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Junior Balkan Mathematical Olympiad

Geometry Difficulty 7.6 National Olympiad, round 2 Prove it JBMO

Problem:
Let XYX Y be a chord of a circle Ω\Omega, with center OO, which is not a diameter. Let P,QP, Q be two distinct points inside the segment XYX Y, where QQ lies between PP and XX. Let ℓ\ell the perpendicular line dropped from PP to the diameter which passes through QQ. Let MM be the intersection point of ℓ\ell and Ω\Omega, which is closer to PP. Prove that
MP⋅XY≥2⋅QX⋅PY M P \cdot X Y \geq 2 \cdot Q X \cdot P Y

Solution

Solution by PSC. At first, we will allow PP and QQ to coincide, and we will prove the inequality in this case. Let the perpendicular from QQ to OQO Q meet Ω\Omega at BB and CC. Then, we have that QB=QCQ B=Q C. We will show that
BQ⋅XY≥2QX⋅QY B Q \cdot X Y \geq 2 Q X \cdot Q Y
By the power of a point Theorem we have that
QX⋅QY=QB⋅QC=QB2 Q X \cdot Q Y=Q B \cdot Q C=Q B^{2}
therefore it is enough to prove that XY≥2BQX Y \geq 2 B Q or XY≥BCX Y \geq B C. Let TT be the foot of the perpendicular from OO to XYX Y. Then, from the right-angled triangle OTQO T Q we have that OT≤OQO T \leq O Q, so the distance from OO to the chord XYX Y is smaller or equal to the distance from OO to the chord BCB C. This means that XY≥BCX Y \geq B C, so (1) holds.

Figure 1

Back to the initial problem, we have to prove that
MP⋅XY≥2QX⋅PY⟺XY2QX≥PYPM M P \cdot X Y \geq 2 Q X \cdot P Y \Longleftrightarrow \frac{X Y}{2 Q X} \geq \frac{P Y}{P M}
By (1) we have that
XY2QX≥QYQB \frac{X Y}{2 Q X} \geq \frac{Q Y}{Q B}
so it is enough to prove that
QYQB≥PYPM \frac{Q Y}{Q B} \geq \frac{P Y}{P M}
If CBC B meets YMY M at SS, then from MP∥QSM P \| Q S we get
QYQB≥QYQS=PYPM \frac{Q Y}{Q B} \geq \frac{Q Y}{Q S}=\frac{P Y}{P M}
which is the desired.

We will show that (QM−QP)⋅XY≥2⋅QX⋅PY(Q M-Q P) \cdot X Y \geq 2 \cdot Q X \cdot P Y. Since MP≥QM−QPM P \geq Q M-Q P, our inequality follows directly. Let AA the intersection point of ℓ\ell with the diameter which passes through QQ. Like in the following picture, choose a coordinative system centered at OO and such that Q=(a,0),A=(c,0)Q=(a, 0), A=(c, 0), P=(c,h)P=(c, h) and denote the lengths QX=x,PQ=t,PY=y,OP=d,QM=zQ X=x, P Q=t, P Y=y, O P=d, Q M=z.
Let λQ=r2−a2\lambda_{Q}=r^{2}-a^{2} and λP=r2−d2\lambda_{P}=r^{2}-d^{2} respectively the power of QQ and PP with respect to our circle Ω\Omega. We will show that:
(z−t)(t+x+y)≥2xy (z-t)(t+x+y) \geq 2 x y
Figure 2

Adding and multiplying respectively the relations x(t+y)=λQx(t+y)=\lambda_{Q} and y(t+x)=λPy(t+x)=\lambda_{P}, we will have
t(x+y)+2xy=λP+λQ t(x+y)+2 x y=\lambda_{P}+\lambda_{Q}
and
xy(t+x)(t+y)=λPλQ x y(t+x)(t+y)=\lambda_{P} \lambda_{Q}
Using these two equations, it's easy to deduce that:
(xy)2−xy(t2+λP+λQ)+λPλQ=0 (x y)^{2}-x y\left(t^{2}+\lambda_{P}+\lambda_{Q}\right)+\lambda_{P} \lambda_{Q}=0
So, w1=xyw_{1}=x y is a zero of the second degree polynomial:
p(w)=w2−w(t2+λP+λQ)+λPλQ p(w)=w^{2}-w\left(t^{2}+\lambda_{P}+\lambda_{Q}\right)+\lambda_{P} \lambda_{Q}
But w1=xy<x(t+y)=λQw_{1}=x y<x(t+y)=\lambda_{Q} and
p(λQ)=(r2−a2)2−(r2−a2)(t2+λP+λQ)+λPλQ=(r2−a2)2−(r2−a2)(t2+r2−d2+r2−a2)+(r2−d2)(r2−a2)=(r2−a2)2−(r2−a2)t2−(r2−d2)(r2−a2)−(r2−a2)4+(r2−d2)(r2−a2)=−t2(r2−a2)=−t2λQ<0 \begin{aligned} p\left(\lambda_{Q}\right) & =\left(r^{2}-a^{2}\right)^{2}-\left(r^{2}-a^{2}\right)\left(t^{2}+\lambda_{P}+\lambda_{Q}\right)+\lambda_{P} \lambda_{Q} \\ & =\left(r^{2}-a^{2}\right)^{2}-\left(r^{2}-a^{2}\right)\left(t^{2}+r^{2}-d^{2}+r^{2}-a^{2}\right)+\left(r^{2}-d^{2}\right)\left(r^{2}-a^{2}\right) \\ & =\left(r^{2}-a^{2}\right)^{2}-\left(r^{2}-a^{2}\right) t^{2}-\left(r^{2}-d^{2}\right)\left(r^{2}-a^{2}\right)-\left(r^{2}-a^{2}\right)^{4}+\left(r^{2}-d^{2}\right)\left(r^{2}-a^{2}\right) \\ & =-t^{2}\left(r^{2}-a^{2}\right)=-t^{2} \lambda_{Q}<0 \end{aligned}
This implies that λQ\lambda_{Q} lies (strictly) between the two (positive) zeros w1,w2w_{1}, w_{2} of p(w)p(w) and w1=xyw_{1}=x y is the smaller one.
After using (2) and (3), inequality (1) can be rewritten as:
(xy)2≤(z−tz+t)λPλQ (x y)^{2} \leq\left(\frac{z-t}{z+t}\right) \lambda_{P} \lambda_{Q}
In order to show this, it is enough to show that
p(z−tz+tλPλQ)≤0 p\left(\sqrt{\frac{z-t}{z+t} \lambda_{P} \lambda_{Q}}\right) \leq 0
because this will imply z−tz+tλPλQ∈[w1,w2]\sqrt{\frac{z-t}{z+t} \lambda_{P} \lambda_{Q}} \in\left[w_{1}, w_{2}\right]. After some manipulations, inequality (6) can be equivalently transformed to:
4z2λPλQ≤(z2−t2)(t2+λP+λQ)2 4 z^{2} \lambda_{P} \lambda_{Q} \leq\left(z^{2}-t^{2}\right)\left(t^{2}+\lambda_{P}+\lambda_{Q}\right)^{2}
Since z2−t2=r2−d2=λPz^{2}-t^{2}=r^{2}-d^{2}=\lambda_{P}, this is equivalent to:
4z2λQ≤(t2+λP+λQ)2 4 z^{2} \lambda_{Q} \leq\left(t^{2}+\lambda_{P}+\lambda_{Q}\right)^{2}
But t2=(a−c)2+h2=a2+d2−2ac,z2=t2+r2−d2=a2−2ac+r2t^{2}=(a-c)^{2}+h^{2}=a^{2}+d^{2}-2 a c, z^{2}=t^{2}+r^{2}-d^{2}=a^{2}-2 a c+r^{2} and t2+λP+λQ=…=2(r2−ac)t^{2}+\lambda_{P}+\lambda_{Q}=\ldots=2\left(r^{2}-a c\right). Hence, (8) is equivalent with:
(a2−2ac+r2)(r2−a2)≤(r2−ac)2⇔⋯⇔0≤a2(a−c)2 \left(a^{2}-2 a c+r^{2}\right)\left(r^{2}-a^{2}\right) \leq\left(r^{2}-a c\right)^{2} \Leftrightarrow \cdots \Leftrightarrow 0 \leq a^{2}(a-c)^{2}
which is clearly true.

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