I am working on something using this equation, and I find something strange. I am manipulating $\ell$ here between $0$ and $1$. I note that as $\ell$ approaches zero ($\sim0.001$ or less) it becomes a graph of $y=c\frac{1}{x}$. I cannot understand why, or how $c$ would be calculated as a simplification/approximation of the equivalent full formula at this point.
The full equation is: $$y = \frac{2A\sin(x\pi \ell)}{\pi^2 \ell (1-\ell) x^2}$$
As you can see as $\ell$ is close to $0$, this becomes equivalent to $y=c\frac{1}{x}$:
However, I don't know how this is happening, or what $c$ value would then reliably approximate the full equation at a certain value of $A$ (I just matched the curves visually here with an arbitrary constant).
Any help understanding the simplification and thus how $c$ could be calculated in terms of $A$ to roughly match in these circumstances?

Recall $\sin t \approx t$ for $t$ near $0$, so your equation can be approximated by $$y = \frac{2A\sin(x\pi l)}{\pi^2 l (1-l) x^2} $$ $$\approx \frac{2Ax\pi l}{\pi^2 l (1-l) x^2}$$ $$=\frac{2A}{\pi (1-l) x}$$ $$\approx \frac{2A}{\pi}\cdot \frac1x$$ (this last approximation because $1-l\approx 1$)