Let $f\in C^1$ and $g\in C^2$ be scalar functions. How do I prove the identity
$$\operatorname{div} (f \nabla g) = f\Delta g + \nabla f \cdot\nabla g$$
?
Let $f\in C^1$ and $g\in C^2$ be scalar functions. How do I prove the identity
$$\operatorname{div} (f \nabla g) = f\Delta g + \nabla f \cdot\nabla g$$
?
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It's all just a matter of plugging things into the definitions. Recall the following definitions:
$$\operatorname{div}(F)=\sum_{j=1}^n\partial_jF_j,$$
$$\nabla G=(\partial_1 G,\dots,\partial_n G),$$
$$\Delta G=\sum_{j=1}^n\partial_j^2G,$$
$$\langle x,y \rangle = \sum_{j=1}^n x_jy_j.$$
The left hand side then becomes
$$\operatorname{div}(f\cdot\nabla g)=\operatorname{div}(f\cdot\partial_1g,\dots,f\cdot\partial_ng)=\sum_{j=1}^n\partial_j(f\cdot\partial_jg)=\sum_{j=1}^n\bigl(\partial_jf\cdot\partial_jg+f\cdot\partial_j^2g\bigr).$$
One the other hand we can compute the right hand side as
$$f\cdot\Delta g+\langle \nabla f,\nabla g\rangle=\sum_{j=1}^nf\cdot\partial_j^2g+\sum_{j=1}^n\partial_jf\cdot\partial_jg=\sum_{j=1}^n\bigl(\partial_jf\cdot\partial_jg+f\cdot\partial_j^2g\bigr).$$
Now both computations gave us the same thing, and so $\operatorname{div}(f\cdot\nabla g)=f\cdot\Delta g+\langle \nabla f,\nabla g\rangle$, as was desired.