1 2 A 0 A 3 ⃗ ⋅ ( A 0 A 1 ⃗ − 1 2 A 0 A 3 ⃗ ) = cos 2 3 π \displaystyle \frac{1}{2} \vec{A _{0} A _{3}} \cdot ( \vec{A _{0} A _{1}} - \frac{1}{2} \vec{A _{0} A _{3}} ) = \cos \frac{2}{3} \pi 2 1 A 0 A 3 ⋅ ( A 0 A 1 − 2 1 A 0 A 3 ) = cos 3 2 π
A 0 A 3 ⃗ ⋅ A 0 A 1 ⃗ − 1 2 ∣ A 0 A 3 ⃗ ∣ 2 = − 1 \displaystyle \vec{A _{0} A _{3}} \cdot \vec{A _{0} A _{1}} - \frac{1}{2} | \vec{A _{0} A _{3}} | ^{2} = - 1 A 0 A 3 ⋅ A 0 A 1 − 2 1 ∣ A 0 A 3 ∣ 2 = − 1 …㉠
1 2 A 0 A 3 ⃗ ⋅ ( A 0 A 2 ⃗ − 1 2 A 0 A 3 ⃗ ) = cos π 3 \displaystyle \frac{1}{2} \vec{A _{0} A _{3}} \cdot ( \vec{A _{0} A _{2}} - \frac{1}{2} \vec{A _{0} A _{3}} ) = \cos \frac{\pi}{3} 2 1 A 0 A 3 ⋅ ( A 0 A 2 − 2 1 A 0 A 3 ) = cos 3 π
A 0 A 3 ⃗ ⋅ A 0 A 2 ⃗ − 1 2 ∣ A 0 A 3 ⃗ ∣ 2 = 1 \displaystyle \vec{A _{0} A _{3}} \cdot \vec{A _{0} A _{2}} - \frac{1}{2} | \vec{A _{0} A _{3}} | ^{2} = 1 A 0 A 3 ⋅ A 0 A 2 − 2 1 ∣ A 0 A 3 ∣ 2 = 1 …㉡
1 2 A 0 A 3 ⃗ ⋅ ( A 0 A 3 ⃗ − 1 2 A 0 A 3 ⃗ ) = 1 \displaystyle \frac{1}{2} \vec{A _{0} A _{3}} \cdot ( \vec{A _{0} A _{3}} - \frac{1}{2} \vec{A _{0} A _{3}} ) = 1 2 1 A 0 A 3 ⋅ ( A 0 A 3 − 2 1 A 0 A 3 ) = 1
∴ \therefore ∴ ∣ A 0 A 3 ⃗ ∣ = 2 | \vec{A _{0} A _{3}} | = 2 ∣ A 0 A 3 ∣ = 2
이때, ㉠, ㉡에 대입하면
A 0 A 3 ⃗ ⋅ A 0 A 1 ⃗ = 1 \vec{A _{0} A _{3}} \cdot \vec{A _{0} A _{1}} = 1 A 0 A 3 ⋅ A 0 A 1 = 1 , A 0 A 3 ⃗ ⋅ A 0 A 2 ⃗ = 3 \vec{A _{0} A _{3}} \cdot \vec{A _{0} A _{2}} = 3 A 0 A 3 ⋅ A 0 A 2 = 3
이고 A 0 A 3 ⃗ \vec{A _{0} A _{3}} A 0 A 3 과 A 0 A 1 ⃗ \vec{A _{0} A _{1}} A 0 A 1 이 이루는 각의 크기를 θ 1 \theta _{1} θ 1 , A 0 A 3 ⃗ \vec{A _{0} A _{3}} A 0 A 3 과 A 0 A 2 ⃗ \vec{A _{0} A _{2}} A 0 A 2 가 이루는 각의 크기를 θ 2 \theta _{2} θ 2 라 하면
A 0 A 3 ⃗ ⋅ A 0 A 1 ⃗ = 2 ∣ A 0 A 1 ⃗ ∣ cos θ 1 = 1 \vec{A _{0} A _{3}} \cdot \vec{A _{0} A _{1}} = 2 | \vec{A _{0} A _{1}} | \cos \theta _{1} = 1 A 0 A 3 ⋅ A 0 A 1 = 2∣ A 0 A 1 ∣ cos θ 1 = 1
∴ \therefore ∴ ∣ A 0 A 1 ⃗ ∣ cos θ 1 = 1 2 \displaystyle | \vec{A _{0} A _{1}} | \cos \theta _{1} = \frac{1}{2} ∣ A 0 A 1 ∣ cos θ 1 = 2 1
A 0 A 3 ⃗ ⋅ A 0 A 2 ⃗ = 4 cos θ 2 = 3 \vec{A _{0} A _{3}} \cdot \vec{A _{0} A _{2}} = 4 \cos \theta _{2} = 3 A 0 A 3 ⋅ A 0 A 2 = 4 cos θ 2 = 3
∴ \therefore ∴ cos θ 2 = 3 4 \displaystyle \cos \theta _{2} = \frac{3}{4} cos θ 2 = 4 3
이때,
∣ A 2 A 3 ⃗ ∣ 2 = 2 2 + 2 2 − 2 × 2 × 2 × 3 4 = 2 \displaystyle | \vec{A _{2} A _{3}} | ^{2} = 2 ^{2} + 2 ^{2} - 2 \times 2 \times 2 \times \frac{3}{4} = 2 ∣ A 2 A 3 ∣ 2 = 2 2 + 2 2 − 2 × 2 × 2 × 4 3 = 2
∴ \therefore ∴ ∣ A 2 A 3 ⃗ ∣ = 2 \displaystyle | \vec{A _{2} A _{3}} | = \sqrt{2} ∣ A 2 A 3 ∣ = 2
따라서, ∣ A 1 A 3 ⃗ ∣ = 2 | \vec{A _{1} A _{3}} | = 2 ∣ A 1 A 3 ∣ = 2 이고 ∣ A 0 A 1 ⃗ ∣ cos θ = 1 2 \displaystyle | \vec{A _{0} A _{1}} | \cos \theta = \frac{1}{2} ∣ A 0 A 1 ∣ cos θ = 2 1 이므로 점 A 1 A _{1} A 1 이 나타내는 도형은 선분 A 0 A 3 A _{0} A _{3} A 0 A 3 을 1 : 3 으로 내분하는 점을 C라 할 때, 점 C를 중심으로 하는 원이다.
1 2 \displaystyle \frac{1}{2} 2 1
3 2 \displaystyle \frac{3}{2} 2 3
따라서, 반지름의 길이를 r r r 라 하면
r 2 = 2 2 − ( 3 2 ) 2 = 7 4 \displaystyle r ^{2} = 2 ^{2} - ( \frac{3}{2} ) ^{2} = \frac{7}{4} r 2 = 2 2 − ( 2 3 ) 2 = 4 7
∴ \therefore ∴ r = 7 2 \displaystyle r = \frac{\sqrt{7}}{2} r = 2 7
이때, ∣ A 1 A 2 ⃗ ∣ | \vec{A _{1} A _{2}} | ∣ A 1 A 2 ∣ 가 최대가 되려면 즉, 선분 A 1 A 2 ‾ \displaystyle \overline{A _{1} A _{2}} A 1 A 2 가 가장 긴 경우는 점 A 1 A _{1} A 1 이 평면 A 0 A 2 A 3 A _{0} A _{2} A _{3} A 0 A 2 A 3 과 같은 평면에 있을 때이다.
1 2 \displaystyle \frac{1}{2} 2 1
3 2 \displaystyle \frac{3}{2} 2 3
7 2 \displaystyle \frac{\sqrt{7}}{2} 2 7
2 \displaystyle \sqrt{2} 2
그런데, A 0 A 1 ‾ = ( 7 2 ) 2 + ( 1 2 ) 2 = 2 \displaystyle \overline{A _{0} A _{1}} = \sqrt{( \frac{\sqrt{7}}{2} ) ^{2} + ( \frac{1}{2} ) ^{2}} = \sqrt{2} A 0 A 1 = ( 2 7 ) 2 + ( 2 1 ) 2 = 2 이므로 두 삼각형 A 0 A 1 A 3 A _{0} A _{1} A _{3} A 0 A 1 A 3 , A 0 A 2 A 3 A _{0} A _{2} A _{3} A 0 A 2 A 3 은 합동이므로 ∠ A 1 A 0 A 3 = θ 3 \angle A _{1} A _{0} A _{3} = \theta _{3} ∠ A 1 A 0 A 3 = θ 3 이라 하면
M 2 = 2 2 + ( 2 ) 2 − 2 × 2 × 2 cos ( θ 2 + θ 3 ) \displaystyle M ^{2} = 2 ^{2} + ( \sqrt{2} ) ^{2} - 2 \times 2 \times \sqrt{2} \cos ( \theta _{2} + \theta _{3} ) M 2 = 2 2 + ( 2 ) 2 − 2 × 2 × 2 cos ( θ 2 + θ 3 )
= 6 − 4 2 ( cos θ 2 cos θ 3 − sin θ 2 sin θ 3 ) \displaystyle = 6 - 4 \sqrt{2} ( \cos \theta _{2} \cos \theta _{3} - \sin \theta _{2} \sin \theta _{3} ) = 6 − 4 2 ( cos θ 2 cos θ 3 − sin θ 2 sin θ 3 )
= 6 − 4 2 ( 3 4 × 2 4 − 7 4 × 14 4 ) \displaystyle = 6 - 4 \sqrt{2} ( \frac{3}{4} \times \frac{\sqrt{2}}{4} - \frac{\sqrt{7}}{4} \times \frac{\sqrt{14}}{4} ) = 6 − 4 2 ( 4 3 × 4 2 − 4 7 × 4 14 )
= 6 − ( 3 2 − 7 2 ) = 8 \displaystyle = 6 - ( \frac{3}{2} - \frac{7}{2} ) = 8 = 6 − ( 2 3 − 2 7 ) = 8