第1章 1.10

(1)

x=t3−tx = t^3 - t

y=t2+t(t=1)y = t^2 + t \qquad (t = 1)

x′=3t2−1t=1のときx′=3−1=2x' = 3t^2 - 1 \qquad t = 1 \text{のとき} \qquad x' = 3 - 1 = 2

y′=2t+1t=1のときy′=2+1=3y' = 2t + 1 \qquad t = 1 \text{のとき} \qquad y' = 2 + 1 = 3

x′′=6tt=1のときx′′=6x'' = 6t \qquad t = 1 \text{のとき} \qquad x'' = 6

y′′=2y'' = 2

これから

v⃗=(x′,y′)=(2,3)a⃗=(x′′,y′′)=(6,2)v=∣v⃗∣=22+32=13\vec{v} = (x', y') = (2, 3) \qquad \vec{a} = (x'', y'') = (6, 2) \qquad v = |\vec{v}| = \sqrt{2^2 + 3^2} = \sqrt{13}

(2)

x=t−sin⁡tx = t - \sin t

y=1−cos⁡t(t=π3)y = 1 - \cos t \qquad \left(t = \frac{\pi}{3}\right)

x′=1−cos⁡tt=π3のときx′=1−cos⁡π3=12x' = 1 - \cos t \qquad t = \frac{\pi}{3} \text{のとき} \qquad x' = 1 - \cos\frac{\pi}{3} = \frac{1}{2}

y′=−(−sin⁡t)=sin⁡tt=π3のときy′=sin⁡π3=32y' = -(-\sin t) = \sin t \qquad t = \frac{\pi}{3} \text{のとき} \qquad y' = \sin\frac{\pi}{3} = \frac{\sqrt{3}}{2}

x′′=sin⁡tt=π3のときx′′=sin⁡π3=32x'' = \sin t \qquad t = \frac{\pi}{3} \text{のとき} \qquad x'' = \sin\frac{\pi}{3} = \frac{\sqrt{3}}{2}

y′′=cos⁡tt=π3のときy′′=cos⁡π3=12y'' = \cos t \qquad t = \frac{\pi}{3} \text{のとき} \qquad y'' = \cos\frac{\pi}{3} = \frac{1}{2}

これから

v⃗=(x′,y′)=(12,32)a⃗=(x′′,y′′)=(32,12)v=∣v⃗∣=(12)2+(32)2=1\vec{v} = (x', y') = \left(\frac{1}{2}, \frac{\sqrt{3}}{2}\right) \qquad \vec{a} = (x'', y'') = \left(\frac{\sqrt{3}}{2}, \frac{1}{2}\right) \qquad v = |\vec{v}| = \sqrt{\left(\frac{1}{2}\right)^2 + \left(\frac{\sqrt{3}}{2}\right)^2} = 1

解説: r31bn1z