Consider the following set of Bessel functions
$$\{J_1(\alpha_ir)\}, \qquad J_0(\alpha_ia)=0 \tag{1}$$
I want to show that this set of functions form a basis for the space of $C^{1}[0,a]$ functions. So I should prove that
They are linearly independent and that they span the space so they form a basis for that space.
My Work
My first thought was to find the corresponding Sturm-Liouville problem for this set of functions. However, I failed to find proper boundary conditions. For example, the following Sturm-Liouville system
\begin{align} \,&\frac{d}{dr}\left[r\frac{dR}{dr}\right]+\left[\lambda r + \frac{1}{r}\right]R=0\\ &R(0)<\infty\\ &R(a)=0 \tag{2} \end{align} leads to the following basis $$\{J_1(\alpha_ir)\}, \qquad J_1(\alpha_ia)=0 \tag{3}$$ for the aforementioned space (note the order of the Bessel functions).
Anyway, I could show that the set of functions mentioned in Eq.$(1)$ are orthogonal and consequently linearly independent by just computing the following integral
$$\int_{0}^{a} r J_1(\alpha r) J_1(\beta r)dr = \frac{a}{\alpha^2-\beta^2}\Big(\beta J_0(\beta a)J_1(\alpha a)- \alpha J_0(\alpha a)J_1(\beta a)\Big)$$

Finally, I figured out that my first idea will work. The Sturm-Liouville system
\begin{align} \,&\frac{d}{dr}\left[r\frac{dR}{dr}\right]+\left[\lambda r + \frac{1}{r}\right]R=0\\ &R(0)<\infty\\ &a\frac{dR}{dr}(a)+R(a)=0 \tag{1} \end{align}
will lead to the eigen-functions
$$\{J_1(\alpha_ir)\}, \qquad J_0(\alpha_ia)=0 \tag{2}$$
I leave the proof as an exercise for the interested reader and just mention a key Hint to crack the problem.
$$\frac{dJ_1(\alpha r)}{dr}=\alpha J_0(\alpha r) -\frac{1}{r}J_1(\alpha r) \tag{3}$$