(R_{m}/R_{2}% \right)^{N-1}B\,m_{\beta}\right)$
	$\displaystyle>$	$\displaystyle\beta/k_{3}.$

we may prove that $T_{3}(v)(R_{m}+c)>\beta/k_{3}\geq v(r)$ for all $r\in I_{c}$ .

Therefore, $v\neq T_{3}(v)+\lambda$ for all $v\in\partial_{K_{3}}W_{\beta}$ and all $\lambda\geq 0$ . The conclusion follows from Theorem 3.1. ∎

Remark 3.16.

If $\phi$ is odd then the two conditions (3.16)and (3.17) on $\beta$ reduce to the unique inequality

(3.18)

k_{3}\left(R_{2}-R_{m}-c\right)\phi^{-1}\left(\left(R_{m}/R_{2}\right)^{N-1}Bm% _{\beta}\right)>\beta.

We emphasize that if $\phi$ is a classical or bounded odd homeomorphism, then conditions (3.15) and (3.18) can be rewritten as

\frac{M_{\alpha}}{\phi\left(C_{1}\,\alpha\right)}<C_{2}\quad\text{and}\quad% \frac{m_{\beta}}{\phi\left(C_{3}\,\beta\right)}>C_{4},

for certain positive constants $C_{1}$ , $C_{2}$ , $C_{3}$ and $C_{4}$ . Therefore, existence results for sublinear and superlinear nonlinearities can be proven exactly as in Section 3.1.

Theorem 3.17.

Assume that $\phi$ is odd and that one of the following conditions holds:

(i):: $f_{0}=+\infty$ , $f_{\infty}=0$ and $\phi$ is a classical or bounded homeomorphism satisfying (3.6).
(ii):: $f_{0}=0$ , $f_{\infty}=+\infty$ and $\phi$ is a classical homeomorphism satisfying (3.9).
(iii):: $f_{0}=+\infty$ and $\phi$ is a singular homeomorphism satisfying (3.10).

Then problem (1.8)–(1.10) has at least one positive solution.

Remark 3.18.

Theorem 3.15 allows us to deduce the existence of multiple positive solutions for problem (1.8)–(1.10) provided that there are several pairs of positive numbers $(\alpha,\beta)$ satisfying conditions (3.15)–(3.17).

4. Numerical examples

From numerical point of view we will consider three distinct boundary value problems. In order to solve them we make use of the new and powerful MATLAB package Chebfun which is a product of the numerical analysis group at Oxford University led by Professor Trefethen (see for instance [17] and [18] to quote but a few).

The philosophy behind this package is non-standard in numerical analysis and can be summed up in the words of its initiator as “Feel symbolic but run at the speed of numerics”.

In short, the method implemented by Chebfun is a Chebyshev type collocation one. Chebfun tries to solve a BVP by using successively to approximate the solution Chebyshev polynomials on grids of size $17$ , $33$ , $65\ldots$ until the spectral convergence is reached. The relative accuracy of each computation carried out by a Chebfun algorithm is usually about $16$ digits, and in principle the user need have no knowledge of the underlying algorithms. However, when solving a nonlinear BVP, Chebfun provides useful information on the convergence of the Newtonian method used to solve nonlinear algebraic systems obtained by discretization. In addition, the behavior of the solution coefficients can be visualized (the way in which they decrease to the machine accuracy). We will display these two outputs for each of the three issues considered. In fact, we must emphasize that we have used Chebfun with excellent results in our previous works [7] and [14].

4.1. First example: a Dirichlet-Neumann problem

Consider the Dirichlet-Neumann problem for an equation involving a singular homeomorphism

(4.1)

\left\{\begin{array}[]{l}-\left(r\frac{v^{\prime}}{\sqrt{1-v^{\prime 2}}}% \right)^{\prime}=rg\left(r\right)f\left(v\right),\ \ \ r\in\left(1,2\right)\\ v\left(1\right)=v^{\prime}\left(2\right)=0,\end{array}\right.

where

g\left(r\right)=\frac{r+1}{2r^{2}+1},\ \ \ \ f\left(v\right)=v^{2}+1.

Refer to caption — Figure 1. Graph of the numerical solution of problem (4.1). The initial guess for the initialization of the Newton procedure is $v_{0}:=1.$

The residual Chebfun satisfies the operator is of order $10^{-10}$ and the boundary conditions are satisfied exactly.

From the left panel of Fig. 2 it is very clear that Newton method converges with an order of at most $2$ and from the right panel of the same figure one can observe that a Chebyshev polynomial of order $16$ , with highly and smoothly decreasing coefficients is the solution of this problem.

4.2. Second example: a Neumann-Dirichlet problem

We now solve numerically the following problem

(4.2)

\left\{\begin{array}[]{l}-\left(r\frac{v^{\prime}}{\sqrt{1-v^{\prime 2}}}% \right)^{\prime}=rg\left(r\right)f\left(v\right),\ \ \ r\in\left(0,1\right)\\ v^{\prime}\left(0\right)=v\left(1\right)=0,\end{array}\right.

where

g\left(r\right)=e^{-r}+\frac{1}{2}r,\ \ \ \ f\left(v\right)=\frac{1}{v^{2}+1}.

The residual Chebfun satisfies the operator is of order $10^{-11}$ and the boundary conditions are satisfied exactly.

From the left panel of Fig. 4 it is very clear that Newton method converges with an order of at least $2$ and from the right panel of the same figure one can observe that a Chebyshev polynomial of order $17$ , with highly decreasing coefficients is the solution of the problem.

4.3. Third example: a Dirichlet problem

The last example is giving by the Dirichlet problem

(4.3)

\left\{\begin{array}[]{l}-\left(r\frac{v^{\prime}}{\sqrt{1-v^{\prime 2}}}% \right)^{\prime}=rg\left(r\right)f\left(v\right),\ \ \ r\in\left(1,2\right)\\ v\left(1\right)=v\left(2\right)=0,\end{array}\right.

where

g\left(r\right)=1,\ \ \ \ f\left(v\right)=\frac{v+1}{v^{2}+1}.

The residual Chebfun satisfies the operator is of order $10^{-10}$ and the boundary conditions are satisfied exactly.

From the left panel of Fig. 6 it is very clear that Newton method converges with an order of at least $2$ and from the right panel of the same figure one can observe that a Chebyshev polynomial of order $24$ , with highly decreasing coefficients is the solution of the problem.

We must make an important remark at the end of these three examples. Spectral convergence occurs for solutions represented by Chebyshev polynomials of relatively small order (of the order of a few tens). Moreover and more important, the convergence is so fast that no rounding off plateau appears (see the right panels of the figures 2, 4 and 6).

Acknowledgements

Jorge Rodríguez-López was partially supported by Institute of Advanced Studies in Science and Technology of Babeş-Bolyai University of Cluj-Napoca (Romania) under a Postdoctoral Advanced Fellowship, project CNFIS-FDI-2021-0061; by Xunta de Galicia (Spain), project ED431C 2019/02 and AIE, Spain and FEDER, grant PID2020-113275GB-I00.

References

[1] C. Bereanu, P. Jebelean and J. Mawhin, Radial solutions for some nonlinear problems involving mean curvature operators in Euclidean and Minkowski spaces, Proc. Amer. Math. Soc., 137 1 (2009), 161–169.
[2] C. Bereanu, P. Jebelean and J. Mawhin, Radial solutions for Neumann problems with $\phi$ -Laplacians and pendulum-like nonlinearities, Discrete Contin. Dyn. Syst., 28 (2010), 637–648.
[3] C. Bereanu, P. Jebelean and P. J. Torres, Positive radial solutions for Dirichlet problems with mean curvature operators in Minkowski space, J. Funct. Anal., 264 (2013), 270–287.
[4] C. Bereanu and J. Mawhin, Existence and multiplicity results for some nonlinear problems with singular $\phi$ -Laplacian, J. Differential Equations, 243 (2007), 536–557.
[5] F. Cianciaruso, G. Infante and P. Pietramala, Non-zero radial solutions for elliptic systems with coupled functional BCs in exterior domains, Proc. Edinb. Math. Soc., 62 (2019), 747–769.
[6] I. Coelho, C. Corsato and S. Rivetti, Positive radial solutions of the Dirichlet problem for the Minkowski-curvature equation in a ball, Topol. Methods Nonlinear Anal., 44 1 (2014), 23–39.
[7] C.-I. Gheorghiu, A Third-Order BVP on the Real Line, January 2020, https://www.chebfun.org/examples/ode-nonlin/index.html
[8] D. Gurban and P. Jebelean, Positive radial solutions for multiparameter Dirichlet systems with mean curvature operator in Minkowski space and Lane-Emden type nonlinearities, J. Differential Equations, 266 (2019), 5377–5396.
[9] D.-R. Herlea, Positive solutions for second-order boundary-value problems with $\phi$ -Laplacian, Electron. J. Differential Equations, 2016 (2016), 1-8.
[10] D.-R. Herlea, Existence, localization and multiplicity of positive solutions for the Dirichlet BVP with $\phi$ -Laplacian, Fixed Point Theory, 18 (2017), 237–246.
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[12] R. Precup, Positive solutions of semi-linear elliptic problems via Krasnoselskii type theorems in cones and Harnack’s inequality, in Mathemathical Analysis and Applications, Eds. C.P. Niculescu and V.D. Rădulescu, AIP Conf. Proc. 835, 2006, 125-132.
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[1] C. Bereanu, P. Jebelean, J. Mawhin, Radial solutions for some nonlinear problems involving mean curvature operators in Euclidean and Minkowski spaces, Proc. Amer. Math.
[2] C. Bereanu, P. Jebelean, J. Mawhin, Radial solutions for Neumann problems with ϕ-Laplacians and pendulum-like nonlinearities, Discrete Contin. Dyn. Syst. 28(2010), 637– 648. https://doi.org/10.3934/dcds.2010.28.637; MR2644761
[3] C. Bereanu, P. Jebelean, P. J. Torres, Positive radial solutions for Dirichlet problems with mean curvature operators in Minkowski space, J. Funct. Anal. 264(2013), 270–287. https://doi.org/10.1016/j.jfa.2012.10.010; MR2995707
[4] C. Bereanu, J. Mawhin, Existence and multiplicity results for some nonlinear problems with singular ϕ-Laplacian, J. Differential Equations 243(2007), 536–557. https://doi.org/ 10.1016/j.jde.2007.05.014; MR2371799
[5] F. Cianciaruso, G. Infante, P. Pietramala, Non-zero radial solutions for elliptic systems with coupled functional BCs in exterior domains, Proc. Edinb. Math. Soc. (2) 62(2019), 747–769. https://doi.org/10.1017/S0013091518000706; MR3974965
[6] I. Coelho, C. Corsato, S. Rivetti, Positive radial solutions of the Dirichlet problem for the Minkowski-curvature equation in a ball, Topol. Methods Nonlinear Anal. 44(2014), No. 1, 23–39. https://doi.org/10.12775/TMNA.2014.034; MR3289006
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[8] C.-I. Gheorghiu, Chebfun solutions to a class of 1D singular and nonlinear boundary value problems, Computation 10(2022), 10(7), 116. https://doi.org/10.3390/ computation10070116.
[9] D. Gurban, P. Jebelean, Positive radial solutions for multiparameter Dirichlet systems with mean curvature operator in Minkowski space and Lane–Emden type nonlinearities, J. Differential Equations 266(2019), 5377–5396. https://doi.org/j.jde.2018.10.030;MR3912753
[10] D.-R. Herlea, Positive solutions for second-order boundary-value problems with ϕLaplacian, Electron. J. Differential Equations 2016, No. 51, 1–8. MR3466522
[11] D.-R. Herlea, Existence, localization and multiplicity of positive solutions for the Dirichlet BVP with ϕ-Laplacian, Fixed Point Theory 18(2017), 237–246. https://doi.org/10. 24193/fpt-ro.2017.1.20; MR3675538
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On the localization and numerical computation of positive radial solutions for φ-Laplace equations in the annulus

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On the localization and numerical computation of positive radial solutions for ϕ-Laplace equations in the annulus

Abstract.

Key words and phrases:

1991 Mathematics Subject Classification:

1. Introduction

2. Harnack type inequalities

2.1. Case of the boundary conditions (1.12)

Theorem 2.1.

Proof.

2.2. Case of the boundary conditions (1.14)

Theorem 2.2.

Proof.

2.3. Case of the boundary conditions (1.10)

Theorem 2.3.

Proof.

3. Existence and localization

Theorem 3.1 (Krasnosel’skiĭ).

3.1. Case of the boundary conditions (1.12)

Theorem 3.2.

Proof.

Theorem 3.3.

Proof.

Theorem 3.4.

Remark 3.5.

Theorem 3.6.

Theorem 3.7.

Proof.

3.2. Case of the boundary conditions (1.14)

Theorem 3.8.

Remark 3.9.

Corollary 3.10.

Remark 3.11.

Remark 3.12.

3.3. Case of the boundary conditions (1.10)

Lemma 3.13.

Proof.

Lemma 3.14.

Proof.

Theorem 3.15.

Proof.

Remark 3.16.

Theorem 3.17.

Remark 3.18.

4. Numerical examples

4.1. First example: a Dirichlet-Neumann problem

4.2. Second example: a Neumann-Dirichlet problem

4.3. Third example: a Dirichlet problem

Acknowledgements

References

References

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On the localization and numerical computation of positive radial solutions for $\phi$ -Laplace equations in the annulus