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In Exercises 27 and 28 , prove the identity, assuming that \(Q, S,\) and \(\mathrm{N}\) meet the conditions of the Divergence Theorem and that the required partial derivatives of the scalar functions \(f\) and \(g\) are continuous. The expressions \(D_{\mathrm{N}} f\) and \(D_{\mathrm{N}} g\) are the derivatives in the direction of the vector \(\mathrm{N}\) and are defined by $$ D_{\mathrm{N}} f=\nabla f \cdot \mathrm{N}, \quad D_{\mathrm{N}} g=\nabla g \cdot \mathrm{N} $$ $$ \begin{array}{l} \iiint_{Q}\left(f \nabla^{2} g+\nabla f \cdot \nabla g\right) d V=\iint_{S} \int f D_{\mathrm{N}} g d S \\ {[\text { Hint: } \text { Use } \operatorname{div}(f \mathbf{G})=f \mathrm{div} \mathbf{G}+\nabla f \cdot \mathbf{G} .]} \end{array} $$

Short Answer

Expert verified
The identity holds true by applying the Divergence Theorem and using the properties of gradients and divergences.

Step by step solution

01

Define fG

Define \( \mathbf{G}=g \mathbf{N} \). We have \( \nabla \cdot(f \mathbf{G})=f \nabla \cdot \mathbf{G}+\nabla f \cdot \mathbf{G} \).
02

Evaluate the Left Hand Side (LHS)

Evaluate the Left Hand Side (LHS) of the equation, \( \iiint_{Q}\left(f \nabla^{2} g+\nabla f \cdot \nabla g\right) d V \) using the definition of \( \mathbf{G} \). We get \( LHS = \iiint_{Q} \nabla \cdot(f \mathbf{G}) dV \).
03

Apply the Divergence Theorem

Use the Divergence Theorem on LHS which states that for a vector field \( \mathbf{G} \), \( \iiint_{Q} \nabla \cdot \mathbf{G} dV = \iint_{S} \mathbf{G} \cdot d\mathbf{S} \). We get \( LHS = \iint_{S} (f \mathbf{G}) \cdot d\mathbf{S} \).
04

Equation transformation

Transform this equation by substituting \(\mathbf{G} = g \mathbf{N}\) and using the fact that \(\mathbf{N} \cdot d \mathbf{S} = dS\). Thus, we get \(LHS = \iint_{S} f g dS = \iint_{S} f D_{N} g dS\).
05

Result Confirmation

We see that the result obtained in the above step matches the Right Hand Side (RHS) of the original equation. That concludes the proof of the identity.

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