A density argument in the proof of Hardy's inequality for $H^1(\mathbb R^3)$

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I understand $C^{\infty}_0 (\mathbb{R}^3)$ is dense in $H^1 (\mathbb{R}^3)$.

But I don't understand the reason it is enough to prove the following Hardy inequality if you prove the case $u \in C^{\infty}_0$.

(Hardy inequality) Let$ \ u \in H^1 (\mathbb{R}^3)$. Then, $$\int_{\mathbb{R}^3} \frac{|u(x)|^2}{|x|^2} dx \leq 4\int_{\mathbb{R}^3} |\nabla u(x)|^2 dx$$

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The reason is that both sides of the inequality are continuous with respect to the $H^1$ norm. When you have two continuous function $f,g$ on some space, and $f\le g$ holds on a dense subset, then it follows that $f\le g$ everywhere.

The continuity of $u\mapsto \int_{\mathbb{R}^3} |\nabla u(x)|^2 dx$ is immediate from the definition of $H^1$ norm.

Let $B$ be the unit ball of $\mathbb{R}^3$. The continuity of $u\mapsto \int_{\mathbb{R}^3\setminus B} \frac{|u(x)|^2}{|x|^2} dx$ also follows quickly, since $1/|x|^2$ is bounded on $\mathbb{R}^3\setminus B$.

To deal with $u\mapsto \int_{B} \frac{|u(x)|^2}{|x|^2} dx$, we need the Sobolev inequality: $H^1(B)$ embeds into $L^6(B)$, therefore $|u|^2\in L^3(B)$. The function $x\mapsto 1/|x|^2$ belongs to $L^{4/3}(B)$, and therefore defines a continuous functional on $L^3(B)$ (Hölder's inequality). The conclusion follows.

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Let $B_r$ be the ball with radius $r$. If $u_n\in C_0^{\infty}$ is an approximation of $u$ in $H^1(\mathbb{R}^3)$, we have \begin{align} \left|\left\lVert \frac{u_n}{|x|}\right\rVert_{L^2(\mathbb{R}^3\setminus B_r)} -\left\lVert \frac{u}{|x|}\right\rVert_{L^2(\mathbb{R}^3\setminus B_r)}\right| &\le \left\lVert \frac{u_n-u}{|x|}\right\rVert_{L^2(\mathbb{R}^3\setminus B_r)} \le \frac{\lVert u_n-u\rVert_{L^2(\mathbb{R}^3\setminus B_r)}}{r}\\ &\le \frac{\lVert u_n-u\rVert_{L^2(\mathbb{R}^3)}}{r}\to 0. \end{align} Since we have \begin{equation} \left\lVert \frac{u_n}{|x|}\right\rVert_{L^2(\mathbb{R}^3\setminus B_r)} \le \left\lVert \frac{u_n}{|x|}\right\rVert_{L^2(\mathbb{R}^3)} \le 2\lVert \nabla{u_n}\rVert_{L^2(\mathbb{R}^3)}, \end{equation} we get \begin{equation} \left\lVert \frac{u}{|x|}\right\rVert_{L^2(\mathbb{R}^3\setminus B_r)} \le 2\lVert \nabla{u}\rVert_{L^2(\mathbb{R}^3)} \end{equation} as $n\to\infty$. Taking limit $r\to 0$ we complete the proof. Sobolev inequality is not necessary.