用曲线系方法解2023年ELMO预选题G7
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2023年ELMO预选题G7
已知椭圆$\mathcal E$的焦点为$F_1$和$F_2$,$P$是$\mathcal E$上一点.直线$PF_1$和$PF_2$分别再次交$\mathcal E$于不同的点$A$和点$B$,点$A$和点$B$处的$\mathcal E$的切线交于点$Q$.证明:$PQ$的中点在$\triangle PF_1F_2$的外接圆上.
设椭圆为:$\dfrac{x^2}{a^2}+\dfrac{y^2}{b^2}=1$($a>b>0$),$c=\sqrt{a^2-b^2}$. 则$F_1(-c,0)$,$F_2(c,0)$,设$P(x_1,y_1)$,$Q(x_2,y_2)$. $\mathcal E$在点$P$处的切线$PP$方程为:$\dfrac{x_1x}{a^2}+\dfrac{y_1y}{b^2}=1$. 点$Q$关于$\mathcal E$的切点弦方程为:$\dfrac{x_2x}{a^2}+\dfrac{y_2y}{b^2}=1$. 过$P,P,A,B$四点的二次曲线系方程为: $$\lambda\left(\dfrac{x^2}{a^2}+\dfrac{y^2}{b^2}-1\right)+\mu\left(\frac{x_1x}{a^2}+\frac{y_1y}{b^2}-1\right)\left(\frac{x_2x}{a^2}+\frac{y_2y}{b^2}-1\right)=0.$$
其中一条为双直线$PA\times PB$: $$(y_1x-(x_1+c)y+y_1c)(y_1-(x_1-c)y-y_1c)=0.$$
对比$(1)$和$(2)$中$x$的系数得:$$\mu\left(\frac{x_{1}}{a^{2}}\cdot(-1)+(-1)\cdot\frac{x_{2}}{a^{2}}\right)=y_{1}\cdot(-y_{1})+y_{1}\cdot y_{1}$$ 注意到$\mu\neq 0$(否则为椭圆),于是$x_{1}+x_{2}=0$. 对比$(1)$和$(2)$中$y$的系数得:$$\mu\left(\frac{y_{1}}{b^{2}}\cdot(-1)+(-1)\cdot\frac{y_{2}}{b^{2}}\right)=-(x_{1}+c)\cdot(-y_{1})+y_{1}\cdot(-(x_{1}-c))$$ 化简得:$y_{1}+y_{2}=-\dfrac{2b^{2}c^{2}y_{1}}{\mu}$. 对比$(1)$和$(2)$中$xy$的系数得:$$\mu\left(\frac{x_{1}}{a^{2}}\cdot\frac{y_{2}}{b^{2}}+\frac{y_{1}}{b^{2}}\cdot\frac{x_{2}}{a^{2}}\right)=y_{1}\cdot(-(x_{1}-c))+(-(x_{1}+c))\cdot y_{1}$$ 代入$x_{1}+x_{2}=0$,并化简得:$y_{1}-y_{2}=\frac{2a^{2}b^{2}y_{1}}{\mu}$. 于是$\dfrac{y_{1}-y_{2}}{y_{1}+y_{2}}=-\dfrac{a^{2}}{c^{2}}$,即$\dfrac{y_{1}+y_{2}}{2}=-\dfrac{c^{2}}{b^{2}}y_{1}$. 因此$PQ$中点$M$的坐标为$\left(0,-\dfrac{c^{2}}{b^{2}}y_{1}\right)$. 由对称性不妨设$y_{1}>0$. 设$\angle F_{1}PF_{2}=\alpha$,$\angle F_{1}MF_{2}=\beta$,则只需证明:$\alpha+\beta=\pi$. 熟知$S_{\triangle PF_{1}F_{2}}=b^{2}\tan\dfrac{\alpha}{2}=\dfrac{1}{2}\cdot 2c\cdot y_{1}$,于是$\tan\dfrac{\alpha}{2}=\dfrac{cy_{1}}{b^{2}}$. 因为$\triangle MF_{1}F_{2}$为等腰三角形,故$\tan\dfrac{\beta}{2}=\dfrac{c}{\frac{c^{2}}{b^{2}}y_{1}}=\dfrac{b^{2}}{cy_{1}}$. 因此$\tan\dfrac{\alpha}{2}\tan\dfrac{\beta}{2}=1$,证毕.
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\section*{2023年ELMO预选题G7}
已知椭圆$\mathcal E$的焦点为$F_1$和$F_2$,$P$是$\mathcal E$上一点.直线$PF_1$和$PF_2$分别再次交$\mathcal E$于不同的点$A$和点$B$,点$A$和点$B$处的$\mathcal E$的切线交于点$Q$.证明:$PQ$的中点在$\triangle PF_1F_2$的外接圆上.
\begin{proof}设椭圆为:$\dfrac{x^2}{a^2}+\dfrac{y^2}{b^2}=1$($a>b>0$),$c=\sqrt{a^2-b^2}$.
则$F_1(-c,0)$,$F_2(c,0)$,设$P(x_1,y_1)$,$Q(x_2,y_2)$.
$\mathcal E$在点$P$处的切线$PP$方程为:$\dfrac{x_1x}{a^2}+\dfrac{y_1y}{b^2}=1$.
点$Q$关于$\mathcal E$的切点弦方程为:$\dfrac{x_2x}{a^2}+\dfrac{y_2y}{b^2}=1$.
过$P,P,A,B$四点的二次曲线系方程为:\begin{equation}\lambda\left(\dfrac{x^2}{a^2}+\dfrac{y^2}{b^2}-1\right)+\mu\left(\frac{x_1x}{a^2}+\frac{y_1y}{b^2}-1\right)\left(\frac{x_2x}{a^2}+\frac{y_2y}{b^2}-1\right)=0.\end{equation}
其中一条为双直线$PA\times PB$:\begin{equation}(y_1x-(x_1+c)y+y_1c)(y_1-(x_1-c)y-y_1c)=0.\end{equation}
对比$(1)$和$(2)$中$x$的系数得:$$\mu\left(\frac{x_{1}}{a^{2}}\cdot(-1)+(-1)\cdot\frac{x_{2}}{a^{2}}\right)=y_{1}\cdot(-y_{1})+y_{1}\cdot y_{1}$$
注意到$\mu\neq 0$(否则为椭圆),于是$x_{1}+x_{2}=0$.
对比$(1)$和$(2)$中$y$的系数得:$$\mu\left(\frac{y_{1}}{b^{2}}\cdot(-1)+(-1)\cdot\frac{y_{2}}{b^{2}}\right)=-(x_{1}+c)\cdot(-y_{1})+y_{1}\cdot(-(x_{1}-c))$$
化简得:$y_{1}+y_{2}=-\dfrac{2b^{2}c^{2}y_{1}}{\mu}$.
对比$(1)$和$(2)$中$xy$的系数得:$$\mu\left(\frac{x_{1}}{a^{2}}\cdot\frac{y_{2}}{b^{2}}+\frac{y_{1}}{b^{2}}\cdot\frac{x_{2}}{a^{2}}\right)=y_{1}\cdot(-(x_{1}-c))+(-(x_{1}+c))\cdot y_{1}$$
代入$x_{1}+x_{2}=0$,并化简得:$y_{1}-y_{2}=\frac{2a^{2}b^{2}y_{1}}{\mu}$.
于是$\dfrac{y_{1}-y_{2}}{y_{1}+y_{2}}=-\dfrac{a^{2}}{c^{2}}$,即$\dfrac{y_{1}+y_{2}}{2}=-\dfrac{c^{2}}{b^{2}}y_{1}$.
因此$PQ$中点$M$的坐标为$\left(0,-\dfrac{c^{2}}{b^{2}}y_{1}\right)$.
由对称性不妨设$y_{1}>0$.
设$\angle F_{1}PF_{2}=\alpha$,$\angle F_{1}MF_{2}=\beta$,则只需证明:$\alpha+\beta=\pi$.
熟知$S_{\triangle PF_{1}F_{2}}=b^{2}\tan\dfrac{\alpha}{2}=\dfrac{1}{2}\cdot 2c\cdot y_{1}$,于是$\tan\dfrac{\alpha}{2}=\dfrac{cy_{1}}{b^{2}}$.
因为$\triangle MF_{1}F_{2}$为等腰三角形,故$\tan\dfrac{\beta}{2}=\dfrac{c}{\frac{c^{2}}{b^{2}}y_{1}}=\dfrac{b^{2}}{cy_{1}}$.
因此$\tan\dfrac{\alpha}{2}\tan\dfrac{\beta}{2}=1$,证毕.\end{proof}



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