Prove that the common chord passes through the origin. 
Consider the parabola $x^2=4ay$. Two focal chords are constructed, and
  the interval that the chord makes with the parabola are diameters of
  two circles. 
Prove that that the common chord of the two circles passes through the
  origin (vertex of the parabola). 

I am having trouble finding a purely geometric way of proving this result. 

 A: Consider a parabola with focus $F$ and vertex $V$; define $a := |\overline{VF}|$. Let $\overline{PQ}$ be a focal chord of the parabola, with $M$ its midpoint. Let $F^\prime$, $P^\prime$, $Q^\prime$, $M^\prime$ be the projections of the corresponding points onto the directrix. (Note that $|\overline{VF^\prime}| = a$.)

It is "known" that the tangents (not shown) at the endpoints of a focal chord are perpendicular, and that they meet at the point on the directrix halfway between their own projections. In our scenario, that point must be $M^\prime$, so that the circle with diameter $\overline{PQ}$ is tangent to the directrix at $M$. Let $r := |\overline{MM^\prime}|$ be the radius of that circle.
It is also "known" that the tangents at $P$ and $Q$ bisect respective angles $\angle FPP^\prime$ and $\angle FQQ^\prime$. This implies that $F$ is the common reflection of $P$ over $\overline{PM^\prime}$ and $Q$ over $\overline{QM^\prime}$, so that $\overline{FM^\prime}\perp\overline{PQ}$. Define $m := |\overline{FM^\prime}|$. A little angle chasing shows that $\angle FM^\prime F^\prime \cong \angle FMM^\prime$, so that the similar right triangles yield
$$\frac{2a}{m} = \frac{m}{r} \qquad\to\qquad m^2 = 2 a r \tag{1}$$
This comes in handy for calculating the power of $V$ with respect to the circle:
$$\begin{align}
\text{power of $V$ wrt $\bigcirc{M}$} &:= n^2 - r^2 \\
&\,= n^2 - (r - a)^2 - 2 a r+ a^2 \\
&\,= |\overline{M^\prime F^\prime}|^2 - 2 a r + a^2 \\
&\,= m^2 - (2a)^2 - 2 a r + a^2 \\
&\,= (m^2 - 2 a r) - 3 a^2 \\
&\,= - 3 a^2 \tag{2}
\end{align}$$
We observe that this value is independent of our choice of $P$ and $Q$, and is therefore a constant of this configuration. Consequently, for any two focal-chord-diameter circles, vertex $V$ has the same power with respect to each; this places $V$ on the circles' radical axis, which for intersecting circles is the line containing their common chord. $\square$ 
A: Woah!! Amazing Problem!

Let the chords be $AC$ and $BD$. It is well known that the tangents from a focal chord intersect on the directrix and that the two tangents are perpendicular. If we drop the perpendicular $AA'$ from $A$ to the directrix, then $\angle A'AE = \angle AEF = \angle ECA$ so the circle with diameter $AC$ passes through E and is tangent to the directrix at $E$. Thus the power of $F$ with respect to $(AEC)$ is $EF^2$. Similarly, the power of $F$ with respect to $(BGD)$ is $GF^2$. Let $F'$ be the reflection of $F$ with respect to the origin. Then the power of $F'$ with respect to $(AEC)$ is $EF'^2$ and similarly the power of $F'$ with respect to $(BGD)$ is $GF'^2$.
Now by Linearity of Power of Point, we have that $$\text{Pow}_O(AEC) - \text{Pow}_O(BGD) = \frac{1}{2} \left( \text{Pow}_F(AEC) - \text{Pow}_F(BGD) \right) + \frac{1}{2} \left( \text{Pow}_{F'}(AEC) - \text{Pow}_{F'}(BGD)  \right)$$
$$ = \frac{1}{2} ( -FE^2 + FG^2 + EF'^2 - GF'^2 )$$
$$ = 0 $$ because $FF' \perp EG$
And we are DONE!!!
(Note that power of a point is a directed quantity and hence the powers of $F$ are taken with a negative sign)
