Without loss of generality, the three points on the unit circle are $1,e^{is},e^{it}$, where $s$ and $t$ are uniformly and independently distributed on the interval $[0,2\pi]$, so that $a=|e^{is}-1|$, $b=|e^{it}-1|$, $c=|e^{is}-e^{it}|$.
Then the condition $ab>c$ can be rewritten as
$$|u|<h(v):=\cos^{-1}g(v) \tag{10}\label{10}$$
for
$$(u,v):=\Big(\frac{s-t}2,\frac{s+t}2\Big)\in[-\pi/2,\pi/2]\times[0,2\pi],$$
where
$$g(v):=\frac{\cos v+\sqrt{2-\cos^2 v}}2;$$
see details on \eqref{10} at the end of this answer.
Here is the set of all pairs $(v,u)\in[0,2\pi]\times[-\pi/2,\pi/2]$ satisfying condition \eqref{10}:
Note the symmetries
$$h(2\pi-v)=h(v)\quad\text{and especially}\quad h(v)+h(\pi-v)=\pi/2;\tag{20}\label{20}$$
see details on this at the end of the answer.
Also, the Jacobian $J:=\frac{\partial(s,t)}{\partial(u,v)}$ is $2$.
The probability (say $p$) in question is $\dfrac A{(2\pi)^2}$, where $A$ is the area of the set of all $(s,t)\in[0,2\pi]^2$ satisfying the condition $ab>c$, so that
$$A=2\times2\int_0^{2\pi}dv\,h(v)
=8\int_0^\pi dv\,h(v)=8\int_0^\pi dv\,h(\pi-v) \\
=8\times\frac12 \int_0^\pi dv\,[h(v)+h(\pi-v)]
=8\times\frac12 \,\pi\times\pi/2=2\pi^2. $$
(This result is "obvious" from the above picture, because $A$ is $J$ times the depicted area (that is, twice the depicted area), whereas the depicted area is half of the area $2\pi\times\pi$ of the rectangle enclosing the depicted area.)
So, $p=\dfrac{2\pi^2}{(2\pi)^2}=\dfrac12$. $\quad\Box$
Details on \eqref{10}: Note that $a^2=(e^{is}-1)(e^{-is}-1)=2(1-\cos s)$. Similarly, $b^2=2(1-\cos t)$ and $c^2=(e^{i(s-t)}-1)(e^{-i(s-t)}-1)=2(1-\cos(s-t))$. So, $ab>c$ can be rewritten as
$2(1-\cos s)(1-\cos t)>1-\cos(s-t)$ or as $2(1-(\cos s+\cos t)+\cos s\,\cos t)>1-\cos(s-t)$. Now use the identities $\cos s+\cos t=2\cos u\cos v$ and $2\cos s\,\cos t=\cos2u+\cos2v$, $\cos 2x=2\cos^2x-1$, and $s-t=2u$ to rewrite $ab>c$ as $\cos u\ge g(v)$, which is equivalent to \eqref{10}, because $0\le g\le1$.
Details on the identity $h(v)+h(\pi-v)=\pi/2$ in \eqref{20}: Since $0\le g\le1$, \eqref{10} implies $0\le h\le\pi/2$. So,
for
$$f(v):=g(\pi-v)=\frac{-\cos v+\sqrt{2-\cos^2 v}}2$$
we have
$$0\le\cos(\pi/2-h(\pi-v))=\sin(h(\pi-v)) \\
=\sin(\cos^{-1} f(v))
=\sqrt{1-f(v)^2}=g(v)=\cos h(v). $$
Using again the fact that $0\le h\le\pi/2$, we get $\pi/2-h(\pi-v)=h(v)$, as desired.
Responding to the comment that "$\sqrt{1-f(v)^2}=g(v)$ is true but not obviously true", here is a symmetry proof of that: Letting $y:=\cos v$, $x_+:=g(v)=\frac{y+\sqrt{2-y^2}}2$, and $x_-:=f(v)=\frac{-y+\sqrt{2-y^2}}2$, we have $x_+ +x_-=\sqrt{2-y^2}$ and $2x_+ x_-=1-y^2$, so that
$g(v)^2+f(v)^2=x_+^2+x_-^2=(x_+ +x_-)^2-2x_+ x_-=(2-y^2)-(1-y^2)=1$. Therefore and because $g(v)\ge0$, we get $\sqrt{1-f(v)^2}=g(v)$.