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EQUATIONS OF ELASTIC HYPERSURFACES

EQUATIONS OF ELASTIC HYPERSURFACES

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44 SHELLS<br />

Definition 2.49 Let { S , β S<br />

}<br />

be a smooth hypersurface with a boundary Γ = ∂M , oriented<br />

by the non-vanishing differential form of maximal order β S ∈ Λ n−1 (S ).<br />

The natural orientation of the boundary Γ is then specified by the restriction β Γ = β S<br />

∣<br />

∣Γ<br />

which is a form of maximal order β Γ ∈ Λ n−2 (Γ).<br />

The next Lemma 2.50 provides an useful and interesting example of restriction of the<br />

differential form to hypersurface and to it’s boundary.<br />

Lemma 2.50 Let Θ : Ω → S be a smooth hypersurface in R n with a smooth boundary<br />

Γ := ∂S , while dS and ds designate the respective volume elements on S and on Γ.<br />

Let ν(X ) = ( ν 1 (X ), . . . , ν n (X ) ) ⊤<br />

be the outer unit normal vector to S at X ∈ S and<br />

ν Γ (s) = ( ν 1 Γ (s), . . . , νn Γ (s)) ⊤<br />

-the unit tangential vector to S at the boundary point s ∈ Γ,<br />

which is outward (unit) normal vector to the boundary S . Then<br />

∣<br />

ν j dS = β ∣S j , (2.174)<br />

[<br />

νj νΓ k − ν ] ∣<br />

kν j Γ ds = βjk∣Γ , (2.175)<br />

where<br />

β j := ∣ ∣ dx1 ∧ . . . ∧ ̂dx j ∧ . . . ∧ dx n<br />

∣ ∣ = (−1) j−1 dx 1 ∧ . . . ∧ ̂dx j ∧ . . . ∧ dx n ,<br />

β jk := ∣ ∣dx 1 ∧ . . . ∧ ̂dx j ∧ . . . ∧ ̂dx k ∧ . . . ∧ dx n<br />

∣ ∣<br />

= (−1) j+k−1 dx 1 ∧ . . . ∧ ̂dx j ∧ . . . ∧ ̂dx k ∧ . . . ∧ dx n<br />

and the “hat” symbol indicates omission.<br />

Proof: According to Lemma 2.29 the differential form β j generates the volume element<br />

of the hyperplane x j = const in R n . On the other hand, being a positive ∣ (n − 1)-form,<br />

the restriction to the surface S is a maximal form and, due to (2.140), β ∣S j = g j dS for<br />

some function g j (X ). To find the function g j (X<br />

∣ ) it suffices to consider the restriction to the<br />

hyperplane β ∣xk j = β =const j, where it defines the volume element. The projection of the<br />

volume element dS of S to the hyperplane x j = const is ν j dS = cos θ j dS and, therefore,<br />

g j (X ) ≡ ν j (X ).<br />

∣<br />

By applying the above argument on projection to the (n − 2)-form β ∣Γ jk = g jk ds which<br />

is maximal on Γ, we get similarly g jk = ν j νΓ k − ν kν j Γ<br />

and formula (2.175) follows.<br />

Theorem 2.51 Let β be a compactly supported (n − 2)-form with coefficients in the class<br />

C 1 on an oriented n-dimensional 2-smooth manifold S with boundary Γ oriented naturally.<br />

The following Stoke’s formula is valid:<br />

∫ ∫<br />

dβ := β . (2.176)<br />

S<br />

Γ

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