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A continuous traction field balanced on every piecewise C1 region is given by a continuous stress matrix, and t(−n)=−t(n)

Statement

Assume ACω where the surface and divergence machinery of the cited items assumes it. Let O⊆R3 be open, let t:O×S2→R3 be continuous, where S2={n∈R3:∥n∥2=1} is the unit sphere, and let g:O→R3 be continuous and bounded, with Cg:=sup⁡O∥g∥2<+∞. Suppose that for every bounded piecewise C1 Euclidean domain D with a specified finite presentation (Specified finite piecewise C1 boundary presentations) whose closure lies in O and whose associated pieces lie in O,

∫∂Dt(y,νD(y)) dS(y)+∫Dg(y) dy=0,(B)

where νD is the actual outward unit normal off the edge set of the presentation, the boundary term is the sum of the surface integrals over the specified faces (Surface integration on compact C1 hypersurfaces), and values of the normal on the edge set are irrelevant.

Then there is a unique continuous map

σ:O⟶M3(R)

with

t(y,n)=σ(y)nfor every (y,n)∈O×S2,

the product being matrix-vector multiplication (The vector space Mm×n(F):=F m×n of m by n matrices over a field, with entrywise operations, Rectangular matrix multiplication and the identity matrix In, including zero-sized shapes). Explicitly, the columns of σ(y) are the vectors t(y,e1),t(y,e2),t(y,e3); and necessarily

t(y,−n)=−t(y,n)for every (y,n)∈O×S2.

Facts & Assumptions

Given: The open set O, the continuous traction field t, the bounded continuous field g, and the balance hypothesis (B).

[F1]

A bounded piecewise C1 domain is a nonempty bounded open set with compact faces covering its boundary, a compact edge set of surface measure zero on each face, and, off the edges, a local C1 graph description with the domain on one side; the boundary integral is the sum of the face surface integrals with the actual outward normals (Specified finite piecewise C1 boundary presentations, Surface integration on compact C1 hypersurfaces). Boxes and tetrahedra with closures in O and vertices in general position are examples: their faces are compact planar triangles or rectangles, their edges form a compact set meeting each face in a segment of zero surface measure, and off the edges the boundary is locally a plane. The cube and tetrahedron constructions below therefore fall under (B).

[F2]

For a continuous h on a compact set K and a compact surface piece F contained in K with finite area S(F)>0, the face average satisfies

∣1S(F)∫Fh dS−h(y0)∣≤sup⁡y∈F∥h(y)−h(y0)∥2.

Indeed the definition of the surface integral and the order rules for the nonnegative Lebesgue integral bound ∫F∥h−h(y0)∥2 dS by the supremum times S(F), and the signed integral obeys the triangle inequality (Surface integration on compact C1 hypersurfaces, Monotonicity and nonnegative homogeneity of the nonnegative integral, The Lebesgue integral is linear on L1(μ)). If moreover all points of F are within distance ρ of y0, then by uniform continuity of h on a compact neighbourhood of y0 the right-hand side tends to 0 as ρ→0 (Heine-Cantor: a continuous map from a compact metric space to any metric space is uniformly continuous, Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line).

[F3]

(Geometry of the two test bodies.) Fix an orthonormal basis (n,p,q) of R3 and h>0.

  1. The thin box Dh:=y0+{an+bp+cq: ∣a∣<h2, ∣b∣<h, ∣c∣<h} has two faces of area 4h2 with outward normals ±n and four lateral faces of area 4h3 with outward normals ±p,±q; its volume is 8h4. These areas are the products of the corresponding side lengths 2h2,2h,2h.
  2. Let n∈S2 have no zero component, define si:=1 when ni>0 and si:=−1 when ni<0, and put Pi:=y0+(h/ni)ei, and let Th be the open tetrahedron with vertices y0,P1,P2,P3. Equivalently, in coordinates v=y−y0 it is given by sivi>0 and n⋅v<h. Its coordinate face Fi has outward normal −siei and area A∣ni∣, where A:=h2/(2∣n1n2n3∣); its oblique face F0 has outward normal n and area A. Indeed the coordinate-face normal points out of sivi>0, and the oblique-face normal points out of n⋅v<h. The volume is Ah/3. The reflection vi↦sivi is an isometry taking this tetrahedron to the positive-coordinate tetrahedron with intercepts h/∣ni∣, so its face areas are unchanged. Alternatively the cross-product formula for triangle area gives 12∥(P2−P1)×(P3−P1)∥2=h2/(2∣n1n2n3∣), since ∑ini2=1 (The cross product is bilinear, alternating, and orthogonal to both factors, The squared cross-product norm is the Gram determinant of two vectors). The face opposite Pi is a right triangle with legs h/∣nj∣,h/∣nk∣, and the volume is one third of the oblique-face area times its distance h from y0.
[F4]

The columns of a matrix σ∈M3(R) determine it, and (σn)k=∑iσkini. A map into M3(R) is continuous if and only if its three columns are continuous.

Proof

technique · direct; shrink a box and a right tetrahedron about an arbitrary point and pass to the limit in the balance (B)
2.1givenF1F2F3step 1.1algebra

(Reversed normals.) Fix n∈S2 and extend it to an orthonormal basis (n,p,q). For 0<h<min⁡{1,r/3} use the thin box of F3, whose closure lies in B(y0,r). Its two large-face averages t‾n± satisfy t‾n±→t(y0,±n) by [F2], since each face lies within distance h4+2h2≤3h of y0. The four lateral-face contributions have total norm at most 16Cth3, and ∥∫Dhg dy∥2≤8Cgh4. Thus (B), divided by 4h2, gives ∥t‾n++t‾n−∥2≤4Cth+2Cgh2. Letting h↓0 yields t(y0,n)+t(y0,−n)=0.(R)

3.1givenF1F2F3step 1.1step 2.1algebra

(Signed tetrahedron identity.) Fix n∈S2 with ni≠0 for all i and put si=1 if ni>0 and si=−1 if ni<0. For 0<h<rmin⁡i∣ni∣/2 the signed tetrahedron of F3 has closure in O. Divide its balance (B) by the oblique-face area A. The coordinate-face area ratios are ∣ni∣, their actual outward normals are −siei, and the volume ratio is h/3. All face points tend to y0 as h↓0, so [F2] and the bound ∥∫Thg∥2/A≤Cgh/3 give t(y0,n)+∑i=13∣ni∣t(y0,−siei)=0. By (R), t(y0,−siei)=−sit(y0,ei) for either sign of si. Since ∣ni∣si=ni, this is t(y0,n)=∑i=13nit(y0,ei).(T)

4.1step 3.1givenalgebra

(Zero components.) Let n∈S2 be arbitrary. For ε>0 put vε,i:=ni when ni≠0 and vε,i:=ε when ni=0, and set nε=vε/∥vε∥2. Every component of nε is nonzero, its nonzero original components retain their signs, and nε→n. Apply (T) from step 3.1 to nε. Continuity of t(y0,⋅) and of the finite linear combination ∑init(y0,ei) then gives (T) for n, including all normals with zero components.

5.1F4step 4.1constructalgebra

(Matrix representation and uniqueness.) Define σ(y0)∈M3(R) by σ(y0)ei:=t(y0,ei). Then for every n∈S2, (T) reads t(y0,n)=∑ini t(y0,ei)=σ(y0)n. Since y0∈O was arbitrary, this defines σ:O→M3(R). If σ1,σ2 both represent t, then (σ1−σ2)ei=0 for i=1,2,3 and the columns determine the matrix, so σ1=σ2: the representation is unique.

6.1step 5.1F4given∎

(Continuity.) Each column map y↦σ(y)ei=t(y,ei) is continuous on O because t is; hence each entry y↦σki(y) is continuous, and σ is continuous as a map into M3(R) (finite-dimensional, entrywise continuity). This proves the existence, uniqueness and continuity clauses.

Remarks

  • The mathematical content is conditional: the conclusion is that the assumed balance (B) for all piecewise C1 test regions forces the contact interaction to be linear in the normal and to satisfy the reversed-normal rule. It is not a derivation of (B) itself, which is an adopted contact-balance hypothesis in any continuum model.

  • The hypothesis that (B) holds for boxes and tetrahedra is used only through the two test families; simultaneously the surface integral over the four lateral faces is controlled by the boundedness of t on the compact neighbourhood. No symmetry of σ is asserted here: linearity in n alone does not make σ symmetric, and the separate angular-momentum balance is needed for that.

  • A body couple density or surface couple field contributes to angular-momentum balance; its presence alone does not invalidate the pure-force balance (B). Whenever (B) retains the stated test-region hypotheses, the thin-box argument still forces the reversed-normal traction rule. This theorem makes no claim about additional couple tractions or their representation.

Depends on

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