Abstract
We exhibit a family of convex functionals with infinitely many equal-energy C^1 stationary points that (i) occur in pairs v_{pm } satisfying det nabla v_{pm }=1 on the unit ball B in {mathbb {R}}^2 and (ii) obey the boundary condition v_{pm }=text {id} on partial B. When the parameter epsilon upon which the family of functionals depends exceeds sqrt{2}, the stationary points appear to ‘buckle’ near the centre of B and their energies increase monotonically with the amount of buckling to which B is subjected. We also find Lagrange multipliers associated with the maps v_{pm }(x) and prove that they are proportional to (epsilon -1/epsilon )ln |x| as x rightarrow 0 in B. The lowest-energy pairs v_{pm } are energy minimizers within the class of twist maps (see Taheri in Topol Methods Nonlinear Anal 33(1):179–204, 2009 or Sivaloganathan and Spector in Arch Ration Mech Anal 196:363–394, 2010), which, for each 0le rle 1, take the circle {xin B: |x|=r} to itself; a fortiori, all v_{pm } are stationary in the class of W^{1,2}(B;{mathbb {R}}^2) maps w obeying w=text {id} on partial B and det nabla w=1 in B.
Highlights
Let > 1 be a real parameter, let x = x/|x| for any non-zero x in R2 and let B be the unit ball in R2
We prove that A contains stationary points of D which occur in pairs, v±, say, such that (a) D (v+) = D (v−) and (b) v+ and v−
It is perhaps striking that, in the pure displacement problem we consider, the maps v± appear to emulate the buckling beam examples frequently cited as examples of non-uniqueness of equilibria in nonlinear elasticity when mixed boundary conditions are applied1
Summary
Let > 1 be a real parameter, let x = x/|x| for any non-zero x in R2 and let B be the unit ball in R2. We study the functional D given by. Our goal is to find a global minimizer of D in A. and our goal is to find a global minimizer of D in A In this direction, we prove that A contains stationary points of D which occur in pairs, v±, say, such that (a) D (v+) = D (v−) and (b) v+ and v−
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