Projective Bary

by yayups, May 11, 2019, 6:06 AM

This solution shows a nontrivial usage of the projective nature of barycentric coordinates.
USAMO Shortlist 2014, 110 Geometery Problems #77 wrote:
Let $ABC$ be a triangle with circumcircle $\Gamma$ and incircle $\gamma$. Let $A'$ be the mixtilinear excircle touch point, and let $A'B'$ and $A'C'$ be tangent to $\gamma$ with $B',C'\in\Gamma$. Let $X$ be the tangency point of $B'C'$ with $\gamma$ which exists by Poncelet's Porism. Show that $(XBC)$ is tangent to $\gamma$.

[asy]
 /* Geogebra to Asymptote conversion, documentation at artofproblemsolving.com/Wiki go to User:Azjps/geogebra */
 unitsize(0.2inches);
import graph; size(0cm); 
real labelscalefactor = 0.5; /* changes label-to-point distance */
pen dps = linewidth(0.7) + fontsize(10); defaultpen(dps); /* default pen style */ 
pen dotstyle = black; /* point style */ 
real xmin = -10, xmax = 14, ymin = -22.62, ymax = 13.46;  /* image dimensions */
pen zzttqq = rgb(0.6,0.2,0); 

draw((0.26,7.92)--(-1.52,-2.18)--(9.54,-2.2)--cycle, linewidth(2) + zzttqq); 
 /* draw figures */
draw((0.26,7.92)--(-1.52,-2.18), linewidth(2) + zzttqq); 
draw((-1.52,-2.18)--(9.54,-2.2), linewidth(2) + zzttqq); 
draw((9.54,-2.2)--(0.26,7.92), linewidth(2) + zzttqq); 
draw(circle((4.017668907550992,2.050905875698934), 6.968955550057753), linewidth(2)); 
draw(circle((2.278232171040842,1.001527516890443), 3.1883907164579206), linewidth(2)); 
draw((5.8094995867931365,8.78556876819826)--(0.07556713698788581,3.306761151157378), linewidth(2)); 
draw((0.07556713698788581,3.306761151157378)--(-2.791521751662705,0.5672401366735647), linewidth(2)); 
draw((-2.791521751662705,0.5672401366735647)--(-5.658856324457237,-2.1725156305163527), linewidth(2)); 
draw((-5.658856324457237,-2.1725156305163527)--(-1.52,-2.18), linewidth(2)); 
draw((-2.791521751662705,0.5672401366735647)--(5.215750162966643,-4.8142920649363115), linewidth(2)); 
draw((5.215750162966643,-4.8142920649363115)--(5.8094995867931365,8.78556876819826), linewidth(2)); 
 /* dots and labels */
dot((0.26,7.92),dotstyle); 
label("$A$", (0.34,8.12), N * labelscalefactor); 
dot((-1.52,-2.18),dotstyle); 
label("$B$", (-1.44,-1.98), NE * labelscalefactor); 
dot((9.54,-2.2),dotstyle); 
label("$C$", (9.62,-2), E *3* labelscalefactor); 
dot((2.2724665553022745,-2.1868579865376176),linewidth(4pt) + dotstyle); 
label("$D$", (2.36,-2.02), NE * labelscalefactor); 
dot((5.215750162966643,-4.8142920649363115),linewidth(4pt) + dotstyle); 
label("$A'$", (5.3,-4.66), S * 4*labelscalefactor); 
dot((-2.791521751662705,0.5672401366735647),linewidth(4pt) + dotstyle); 
label("$B'$", (-3.48,0.62), NW*0.01 * labelscalefactor); 
dot((5.8094995867931365,8.78556876819826),linewidth(4pt) + dotstyle); 
label("$C'$", (5.88,8.94), NE * labelscalefactor); 
dot((-5.658856324457237,-2.1725156305163527),linewidth(4pt) + dotstyle); 
label("$T$", (-6.02,-1.92), NE * labelscalefactor); 
dot((0.07556713698788581,3.306761151157378),linewidth(4pt) + dotstyle); 
label("$X$", (0.02,3.66), N * labelscalefactor); 
clip((xmin,ymin)--(xmin,ymax)--(xmax,ymax)--(xmax,ymin)--cycle); 
 /* end of picture */
 [/asy]

Firstly, the problem is clearly just asking us to show that $B'C'$ is tangent to $(XBC)$. Letting $T=B'C'\cap BC$, we see that this is equivalent to $TB\cdot TC=TX^2$, but $TD=TX$, so all we need to show is that
\[TB\cdot TC=TD^2.\]We'll actually just compute the barycentric coordinates of $T$ and verify this explicitly. However, finding $B'$ and $C'$ is really messy, and this doesn't seem tractable immediately. However, the beauty of this solution is getting a simple way to find the coordinates of $T$.

Let $P$ be a variable point on $BC$, and define the composite map $\phi$ given by
\[P\mapsto P'\mapsto P_1P_2\cap BC\]where $P'$ is the $\sqrt{bc}$ inverse of $P$ and $P_1P'$ and $P_2P'$ are tangent to $\gamma$ with $P_1,P_2\in\Gamma$. It's not easy to see that this map $\phi$ is projective but its true.

Why?

Now, we check that
\[B\mapsto C\mapsto AB\mapsto B,\]so $\phi(B)=B$, and similarly $\phi(C)=C$. Also,
\[\infty_{BC}\mapsto A\mapsto BC,\]but uh-oh, what's $BC\cap BC$? The fix is that we actually have the tangent to $\gamma$ at some point infinitesimally close to $D$, which then intersects $BC$ really close to $D$, so we have $\phi(\infty_{BC})=D$.

Now, use projective coordinates for $BC$ given by the last two coordinates of the barycentric coordinates of a point on $BC$. The map $\phi$ looks like some matrix
\[\begin{pmatrix}w & x\\ y& z\end{pmatrix}\]that is considered the same under scaling. We see that $B=(1:0)$ and $C=(0:1)$ map to themselves, so $x=y=0$. The point $\infty_{BC}$ is given by $(1:-1)$, and it maps to $D=(s-c:s-b)$, so the matrix is
\[\phi\equiv \begin{pmatrix}s-c & 0\\ 0 & -(s-b)\end{pmatrix}.\]Now, we see that $T=\phi(D)$ since $D$ and $A'$ are $\sqrt{bc}$ inverses (the incircle gets sent to the mixtilinear excircle), so
\[T=\begin{pmatrix}s-c & 0\\ 0 & -(s-b)\end{pmatrix}\begin{pmatrix}s-c \\ s-b\end{pmatrix}=\begin{pmatrix}(s-c)^2 \\ -(s-b)^2\end{pmatrix},\]so $T=((s-c)^2:-(s-b)^2)$. The rest is a boring bash which we do below.

Homogenizing, we have $D=\left(\frac{s-c}{a},\frac{s-b}{a}\right)$, $T=\left(\frac{(s-c)^2}{a(b-c)},-\frac{(s-b)^2}{a(b-c)}\right)$, $B=(1,0)$, and $C=(0,1)$. By taking simply the first coordinate, we get a coordinate system on $BC$ that preserves the lengths in the original setup, so
\[TB=\frac{(s-c)^2}{(b-c)a}-1=\frac{(s-b)^2}{(b-c)a}\]and $TC=\frac{(s-c)^2}{(b-c)a}$, and
\[TD=\frac{(s-c)^2}{(b-c)a}-\frac{s-c}{a}=\frac{s-c}{a}\cdot\frac{s-b}{b-c}=\frac{(s-b)(s-c)}{a(b-c)}.\]Evidently, we have $TB\cdot TC=TD^2$, as desired. As we showed before, this means $TB\cdot TD=TX^2$, so $(XBC)$ is tangent to $B'C'$, which is tangent to $\gamma$ at $X$, so $(XBC)$ is tangent to $\gamma$. $\blacksquare$
This post has been edited 3 times. Last edited by yayups, May 11, 2019, 10:35 PM

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4 Comments

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woah how does one access USAMO SL :O

one does not. "110 Geometery Problem #77"
This post has been edited 1 time. Last edited by yayups, May 11, 2019, 10:03 PM

by rocketscience, May 11, 2019, 8:38 PM

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Is there a more "normal" solution to this using known properties of $X$ (say 2002 g7)

I'm not sure, but I'm also not the best person to ask since my configuration geometry isn't the best. The official solution inverts about the incircle and does a bunch of stuff after that.
This post has been edited 1 time. Last edited by yayups, May 11, 2019, 10:39 PM

by Generic_Username, May 11, 2019, 10:25 PM

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Alternatively by DDIT we have $Z=AT\cap A'D\in \odot{ABC}$.Now we have to show $BC$ is tangent to $\odot{ZAD}$.Equivalently $\angle{ADC}=\angle{ABA'}$.But since $D\to A'$ under $\sqrt{AB\cdot AC} \implies \triangle ADC\sim \triangle ABA'$ which concludes the problem.$\square$

by Pluto1708, Jan 6, 2020, 7:10 PM

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Woah I sort of knew bary and projective coordinates were connected because they're both homogenous and there is something said about homogenous coordinates being nice for projective in EGMO, but this is really interesting.

My sol for this problem uses the DDIT lemma that above uses plus a bunch of projections, I think the config knowledge is pretty standard for people who know a little bit about mixtilinear.

by i3435, Apr 2, 2021, 9:22 PM

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