Remark:
- Here is the usual condition. cf. also "Mathematics for Physics and Physicists" (2007), Walter Appel, the notion of Dirac sequence, Thm 8.18 p.232 (proved p.601) and proposition 8.21 p.233.
- I checked several books (ex. Real and Functional Analysis by Serge Lang), and a Dirac sequence is required to be positive but this is in fact not necessary for (weak) converge to the delta distribution. However, without positivity, one must impose finiteness of $\lVert f\rVert_1 =\int_{\mathbb{R}^n} \lvert f(x) \rvert \, dx < +\infty$
With the assumptions of the OP and $\lVert f\rVert_1 =C < +\infty$: we want to show that for any test function $\varphi\in \mathcal{C}^{\infty}_c(\mathbb{R}^n) $
$$ \lim_{k\to\infty} \langle f_k, \varphi\rangle :=\lim_{k\to\infty} \int_{\mathbb{R}^n} f_k(x)\, \varphi(x)\, dx = \varphi(0)$$
Indeed we do a change of variable:
$$\int_{\mathbb{R}^n} f_k(x)\, \varphi(x)\, dx := \int_{\mathbb{R}^n} k^n f(kx)\, \varphi(x)\, = \begin{bmatrix} y = kx \\ dy = k^n dx\end{bmatrix} = \int_{\mathbb{R}^n} f(y)\, \varphi(y/k)\, dy$$
By continuity of $\varphi$ at $0$:
$$ \forall\ \epsilon > 0,\ \exists\ \delta > 0,\enspace\forall\ u\in \mathcal{B}(0,\delta),\ \big\lvert \varphi(u) -\varphi(0)\big\rvert < \epsilon$$
For $k$ large enough, $y/k$ is in the ball $\mathcal{B}(0,\delta)$ if $y\in \mathcal{B}(0,1)$ and since $f$ has support in the unit ball, one needs only integrates on it. Let us now write what we wanted to prove:
$$ \left\lvert \int_{\mathbb{R}^n} f(y)\, \varphi(y/k)\, dy -\varphi(0) \right\rvert= \left\lvert\int_{\mathcal{B}(0,1)} f(y)\, \varphi(y/k)\, dy - \varphi(0) \int_{\mathcal{B}(0,1)} f(y)\, dy \right\rvert$$
$$ \leq \left\lvert\int_{\mathcal{B}(0,1)} f(y)\, \Big( \varphi(y/k) -\varphi(0)\Big)\, dy \right\rvert \leq \int_{\mathcal{B}(0,1)} \left\lvert f(y)\, \Big( \varphi(y/k) -\varphi(0)\Big) \right\rvert\, dy
$$
$$\leq \epsilon \int_{\mathcal{B}(0,1)} \lvert f(y) \rvert \, dy = \epsilon C \tag{*}\label{*}$$
One thus concludes that
$$ \lim_{k\to\infty} \langle f_k, \varphi\rangle = \varphi(0)= \langle \delta ,\varphi \rangle$$
Remark: If one had positivity of $f$ then the absolute value is unecessary in (*), and that integral was supposed to be equal to 1, (hence bounded).