Prove that for any point $\rm P$ and triangle $\triangle\rm ABC$
$$
a\cdot{\rm PA}^2 + b\cdot{\rm PB}^2 + c\cdot{\rm PC}^2
= a\cdot{\rm IA}^2 + b\cdot{\rm IB}^2 + c\cdot{\rm IC}^2 + (a + b + c){\rm IP}^2,
$$
where $a = {\rm BC}, b = {\rm CA}, c = {\rm AB}$ and $\rm I$ is the incenter of
$\triangle\rm ABC$.
Proposed in Crux Mathematicorum, Vol. 14, No. 9 as problem 6; from the 1988 IMO shortlist, by Singapore.
My proof consists in some very nasty algebraic manipulations, resulting from
the indiscriminate use of barycentric coordinates; you have been warned. Let
thus ${\rm P} = (u, v, w)$ be the normalized barycentric coordinates of the
point $\rm P$ (that is, $u+v+w=1$), and recall that those of the remaining ones
are
$$
{\rm A} = (1, 0, 0),\qquad
{\rm B} = (0, 1, 0),\qquad
{\rm C} = (0, 0, 1),\qquad
{\rm I} = \left(\frac a{a+b+c}, \frac b{a+b+c}, \frac c{a+b+c}\right). \tag1
$$
The distance formula for points $\rm P,Q$ in normalized barycentric coordinates
requires taking the so-called displacement vector
$\overrightarrow{\rm PQ} = (r,s,t)$ whose entries are the subtraction of those
of $\rm P$ from those of $\rm Q$; then, it holds that
$$
{\rm PQ}^2 = -a^2st - b^2tr - c^2rs.
$$
Hence $\overrightarrow{\rm AP}=(u - 1, v, w), \overrightarrow{\rm BP}=(u, v - 1, w), \overrightarrow{\rm CP}=(u, v, w - 1)$,
and expanding the left-hand side of the proposed identity yields
$$
\begin{alignat*}2
a\cdot{\rm PA}^2 + b\cdot{\rm PB}^2 + c\cdot{\rm PC}^2
&= &&-a\left[a^2vw + b^2(u-1)w + c^2(u-1)v\right]\\
& &&- b\left[a^2(v-1)w + b^2 uw + c^2 u(v-1)\right]\\
& &&- c\left[a^2v(w-1) + b^2 u(w-1) + c^2 uv\right]\\
&= &&-a^3vw - ab^2uw + ab^2w - ac^2uv + ac^2v\\
& &&-a^2bvw + a^2bw - b^3 uw - bc^2uv + bc^2u\\
& &&-a^2cvw + a^2cv - b^2cuw + b^2cu - c^3uv; \tag2
\end{alignat*}
$$
substituting the values of the last term in equation $(1)$ into the previous
equation produces the first three terms of the right-hand side:
$$
\begin{alignat*}2
a\cdot{\rm IA}^2 + b\cdot{\rm IB}^2 + c\cdot{\rm IC}^2
&= &&-a\cdot \frac{a^2bc - b^2c(b+c) - c^2b(b+c)}{(a+b+c)^2}\\
& &&- b\cdot \frac{ab^2c - a^2c(a+c) - c^2a(a+c)}{(a+b+c)^2}\\
& &&- c\cdot \frac{abc^2 - a^2b(a+b) - b^2a(a+b)}{(a+b+c)^2}\\
&= &&\frac{-1}{(a+b+c)^2}(\cancel{a^3bc} - \cancel{ab^3c} - ab^2c^2 - ab^2c^2 - \cancel{abc^3}\\
& &&\phantom{\frac{-1}{(a+b+c)^2}}+ \cancel{ab^3c} - \cancel{a^3bc} - a^2bc^2 - a^2bc^2 - abc^3\\
& &&\phantom{\frac{-1}{(a+b+c)^2}}+ \cancel{abc^3} - a^3bc - a^2b^2c - a^2b^2c - ab^3c)\\
&= &&\frac{abc\cancel{(a+b+c)^2}}{\cancel{(a+b+c)^2}} = {\color{green} \boxed{abc,}} \tag3
\end{alignat*}
$$
and since $\overrightarrow{\rm IP} = (u-a/(a+b+c), v-b/(a+b+c), w-c/(a+b+c))$
it follows that
$$
\begin{alignat*}2
(a+b+c){\rm IP}^2
&= &&-a^2\left[(a+b+c)vw - bw - cv + \frac{bc}{a+b+c}\right]\\
& &&-b^2\left[(a+b+c)uw - aw - cu + \frac{ac}{a+b+c}\right]\\
& &&-c^2\left[(a+b+c)uv - av - bu + \frac{ab}{a+b+c}\right]\\
&= &&-a^3vw - a^2bvw - a^2cvw + a^2bw + a^2cv - \frac{a^2bc}{a+b+c}\\
& &&-ab^2uw - b^3uw - b^2cuw + ab^2w + b^2cu - \frac{ab^2c}{a+b+c}\\
& &&-ac^2uv - bc^2uv - c^3uv + ac^2v + bc^2u - \frac{abc^2}{a+b+c}. \tag4
\end{alignat*}
$$
Finally, notice that the left-hand side is contained in the $u,v,w$ terms of
equation $(4)$, so it suffices to show that the remaining summands are
cancelled by $(3)$. Indeed
$$
abc - \frac{a^2bc + ab^2c + abc^2}{a+b+c}
= abc - \frac{abc\cancel{(a+b+c)}}{\cancel{a+b+c}} = {\color{green} \boxed{0,}}
$$
as it was to be proven.
References¶
Juan Serrano de Rodrigo (2024). Coordenadas baricéntricas. https://ttm.unizar.es/2024-25/Coordenadas_baricentricas.pdf.