You are right, Grobber's solution is incorrect. He probably got confused by the asymmetric notations (this also happened to me when I saw the problem first). However, the problem is still quite easy:
In the following, $\left|P_1P_2P_3\right|$ will mean the (non-directed) area of a triangle $P_1P_2P_3$.
Let d be the circle with center D and radius DA = DC. This circle d clearly passes through the points A and C. Similarly, we have a circle e with center E and radius EA = EB, which passes through the points A and B, and a circle f with center F and radius FB = FC, which passes through the points B and C.
Let the two circles d and e intersect at a point S (apart from A). In the circle e, the angle < BEA is the central angle of the chord AB, while the angle < ASB is the obtuse chordal angle over this chord; hence, $\measuredangle BEA=2\cdot\left(180^{\circ}-\measuredangle ASB\right)$. Comparing this with $\measuredangle BEA=2\cdot\measuredangle ABC$, we get < ABC = 180° - < ASB, so that < ASB = 180° - < ABC. Similarly, we find < ASC = 180° - < BAC, since the point S lies on the circle d. Hence,
< BSC = 360° - < ASB - < ASC = 360° - (180° - < ABC) - (180° - < BAC)
= < ABC + < BAC = 180° - < ACB (by the sum of angles in triangle ABC).
Thus, < ACB = 180° - < BSC. Hence, $\measuredangle CFB=2\cdot\measuredangle ACB$ becomes $\measuredangle CFB=2\cdot\left(180^{\circ}-\measuredangle BSC\right)$. Now, since the points B and C lie on the circle f, and the angle < CFB is the central angle of the chord BC in this circle, this equation yields that < BSC is the obtuse chordal angle over the chord BC in this circle f; thus, the point S lies on the circle f.
Hence, the point S lies on all three circles d, e, f. The points B and S, being the two common points of the circles e and f, must be symmetric to each other with respect to the line EF joining the centers E and F of these circles; hence, the triangles BEF and SEF are congruent, so that | BEF | = | SEF |.
The two triangles DD'E and BD'E have a common altitude from the vertex E; thus, their areas are proportional to their bases DD' and BD'. In other words, $\frac{\left|DD^{\prime}E\right|}{\left|BD^{\prime}E\right|}=\frac{DD^{\prime}}{BD^{\prime}}$. In other words, $BD^{\prime}\cdot\left|DD^{\prime}E\right|=DD^{\prime}\cdot\left|BD^{\prime}E\right|$. Similarly, $BD^{\prime}\cdot\left|DD^{\prime}F\right|=DD^{\prime}\cdot\left|BD^{\prime}F\right|$. Hence,
$BD^{\prime}\cdot\left|DEF\right|=BD^{\prime}\cdot\left(\left|DD^{\prime}E\right|+\left|DD^{\prime}F\right|\right)=BD^{\prime}\cdot\left|DD^{\prime}E\right|+BD^{\prime}\cdot\left|DD^{\prime}F\right|$
$=DD^{\prime}\cdot\left|BD^{\prime}E\right|+DD^{\prime}\cdot\left|BD^{\prime}F\right|=DD^{\prime}\cdot\left(\left|BD^{\prime}E\right|+\left|BD^{\prime}F\right|\right)=DD^{\prime}\cdot\left|BEF\right|$
$=DD^{\prime}\cdot\left|SEF\right|$,
so that
$\frac{BD^{\prime}}{DD^{\prime}}=\frac{\left|SEF\right|}{\left|DEF\right|}$.
Hence,
$\frac{DB}{DD^{\prime}}=\frac{DD^{\prime}+BD^{\prime}}{DD^{\prime}}=1+\frac{BD^{\prime}}{DD^{\prime}}=1+\frac{\left|SEF\right|}{\left|DEF\right|}$.
Similarly,
$\frac{EC}{EE^{\prime}}=1+\frac{\left|SFD\right|}{\left|DEF\right|}$;
$\frac{FA}{FF^{\prime}}=1+\frac{\left|SDE\right|}{\left|DEF\right|}$.
Thus,
$\frac{DB}{DD^{\prime}}+\frac{EC}{EE^{\prime}}+\frac{FA}{FF^{\prime}}=\left(1+\frac{\left|SEF\right|}{\left|DEF\right|}\right)+\left(1+\frac{\left|SFD\right|}{\left|DEF\right|}\right)+\left(1+\frac{\left|SDE\right|}{\left|DEF\right|}\right)$
$=3+\frac{\left|SEF\right|+\left|SFD\right|+\left|SDE\right|}{\left|DEF\right|}=3+\frac{\left|DEF\right|}{\left|DEF\right|}=3+1=4$.
And the problem is solved.
Darij