Abstract
Let \(\mathbb {A}=\{z: r< |z|<R\}\) and \(\mathbb {A}^*=\{z: r^*<|z|<R^*\}\) be annuli in the complex plane. Let \(p\in [1,2]\) and assume that \(\mathcal {H}^{1,p}(\mathbb {A},\mathbb {A}^*)\) is the class of Sobolev homeomorphisms between \(\mathbb {A}\) and \(\mathbb {A}^*\), \(h:\mathbb {A}\xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}\mathbb {A}^*\). Then we consider the following Dirichlet type energy of h:
We prove that this energy integral attains its minimum, and the minimum is a certain radial diffeomorphism \(h:\mathbb {A}\xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}\mathbb {A}^*\), provided a radial diffeomorphic minimizer exists. If \(p>1\) then such diffeomorphism exists always. If \(p=1\), then the conformal modulus of \(\mathbb {A}^*\) must not be greater or equal to \(\pi /2\). This curious phenomenon is opposite to the Nitsche type phenomenon known for the standard Dirichlet energy.
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1 Introduction
The general law of hyperelasticity tells us that there exists an energy integral \( E[h] = \int _\mathbb {X}E(x, h, Dh) dx\) where \(E: \mathbb {X} \times \mathbb {Y} \times \mathbb {R}^{n\times n}\rightarrow \mathbb {R}\) is a given stored-energy function characterizing mechanical properties of the material. Here \(\mathbb {X}\) and \(\mathbb {Y}\) are nonempty bounded domains in \(\mathbb {R}^n, n > 2.\) The mathematical models of nonlinear elasticity have been first studied by Antman [1], Ball [4, 5], and Ciarlet [8]. One of the interesting and important problems in nonlinear elasticity is whether the radially symmetric minimizers are indeed global minimizers of the given physically reasonable energy. This leads us to study energy minimal homeomorphisms \(h: \mathbb {A}\xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}\mathbb {A}^*\) of Sobolev class \(\mathscr {W}^{1,2}\) between annuli \(\mathbb {A}= \mathbb {A}(r, R) = \{x \in \mathbb {R}^n: r< |x| < R\}\) and \(\mathbb {A}^*=\mathbb {A}(r_*, R_*) = \{x \in \mathbb {R}^n: r_*< |x| < R_*\}\). Here \(0 \leqslant r < R\) and \(0 \leqslant r_*< R_*\) are the inner and outer radii of \(\mathbb {A}\) and \(\mathbb {A}^*\). The variational approach to Geometric Function Theory [2, 3] makes this problem more important. Indeed, several papers are devoted to understanding the expected radial symmetric properties see [17] and the references therein. Many times experimentally known answers to practical problems have led us to the deeper study of such mathematically challenging problems. We seek to minimize the p-harmonic energy of mappings between two annuli in \(\mathbb {R}^2\). We consider the modified Dirichlet energy \(\mathscr {F}_p[f]=\int _{\mathbb {A}}\frac{\Vert Df\Vert ^p}{|f|^p}\), \(1\leqslant p\leqslant 2\) and minimize it.
2 p-harmonic equation and statement of the main results
For natural number n, let \(A=(a_{i,j})_{n\times n}\in \mathbb {R}^{n\times n}\). We use \(A^{T}\) to denote the transpose of A. The Hilbert-Schmit norm, also called the Frobenius norm, of A is denoted by \(\Vert A\Vert \), where
For \(p\ge 1\), we say that a mapping h belongs to the class \(\mathcal {W}^{1, p}(\mathbb {A},\mathbb {A}^*)\), if h belongs to the Sobolev space \(\mathcal {W}^{1, p}(\mathbb {A})\) and maps \(\mathbb {A}\) onto \(\mathbb {A}^*\). Let \(h=(h^{1},\ldots ,h^{n})\) belong to \(\mathcal {W}^{1,p}(\mathbb {A},\mathbb {A}^*)\). We denote the Jacobian matrix of h at the point \(x=(x_{1},\ldots ,x_{n})\) by Dh(x), where \(Dh(x)=\left( \frac{\partial h^{i}}{\partial x_{j}} \right) _{n\times n}\in \mathbb {R}^{n\times n}\). Then
Here \(\frac{\partial h^{i}}{\partial x_{j}}\) denotes the weak partial derivatives of \(h^{i}\) with respect to \(x_{j}\). If h is continuous and belongs to \(\mathcal {W}^{1, p}(\mathbb {A},\mathbb {A}^*)\) \((p\ge 1)\), then the weak and ordinary partial derivatives coincide a.e. in \(\mathbb {A}\) (cf. [19, Proposition 1.2]). Let \(h=\rho S\), where \(S=\frac{h}{|h|}\) and \(\rho =|h|\). By [14, Equality (3.2)], we obtain that
and
where \(\nabla \rho \) denotes the gradient of \(\rho \).
We say that \(h:\mathbb {A} \rightarrow \mathbb {A}^{*} \) is a radial mapping, if \(h(x)=\rho (|x|)\frac{x}{|x|}\) and if \(\rho \) is real and positive function. We use \(\mathcal {R}(\mathbb {A},\mathbb {A}^*)\) to denote the class of radial homeomorphisms in \(\mathcal {W}^{1,p}(\mathbb {A},\mathbb {A}^*)\) and use \(\mathcal {P}(\mathbb {A},\mathbb {A}^*)\) to denote the class of generalized radial homeomorphisms in \(\mathcal {W}^{1,p}(\mathbb {A},\mathbb {A}^*)\). We also use \(\mathcal {H}(\mathbb {A},\mathbb {A}^*)\) to denote the class of homeomorphisms in \(\mathcal {W}^{1,p}(\mathbb {A},\mathbb {A}^*)\).
As it is said before, an important problems in nonlinear elasticity is whether the radially symmetric minimizers are indeed global minimizers. For example, Iwaniec, and Onninen [12] discussed the minimizers of the following two energy integrals:
among all homeomorphisms in \(\mathcal {W}^{1,n}(\mathbb {A},\mathbb {A}^{*})\), respectively. The energy integral \(\mathfrak {F}\) for \(n=2\), has been considered previously by Astala, Iwaniec, and Martin in [2]. Further such energy has been generalized in planar annuli by Kalaj in [15, 16] and spatial annuli in [13]. On the other hand, Koski and Onninen [17] investigated the minimizers of the p-harmonic energy
among all homeomorphisms in \(\mathcal {W}^{1,p}(\mathbb {A},\mathbb {A}^{*})\), where \(\mathbb {A}\) and \(\mathbb {A}^{*}\) are planar annuli and \(1\le p<2\), provided the homeomorphisms fix the outer boundary. Recently, Kalaj [14] studied the Dirichlet-type energy \(\mathscr {F}[h]\) among mappings in \(\mathcal {H}(\mathbb {A},\mathbb {A}^*)\), where
For \(n=3\), the author proved that the minimizers of \(\mathscr {F}[h]\) are certain generalized radial diffeomorphism (cf. [14, Theorem 1.1]). Motivated by the case \(n=3\), in [14] it was posed the following question.
Question 2.1
For \(n\not =3\), does the Dirichlet integral of \(h\in \mathcal {H}(\mathbb {A},\mathbb {A}^{*}) \), i.e. the integral
achieve its minimum for generalized radial diffeomorphisms between annuli?
Then in the subsequent paper by Kalaj and Chen [9] was given the following answer.
Theorem 2.1
For \(n \ge 4\), we have
The last infimum is never attained.
In this paper, we consider the case of the p-energy Sobolev \(\mathcal {W}^{1,p}\) homeomorphisms between annuli \(\mathbb {A}\) and \(\mathbb {A}^*\) in the complex plane. Let
Then we seek the homeomorphisms h of the class \(\mathcal {W}^{1,p}\) which are furthermore assumed to preserve the order of the boundary components \(|h(z)|\rightarrow \)r when \(|z|\rightarrow r^*\) and \(|h(z)|\rightarrow R^*\) when \(|z|\rightarrow R\). Such a class of Sobolev homeomorphisms with the above property is denoted by \(\mathcal {H}^{1,p}(\mathbb {A},\mathbb {A}^*)\) and we say that they are admissible homeomorphisms. Since we minimize the \(\mathscr {F}_p\) energy in the class of homeomorphisms, we can perform the inner variation of the independent variable \(z_\epsilon = z + \epsilon \tau (z)\), which leads to the system (see for example [14])
where
Here \(z=(x,y)\). Our argument does not make direct use of the inner variational equation (2.3). Some important facts that follow from (2.3) are as follows.
-
(1)
If we assume that h is radial, then (2.3) reduces to the Euler-Lagrange equation (3.1) below.
-
(2)
Further if f is a solution of (2.3) then so is \(\tilde{f}=\frac{1}{f}\).
-
(3)
Let \(f_1(z)=\frac{1}{r_*} f(r z)\). Then \(f_1:\mathbb {A}(1,r_1)\xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}\mathbb {A}(1,R_1)\), provided that \(f:\mathbb {A}(r,R)\xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}\mathbb {A}(r^*, R^*)\), where \(R_1=R_*/r_*\) and \(r_1=R/r\). Moreover, f satisfies (2.3) if and only if \(f_1\) satisfies the same equation.
This is why we reduce the problem to the annuli \(\mathbb {A}=\mathbb {A}(1,r)\) and \(\mathbb {A}^*=\mathbb {A}(1,R)\). Now we formulate the main results.
Theorem 2.2
Let \(\mathbb {A}\) and \(\mathbb {A}^*\) be planar annuli and \(1< p\leqslant 2.\) Then there exists a radially symmetric mapping \(h_\circ :\mathbb {A}\rightarrow \mathbb {A}^*\) such that
The map \(h_\circ \) is the unique minimizer, up to a rotation, in the class \(\mathcal {H}^{1,p}(\mathbb {A},\mathbb {A}^*)\). Furthermore, the minimizer \(h_\circ \) is a homeomorphism.
Theorem 2.3
Let \(\mathbb {A}\) and \(\mathbb {A}^*\) be planar annuli. Then there exists a radially symmetric mapping \(h_\circ :\mathbb {A}\rightarrow \mathbb {A}^*\) which is a homeomorphism such that
if and only if
The map \(h_\circ \) is the unique minimizer, up to a rotation, in the class \(\mathcal {H}^{1,1}(\mathbb {A},\mathbb {A}^*)\).
Remark 2.4
Note that the case \(p=2\) of Theorem 2.2 has been already considered by Astala, Iwaniec, and Martin in [2].
On the other hand side our result can be seen as a variation of minimization property of radial mappings of p-Dirichlet energy throughout Sobolev mappings from the unit ball \(\mathbb {B}\subset \mathbb {R}^n\) onto the unit sphere \(\mathbb {S}^{n-1}\), fixing the boundary. This is an old problem solved by several authors (see for example [6, 7, 18]).
Furthermore, as was remarked before, Koski and Onninen [17] have considered \(\mathcal {E}_{p}\) energy and proved the minimization property, under a certain constrain. Indeed, if we denote the outer boundary of \(\mathbb {A}\) by \(\partial _\circ \mathbb {A}\) and consider the subfamily of homomorphisms \(\mathcal {H}_\circ =\{f\in \mathcal {H}^{1,p}(\mathbb {A},\mathbb {A}^*): f(x)=\frac{R_*}{R} x, \ \text { for } x\in \partial _\circ \mathbb {A}\}\), then the minimizer of \(\mathcal {E}_{p}\) energy is a radial mapping \(h(x)=\rho (x)\frac{x}{|x|}\) provided that R and r satisfies some inequality that depends on p ([17, Theorem 1.5]). In the same paper they proved that this constraint is crucial and there exists annuli, where the minimizer of \(\mathcal {E}_{p}\) is not a radial mapping.
Remark 2.5
By virtue of the density of diffeomorphisms in \(\mathcal {H}^{1,p}(\mathbb {A},\mathbb {A}^*)\), see [10, 11], we can equivalently replace the admissible homeomorphisms by sense preserving diffeomorphims. Indeed, for \(p \geqslant 1\), we have
Here by \(\textrm{Diff}(\mathbb {A},\mathbb {A}^*)\) we denote the class of orientation preserving diffeomorphisms from \(\mathbb {A}\) onto \(\mathbb {A}^*\) which also preserve the order of the boundary components. A similar result hold for the \(\mathscr {F}_p\) energy. Indeed
3 Radial minimizer of the energy \(\mathscr {F}_p[h]\), \(1<p<2\)
This section aims is to find the radial minimizer \(h_\circ \) of \(\mathscr {F}_p\) energy that maps annuli \(\mathbb {A}(1,r)\) onto \(\mathbb {A}(1,R)\) keeping the boundary order. Moreover, we will use that solution to prove the minimization property of \(h_\circ \) in the class of all Sobolev homeomorphisms. Contrary to the case \(p=1\), which will be considered later, we will not have any restriction on r and R. Assume that \(h(z) = H(t) e^{i \theta }\), where \(z=t e^{i\theta }\), where H is a differentiable function and that \(t\in [1,r]\), \(\theta \in [0,2\pi ]\). Then
Furthermore
Let
Then Euler-Lagrange equation
can be written in the following form
where \(H=H(t)\), \(\dot{H}= H'(t)\) and \(\ddot{H}=H''(t)\). Then by straightforward calculation (3.1) can be reduced to the following differential equation
where g is a solution to the following differential equation
Show that \(F<0\) provided that \(t\geqslant 1\) and \(g(t)\in (0,1)\). Namely
Since \(2 (2-p) (g(t)-1) g(t)<0\) we infer that g is a decreasing function.
The general solution of (3.3) is given by \(g=k^{-1}\), where the function k is defined by
where b is a positive constant and \(s\in (0,1)\).
By (3.2) we infer that H is given by
By using the change \(t=k(s)\) in (3.5) we obtain
Since we seek increasing homeomorphic mappings \(H:[1,r]\xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}[1,R]\), we have the initial conditions \(H(1)=1\) and \(H(r)=R\). Then \(C=1\). Let \(0<\tau <1\) and chose \(b=b(\tau )\) so that
Denote the corresponding g by \(g_\tau \). Then we have \(g_\tau (1)=\tau \).
Moreover by (3.4)
Define the function
Then we also define
Then
and
Let us show that there is a unique \(s_\circ =s(r,\tau )\in (0,\tau )\) such that \(B(s_\circ )=0\), where
Note that B is continuous, \(B(\tau )=\log \frac{1}{r}<0\) and \(B(0)=+\infty \). Moreover
Thus there is a unique \(s_\circ \) so that \(B(s_\circ )=0\). Then \(g_\tau (r)=s_\circ \). Since for \(0<s<\tau \) and \(p\in (1,2]\), we have
it follows that
Thus
Then
Let us show now that, if \(p>1\), then for every \(R\in (1,+\infty )\), there is \(\tau \in (0,1)\) so that \(\mathcal {R}(\tau )=R\). It is clear that \(\mathcal {R}\) is continuous and also it is clear that \(\lim _{\tau \rightarrow 0} \mathcal {R}(\tau )=1\). Let us show that \(\lim _{\tau \rightarrow 1} \mathcal {R}(\tau )=+\infty \). Observe that \(0\leqslant s\leqslant \sqrt{s}\leqslant 1\). Then from (3.8) we have that
where
Then \(K(\tau )=\exp (k(\tau )-k(\tau _0))\), where
Then
We notice that here is the moment where \(p\in (1,2)\) is an important assumption. In particular \(\lim _{\tau \rightarrow 1} R(\tau )=\infty \). So there is \(\tau =\tau (r, R)\) so that \(\mathcal {R}(\tau )=R\). In view of (3.7), we have constructed a smooth increasing mapping \(H=H_\circ =H_{r,R}:[1,r]\rightarrow [1,R]\) so that \(H(1)=1\) and \(H(r)=R\), See Fig. 1 below. Let us show that
is the minimizer in the class of radial homeomorphisms between \(\mathbb {A}\) and \(\mathbb {A}^*\).
Assume now that \(H: [1,r]\rightarrow [1,R]\) is any smooth homeomorphism and assume that \(h(z)=H(t)e^{i\theta }\). Prove that
We start from a simple inequality from [17]
By inserting \(q=p\), \(s=g(t)\),
in (3.11) we have
The equality in (3.11) is attained precisely when
and thus the equality is attained in (3.12) precisely when
Then by
where \(a=\frac{\dot{H}(t)}{H(t)}\) and \(x=\frac{\sqrt{g(t)}}{\sqrt{1-g(t)} t}\) we get
Notice that, the condition (3.13) is precisely satisfied when we have equality in (3.15).
Define
and show that it is a constant. This fact is crucial for our approach.
By (3.3) we obtain that
Thus
Observe that
Thus \(c=c(r,R)\). Now we have
4 Radial minimizers for the case \(p=1\)
The corresponding subintegral expression for the functional \(\mathscr {F}_1[h]=\int _{\mathbb {A}(1,r)} \frac{|Df(z)|}{|f(z)|}\), for radial function \(h(z)=H(t)e^{i\theta }\), \(z=te^{i\theta }\) is given by
The corresponding differential equation (3.1) for \(p=1\) reduces to
which can be written in the following form
where g is a solution of the differential equation (see (3.3) for \(p=1\)):
Then the general solution of (4.2) is given by \(g(t) = {b t^{-2}}.\) Then the solution of (4.1) is the solution of the equation
and it is given by
If we let that \(H(1)=1\) then
Here \(b\geqslant 1\). Moreover, if we assume that \(H(r)=R\), then after straightforward computations we get
The corresponding minimizer is denoted by \(h_\circ (z)=H(r)e^{i\theta },\) \(z=re^{i\theta }\). Hence
Thus
where
Lemma 4.1
It exists a radial homeomorphism \(h: \mathbb {A}(1,r)\rightarrow \mathbb {A}(1,R)\) if and only if
Proof
By differentiating (4.3) w.r.t. b we get
Hence H is decreasing in b. The largest value is for \(b=1\) and it is equal to
for \(t=r\). In other words, there is a increasing diffeomorphism of [1, r] onto [1, R] if and only if \(R\leqslant R_\circ (r).\) \(\square \)
Remark 4.2
Observe that \(\lim _{r\rightarrow \infty } \mathcal {R}(r)=e^{\pi /2}\), so there is not any homeomorphic minimizer of the \(\mathscr {F}\) energy between annuli \(\mathbb {A}(1,r)\) and \(\mathbb {A}(1,e^{\pi /2})\). Note that the conformal modulus of \(\mod \mathbb {A}(1,e^{\pi /2})\) is \(\log e^{\pi /2}=\pi /2\). So the case \(p=1\) differs from the case \(p>1\). Moreover, this case is also opposite to the Nitsche type phenomenon for Dirichlet energy \(\mathcal {E}\). Namely Nitsche type phenomenon asserts that the modulus of image domain could be arbitrarily large, but not small enough.
5 Proof of Theorem 2.2 and Theorem 2.3
We begin with the following proposition
Proposition 5.1
Assume that \(h=\rho (z)e^{i\Theta (z)}\) is a diffeomorphism between annuli \(\mathbb {A}(1,r)\) and \(\mathbb {A}(1,R)\). Then for every \(t\in [1,r]\) and \(\theta \in [0,2\pi ]\) we have
If the equality hold in (5.1) for every \(\theta \in [0,2\pi ]\), then \(\Theta (z) =e^{i\varphi (\theta )},\) \(z=te^{i\theta }\), for a diffeomorphism \(\varphi :[0,2\pi ]\xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}[\alpha , 2\pi +\alpha ]\). Further, we have
If the equality hold in (5.2) for every \(t\in [1,R]\), then \(\rho (te^{i\theta }) =\rho (t)\).
Proof of Proposition 5.1
First of all, for fixed t, \(\gamma (\theta )=e^{i\Theta (t e^{i\theta })}\) is a surjection of \([0,2\pi ]\) onto \(\mathbb {T}=\{z:|z|=1\}\). Further
So
The equality is attained in (5.3) if and only if \(\Theta _t\equiv 0\). In this case \(\gamma (\theta )=e^{i\varphi (\theta )}\), for a smooth function of \(\varphi :[0,2\pi ] \xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}[\alpha ,2\pi +\alpha ]\).
We obtain that
with an equality if and only if \(\Theta (se^{i\theta })\) does not depend on t. Thus the first statement of the proposition is proved.
Similarly the function \(\alpha (t)=\log \rho (t e^{i\theta })\) is a surjection of [1, r] onto \([0,\log R]\) and hence
The equality statement can be proved in the same way as the former part. We only need to use the formula
\(\square \)
Proof of Theorem 2.2
Assume as before that \(h(z)=\rho (z)e^{i\Theta (z)}\) is a mapping from the annulus \(\mathbb {A}\) onto the annulus \(\mathbb {A}^{*}\). We start from the following inequality which follows from Hölder inequality
In view of (2.1)
where \(\rho (z)=|h(z)|\). And thus
Then by (3.10), for \(q=1\) we have
From (5.4) we get
Let
Then
Thus we again use (3.16) to conclude that \(K(t)=c(r,R)\). Furthermore
Now by Proposition 5.1 we have
and
So we have
Thus
The uniqueness part of this theorem follows from Proposition 5.1. The equation in (5.4) is satisfied if and only if
is a function that depends only on t. Since \(\Theta (\theta )=e^{i\varphi (\theta )}\), we get \(|\nabla \Theta (\theta )|=\varphi '(\theta )=\textrm{const}\). Because \(\varphi :[0,2\pi ]\xrightarrow []{{}_{\!\!\text {onto\,\,}\!\!}}[\alpha , 2\pi +\alpha ]\), it follows that \(\varphi (\theta )=\theta +\alpha \). In other words h(z) is a minimizer if and only if \(h(z) = H_\circ (t)e^{i(\theta +\alpha )}=e^{i\alpha } h_\circ (z)\). This finishes the proof. \(\square \)
Proof of Theorem 2.3
The proof of Theorem 2.3 is the same as the proof of Theorem 2.2 up to the part concerning the existence of the radial solutions given in Sect. 4 (See Lemma 4.1). \(\square \)
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Kalaj, D. Radial symmetry of minimizers to the weighted p-Dirichlet energy. Monatsh Math 204, 903–918 (2024). https://doi.org/10.1007/s00605-024-01986-8
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DOI: https://doi.org/10.1007/s00605-024-01986-8