Let $E:y^2=x^3+ax+b$ be a real elliptic curve such that $0=x^3+ax+b$ has $3$ distinct real roots $w_0<w_1<w_2$ so that $x^3+ax+b=(x-w_0)(x-w_1)(x-w_2)$ and thus $w_0+w_1+w_2=0$. My question then is
Can we express the area $\text{Ar}(E):=2\int_{w_0}^{w_1}\sqrt{x^3+ax+b}\ dx$ in terms of already know special functions?
I have obtained the following infinite series that converges whenever $w_1<0$ $$\boxed{\text{Ar}(E)=\frac{\pi}{2}\sqrt{w_2-w_1}(w_1-w_0)^2\sum_{n=0}^\infty\frac{(-1)^{n+1}(2n+1)}{2n^3+5n^2+n-2}{2n\choose n}^2\frac{1}{16^n}\left(\frac{w_1-w_0}{w_2-w_1}\right)^n}$$ but I haven't been able to link it to other already known special functions. So for example, if we consider the elliptic curve $E_0:y^2=x^3-13x-12=(x+3)(x+1)(x-4)$, we have $$\text{Ar}(E_0)=2\int_{-3}^{-1}\sqrt{x^3-13x-12}dx=2\pi\sqrt{5}\sum_{n=0}^\infty\frac{(-1)^{n+1}(2n+1)}{2n^3+5n^2+n-2}{2n\choose n}^2\frac{1}{40^n}=7.68858977...$$ I think this will be possible via elliptic integrals, but I don't know how exactly. Sorry if this question has already been asked here; I've searched and found nothing.
The affine substitution $u := \frac{x - w_0}{w_1 - w_0}$ transforms the integral into $$(w_1 - w_0)^{5 / 2} \int_0^1 \sqrt{u (u - 1) (u - \lambda)} \,du , $$ where $$\lambda := \frac{w_2 - w_0}{w_1 - w_0} > 1 ,$$ which can be expressed in terms of the complete elliptic integral functions of the First and Second Kinds, $K$ and $E$, respectively: $$\int_0^1 \sqrt{u (u - 1) (u - \lambda)} \,du = \frac{4 \sqrt\lambda}{15} \left[(\lambda^2 - \lambda + 1) E\left(\frac1{\sqrt \lambda}\right) - \left(\lambda - \frac12\right) (\lambda - 1) K\left(\frac1{\sqrt \lambda}\right)\right] .$$ Both $E$ and $K$ are expressible in terms of the Gauss hypergeometric function, ${}_2 F_1$, hence so is the integral: \begin{multline}\int_0^1 \sqrt{u (u - 1) (u - \lambda)} \,du \\ = \frac{\pi \sqrt\lambda}{15} \left[2 (\lambda^2 - \lambda + 1) \cdot {}_2 F_1\left(-\frac12, \frac12; 1; \frac1\lambda\right) - (2 \lambda - 1) (\lambda - 1) \cdot {}_2 F_1\left(\frac12, \frac12; 1; \frac1\lambda\right)\right] .\end{multline}