If $\vec{u} = \vec{r}/r$, find $\mathrm{div} ~(\nabla \vec{u})$.
Please help me to solve this problem.
If $\vec{u} = \vec{r}/r$, find $\mathrm{div} ~(\nabla \vec{u})$.
Please help me to solve this problem.
On
$\newcommand{\angles}[1]{\left\langle\,{#1}\,\right\rangle} \newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace} \newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack} \newcommand{\dd}{\mathrm{d}} \newcommand{\ds}[1]{\displaystyle{#1}} \newcommand{\expo}[1]{\,\mathrm{e}^{#1}\,} \newcommand{\half}{{1 \over 2}} \newcommand{\ic}{\mathrm{i}} \newcommand{\iff}{\Longleftrightarrow} \newcommand{\imp}{\Longrightarrow} \newcommand{\Li}[1]{\,\mathrm{Li}_{#1}} \newcommand{\ol}[1]{\overline{#1}} \newcommand{\pars}[1]{\left(\,{#1}\,\right)} \newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}} \newcommand{\ul}[1]{\underline{#1}} \newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,} \newcommand{\totald}[3][]{\frac{\mathrm{d}^{#1} #2}{\mathrm{d} #3^{#1}}} \newcommand{\verts}[1]{\left\vert\,{#1}\,\right\vert}$
$\ds{\,\mathrm{div}\pars{\nabla\pars{\vec{r} \over r}} = \nabla^{2}\pars{\vec{r} \over r}}$. You can use the identity:
$\ds{\nabla^{2}\pars{ab} = \pars{\nabla^{2}a}b + 2\pars{\nabla a}\cdot\pars{\nabla b} + a\nabla^{2}b}$ which is a ' sort of Newton Binomial '.
\begin{align} \color{#f00}{\nabla^{2}\pars{x \over r}} & = \nabla^{2}\pars{x\,{1 \over r}}= \pars{\nabla^{2}x}\,{1 \over r} + 2\pars{\nabla x}\cdot\nabla\pars{1 \over r} + x\,\nabla^{2}\pars{1 \over r} \\[4mm] & = 0 \times {1 \over r} + 2\,\hat{x}\cdot\pars{-\,{1 \over r^{2}}\,{\vec{r} \over r}} + x\bracks{-4\pi\delta\pars{\vec{r}}} = \color{#f00}{-\,{2x \over r^{3}}} \end{align}
Note that $\ds{\nabla\,\mathrm{f}\pars{r} = \,\mathrm{f}\,'\pars{r}\,{\vec{r} \over r}}$.
Note that we have
$$\nabla \vec u=\hat x_i\hat x_j\partial_i (u_j) \tag 1$$
Taking the divergence of $(1)$ yields
$$\begin{align} \nabla \cdot \left(\nabla \vec u\right)&=\partial_i\left(\hat x_j\partial_i(u_j)\right)\\\\ &=\nabla^2\vec u\\\\ &=\nabla \nabla \cdot \vec u-\nabla \times \nabla \times \vec u \end{align}$$
Then, we have for $r\ne 0$
$$\nabla \times \left(\frac{\vec r}{r}\right)=0$$
and
$$\nabla \cdot \left(\frac{\vec r}{r}\right)=\frac{2}{r}$$
so that
$$\nabla^2 \left(\frac{\vec r}{r}\right)=-2\frac{\vec r}{r^3}$$