점 A \mathrm{A} A 에서 선분 B C \mathrm{BC} BC 에 내린 수선의 발을 H \mathrm{H} H , 점 A \mathrm{A} A 를 선분 B C \mathrm{BC} BC 에 대하여 대칭이동한 점을 A ′ \mathrm{A}' A ′ 이라 하고, 선분 A B \mathrm{AB} AB 를 지름으로 하는 원의 중심을 O \mathrm{O} O 라 하자.
B A ⃗ ∙ B C ⃗ = C B ⃗ ∙ C D ⃗ \mathrm{\vec{BA}} \bullet \vec{BC} = \mathrm{\vec{CB}} \bullet \vec{CD} BA ∙ B C = CB ∙ C D 에서
B A ⃗ ∙ B C ⃗ − C B ⃗ ∙ C D ⃗ = 0 \mathrm{\vec{BA}} \bullet \vec{BC} - \mathrm{\vec{CB}} \bullet \vec{CD} = 0 BA ∙ B C − CB ∙ C D = 0 , B A ⃗ ∙ B C ⃗ + B C ⃗ ∙ C D ⃗ = 0 \mathrm{\vec{BA}} \bullet \vec{BC} + \mathrm{\vec{BC}} \bullet \vec{CD} = 0 BA ∙ B C + BC ∙ C D = 0
B C ⃗ ∙ ( B A ⃗ + C D ⃗ ) = 0 \mathrm{\vec{BC}} \bullet \left( \vec{BA} + \vec{CD} \right) = 0 BC ∙ ( B A + C D ) = 0
B A ⃗ = H A ⃗ − H B ⃗ \mathrm{\vec{BA}} = \mathrm{\vec{HA}} - \vec{HB} BA = HA − H B 이고, C D ⃗ = H D ⃗ − H C ⃗ \mathrm{\vec{CD}} = \mathrm{\vec{HD}} - \vec{HC} CD = HD − H C 이므로
B C ⃗ ∙ ( H A ⃗ − H B ⃗ + H D ⃗ − H C ⃗ ) = 0 \mathrm{\vec{BC}} \bullet \left( \vec{HA} - \vec{HB} + \vec{HD} - \vec{HC} \right) = 0 BC ∙ ( H A − H B + H D − H C ) = 0
B C ⃗ ∙ ( H A ⃗ + H D ⃗ ) = 0 \mathrm{\vec{BC}} \bullet \left( \vec{HA} + \vec{HD} \right) = 0 BC ∙ ( H A + H D ) = 0 (∵ \because ∵ H B ⃗ + H C ⃗ = 0 ⃗ \mathrm{\vec{HB}} + \vec{HC} = \vec{0} HB + H C = 0 )
H A ⃗ = − H A ′ ⃗ \mathrm{\vec{HA}} = - \mathrm{\vec{HA'}} HA = − H A ′ 이므로
B C ⃗ ∙ ( H D ⃗ − H A ′ ⃗ ) = 0 \mathrm{\vec{BC}} \bullet \left( \vec{HD} - \vec{HA'} \right) = 0 BC ∙ ( H D − H A ′ ) = 0 , B C ⃗ ∙ A ′ D ⃗ = 0 \mathrm{\vec{BC}} \bullet \vec{A' D} = 0 BC ∙ A ′ D = 0
따라서 B C ⃗ \mathrm{\vec{BC}} BC 와 A ′ D ⃗ \mathrm{\vec{A' D}} A ′ D 은 서로 수직이고 B C ⃗ ⊥ A A ′ ⃗ \mathrm{\vec{BC}} \perp \mathrm{\vec{AA'}} BC ⊥ A A ′ 이므로 점 D \mathrm{D} D 는 선분 A B \mathrm{AB} AB 의 수직이등분선 위의 점이고 다음 그림과 같이 직선 A A ′ \mathrm{AA}' AA ′ 위에 존재한다.
2 A C ⃗ ∙ A D ⃗ = D A ⃗ ∙ D B ⃗ \mathrm{2} \vec{AC} \bullet \vec{AD} = \mathrm{\vec{DA}} \bullet \vec{DB} 2 A C ∙ A D = DA ∙ D B 에서
2 A C ⃗ ∙ A D ⃗ = A D ‾ × A A ′ ‾ \displaystyle \mathrm{2} \vec{AC} \bullet \vec{AD} = \mathrm{\overline{AD}} \times \overline{AA'} 2 A C ∙ A D = AD × A A ′
D A ⃗ ∙ D B ⃗ \mathrm{\vec{DA}} \bullet \vec{DB} DA ∙ D B = A D ‾ × D H ‾ \displaystyle = \mathrm{\overline{AD}} \times \overline{DH} = AD × D H
이므로 A A ′ ‾ = D H ‾ \displaystyle \mathrm{\overline{AA'}} = \overline{DH} A A ′ = D H , 2 A H ‾ = H D ‾ \displaystyle \mathrm{2} \overline{AH} = \mathrm{\overline{HD}} 2 A H = HD
∴ \therefore ∴ A D ‾ = 3 A H ‾ \displaystyle \mathrm{\overline{AD}} = 3 \overline{AH} AD = 3 A H
이때 ∠ A B H = θ \mathrm{\angle} ABH = \theta ∠ A B H = θ 라 하면 ∠ A D O = θ \mathrm{\angle} ADO = \theta ∠ A D O = θ
A H ‾ = x \displaystyle \mathrm{\overline{AH}} = \mathit{x} AH = x 라 하면
sin θ = x 2 = 1 3 x \displaystyle \sin \theta = \frac{x}{2} = \frac{1}{3 x} sin θ = 2 x = 3 x 1 , x 2 = 2 3 \displaystyle x ^{2} = \frac{2}{3} x 2 = 3 2 , x = 6 3 \displaystyle x = \frac{\sqrt{6}}{3} x = 3 6
원 위의 점X \mathrm{X} X 에 대하여 D X ⃗ = D O ⃗ + O X ⃗ \mathrm{\vec{DX}} = \mathrm{\vec{DO}} + \vec{OX} DX = DO + O X 이므로
D X ⃗ ∙ B C ⃗ \mathrm{\vec{DX}} \bullet \vec{BC} DX ∙ B C = ( D O ⃗ + O X ⃗ ) ∙ B C ⃗ = \mathrm{\left( \vec{DO} + \vec{OX} \right)} \bullet \vec{BC} = ( DO + OX ) ∙ B C
= D O ⃗ ∙ B C ⃗ + O X ⃗ ∙ B C ⃗ \mathrm{=} \vec{DO} \bullet \vec{BC} + \vec{OX} \bullet \vec{BC} = D O ∙ B C + O X ∙ B C ⋯ \cdots ⋯ ⋯ \cdots ⋯ ㉠
이때 D O ⃗ \mathrm{\vec{DO}} DO 와 B C ⃗ \mathrm{\vec{BC}} BC 가 이루는 각은 π 2 + θ \displaystyle \frac{\pi}{2} + \theta 2 π + θ 이고 sin θ = x 2 \displaystyle \sin \theta = \frac{x}{2} sin θ = 2 x 에서
sin θ = 6 6 \displaystyle \sin \theta = \frac{\sqrt{6}}{6} sin θ = 6 6 , cos θ = 1 − sin 2 θ = 30 6 \displaystyle \cos \theta = \sqrt{1 - \sin ^{2} \theta} = \frac{\sqrt{30}}{6} cos θ = 1 − sin 2 θ = 6 30
또한
B C ‾ \displaystyle \mathrm{\overline{BC}} BC = 2 B H ‾ \displaystyle = \mathrm{2} \overline{BH} = 2 B H = 2 2 2 − x 2 \displaystyle = 2 \sqrt{2 ^{2} - x ^{2}} = 2 2 2 − x 2 = 2 4 − 2 3 \displaystyle = 2 \sqrt{4 - \frac{2}{3}} = 2 4 − 3 2 = 2 30 3 \displaystyle = \frac{2 \sqrt{30}}{3} = 3 2 30
D O ‾ \displaystyle \mathrm{\overline{DO}} DO = A D ‾ × cos θ \displaystyle = \mathrm{\overline{AD}} \times \cos \theta = AD × cos θ = 6 × 30 6 \displaystyle = \sqrt{6} \times \frac{\sqrt{30}}{6} = 6 × 6 30 = 5 \displaystyle = \sqrt{5} = 5
이므로 ㉠에서
D O ⃗ ∙ B C ⃗ \mathrm{\vec{DO}} \bullet \vec{BC} DO ∙ B C = D O ‾ × B C ‾ × cos ( π 2 + θ ) \displaystyle \mathrm{=} \overline{DO} \times \overline{BC} \times \cos \left( \frac{\pi}{2} + \theta \right) = D O × B C × cos ( 2 π + θ )
= 5 × 2 B H ‾ × ( − sin θ ) \displaystyle = \mathrm{\sqrt{5}} \times 2 \overline{BH} \times \left( - \sin \theta \right) = 5 × 2 B H × ( − sin θ )
= 5 × 2 30 3 × ( − 6 6 ) \displaystyle = \sqrt{5} \times \frac{2 \sqrt{30}}{3} \times \left( - \frac{\sqrt{6}}{6} \right) = 5 × 3 2 30 × ( − 6 6 )
= − 10 3 \displaystyle = - \frac{10}{3} = − 3 10 ⋯ \cdots ⋯ ⋯ \cdots ⋯ ㉡
점 X \mathrm{X} X 가 원 위의 점이므로 ∣ O X ⃗ ∣ = 1 \mathrm{\left| \vec{OX} \right|} = 1 OX = 1
− B C ‾ ≤ O X ⃗ ∙ B C ⃗ ≤ B C ‾ \displaystyle \mathrm{-} \overline{BC} \leq \mathrm{\vec{OX}} \bullet \vec{BC} \leq \overline{BC} − B C ≤ OX ∙ B C ≤ B C
− 2 30 3 ≤ O X ⃗ ∙ B C ⃗ ≤ 2 30 3 \displaystyle - \frac{2 \sqrt{30}}{3} \leq \mathrm{\vec{OX}} \bullet \vec{BC} \leq \frac{2 \sqrt{30}}{3} − 3 2 30 ≤ OX ∙ B C ≤ 3 2 30 ⋯ \cdots ⋯ ⋯ \cdots ⋯ ㉢
따라서 ㉠, ㉡, ㉢에 의하여
− 10 3 − 2 30 3 ≤ D X ⃗ ∙ B C ⃗ ≤ − 10 3 + 2 30 3 \displaystyle \mathrm{-} \frac{10}{3} - \frac{2 \sqrt{30}}{3} \leq \vec{DX} \bullet \vec{BC} \leq - \frac{10}{3} + \frac{2 \sqrt{30}}{3} − 3 10 − 3 2 30 ≤ D X ∙ B C ≤ − 3 10 + 3 2 30
이므로 M = − 10 3 + 2 30 3 \displaystyle M = - \frac{10}{3} + \frac{2 \sqrt{30}}{3} M = − 3 10 + 3 2 30 , m = − 10 3 − 2 30 3 \displaystyle m = - \frac{10}{3} - \frac{2 \sqrt{30}}{3} m = − 3 10 − 3 2 30
M × m M \times m M × m = 100 9 − 120 9 \displaystyle = \frac{100}{9} - \frac{120}{9} = 9 100 − 9 120 = − 20 9 \displaystyle = - \frac{20}{9} = − 9 20
따라서 ∣ M m ∣ \left| M m \right| ∣ M m ∣ = 20 9 \displaystyle = \frac{20}{9} = 9 20 이므로 p = 9 p = 9 p = 9 , q = 20 q = 20 q = 20
∴ \therefore ∴ p + q = 29 p + q = 29 p + q = 29