(a)
y = x y=\sqrt{x} y = x 이고 z = 2 3 x y = 2 3 x 3 / 2 z=\frac{2}{3}xy=\frac{2}{3}x^{3/2} z = 3 2 x y = 3 2 x 3/2 이므로,
r ( x ) = x ı ^ + x ȷ ^ + 2 3 x 3 / 2 k ^ \begin{aligned}
\mathbf{r}(x)&=x\,\hat{\boldsymbol{\imath}}+\sqrt{x}\,\hat{\boldsymbol{\jmath}}+\frac{2}{3}x^{3/2}\,\hat{\mathbf{k}} \end{aligned} r ( x ) = x ^ + x ^ + 3 2 x 3/2 k ^
이 문제의 나머지 부분을 위해 다음도 필요하다.
r ′ ( x ) = ı ^ + 1 2 x ȷ ^ + x k ^ r ′ ′ ( x ) = − 1 4 x 3 / 2 ȷ ^ + 1 2 x k ^ d s d x = ∣ r ′ ( x ) ∣ = 1 + 1 4 x + x = ( 1 2 x + x ) 2 = 1 2 x + x d s d x ( 1 ) = 3 2 \begin{aligned}
\mathbf{r}'(x)&=\hat{\boldsymbol{\imath}}+\frac{1}{2\sqrt{x}}\,\hat{\boldsymbol{\jmath}}+\sqrt{x}\,\hat{\mathbf{k}}\\
\mathbf{r}''(x)&=-\frac{1}{4x^{3/2}}\,\hat{\boldsymbol{\jmath}}+\frac{1}{2\sqrt{x}}\,\hat{\mathbf{k}}\\
\frac{\mathrm{d}s}{\mathrm{d}x}=|\mathbf{r}'(x)|
&=\sqrt{1+\frac{1}{4x}+x}
=\sqrt{\left(\frac{1}{2\sqrt{x}}+\sqrt{x}\right)^2}
=\frac{1}{2\sqrt{x}}+\sqrt{x}\\
\frac{\mathrm{d}s}{\mathrm{d}x}(1)&=\frac{3}{2}
\end{aligned} r ′ ( x ) r ′′ ( x ) d x d s = ∣ r ′ ( x ) ∣ d x d s ( 1 ) = ^ + 2 x 1 ^ + x k ^ = − 4 x 3/2 1 ^ + 2 x 1 k ^ = 1 + 4 x 1 + x = ( 2 x 1 + x ) 2 = 2 x 1 + x = 2 3
(b)
∫ C d s = ∫ 0 9 d s d x d x = ∫ 0 9 ( 1 2 x + x ) d x = [ x + 2 3 x 3 / 2 ] 0 9 = 3 + 18 = 21 \int_C \ ds
=\int_0^9 \frac{\mathrm{d}s}{\mathrm{d}x}\ \mathrm{d}x
=\int_0^9 \left(\frac{1}{2\sqrt{x}}+\sqrt{x}\right)\ \mathrm{d}x
=\left[\sqrt{x}+\frac{2}{3}x^{3/2}\right]_0^9
=3+18
=21 ∫ C d s = ∫ 0 9 d x d s d x = ∫ 0 9 ( 2 x 1 + x ) d x = [ x + 3 2 x 3/2 ] 0 9 = 3 + 18 = 21
(c)
다음과 같이 놓는다.
r ( x ) \mathbf{r}(x) r ( x ) : 입자의 첫째 좌표가 x x x 일 때의 위치,
R ( t ) \mathbf{R}(t) R ( t ) : 시각 t t t 에서의 입자의 위치,
x ( t ) x(t) x ( t ) : 시각 t t t 에서의 입자의 x x x –좌표,
s ( x ) s(x) s ( x ) : 원점에서 r ( x ) \mathbf{r}(x) r ( x ) 까지의 곡선의 길이.
모든 t t t 에 대해 ∣ R ′ ( t ) ∣ = 9 |\mathbf{R}'(t)|=9 ∣ R ′ ( t ) ∣ = 9 임이 주어져 있다.
따라서
R ( t ) = r ( x ( t ) ) ⟹ R ′ ( t ) = r ′ ( x ( t ) ) d x d t ( t ) ⟹ 9 = ∣ R ′ ( t ) ∣ = d s d x ( x ( t ) ) d x d t ( t ) = ( 1 2 x ( t ) + x ( t ) ) d x d t ( t ) \begin{aligned}
\mathbf{R}(t)=\mathbf{r}\big(x(t)\big)&\implies
\mathbf{R}'(t)=\mathbf{r}'\big(x(t)\big)\frac{\mathrm{d}x}{\mathrm{d}t}(t) \\
&\implies
9=|\mathbf{R}'(t)|=\frac{\mathrm{d}s}{\mathrm{d}x}\big(x(t)\big) \frac{\mathrm{d}x}{\mathrm{d}t}(t)
=\left(\frac{1}{2\sqrt{x(t)}}+\sqrt{x(t)}\right)\frac{\mathrm{d}x}{\mathrm{d}t}(t)
\end{aligned} R ( t ) = r ( x ( t ) ) ⟹ R ′ ( t ) = r ′ ( x ( t ) ) d t d x ( t ) ⟹ 9 = ∣ R ′ ( t ) ∣ = d x d s ( x ( t ) ) d t d x ( t ) = ( 2 x ( t ) 1 + x ( t ) ) d t d x ( t )
특히 입자가 시각 0 0 0 에 ( 1 , 1 , 2 3 ) (1,1,\frac{2}{3}) ( 1 , 1 , 3 2 ) 에 있다면 x ( 0 ) = 1 x(0)=1 x ( 0 ) = 1 이고
9 = ( 1 2 1 + 1 ) d x d t ( 0 ) ⟹ d x d t ( 0 ) = 6 9=\left(\frac{1}{2\sqrt{1}}+\sqrt{1}\right)\frac{\mathrm{d}x}{\mathrm{d}t}(0)
\implies \frac{\mathrm{d}x}{\mathrm{d}t}(0)=6 9 = ( 2 1 1 + 1 ) d t d x ( 0 ) ⟹ d t d x ( 0 ) = 6
이므로
R ′ ( 0 ) = r ′ ( 1 ) d x d t ( 0 ) = ( ı ^ + 1 2 ȷ ^ + k ^ ) 6 = 6 ı ^ + 3 ȷ ^ + 6 k ^ \mathbf{R}'(0)=\mathbf{r}'(1)\frac{\mathrm{d}x}{\mathrm{d}t}(0)
=\left(\hat{\boldsymbol{\imath}}+\frac{1}{2}\,\hat{\boldsymbol{\jmath}}+\hat{\mathbf{k}}\right)6
=\ 6\,\hat{\boldsymbol{\imath}}+3\,\hat{\boldsymbol{\jmath}}+6\,\hat{\mathbf{k}} R ′ ( 0 ) = r ′ ( 1 ) d t d x ( 0 ) = ( ^ + 2 1 ^ + k ^ ) 6 = 6 ^ + 3 ^ + 6 k ^
이다.
(d)
곱의 미분법과 연쇄 법칙에 의해,
R ′ ( t ) = r ′ ( x ( t ) ) d x d t ( t ) ⟹ R ′ ′ ( t ) = r ′ ′ ( x ( t ) ) ( d x d t ( t ) ) 2 + r ′ ( x ( t ) ) d 2 x d t 2 ( t ) \mathbf{R}'(t)=\mathbf{r}'\big(x(t)\big)\frac{\mathrm{d}x}{\mathrm{d}t}(t)\implies
\mathbf{R}''(t)=\mathbf{r}''\big(x(t)\big)\left(\frac{\mathrm{d}x}{\mathrm{d}t}(t)\right)^2
+\mathbf{r}'\big(x(t)\big)\frac{\mathrm{d^2}x}{\mathrm{d}{t}^2}(t) R ′ ( t ) = r ′ ( x ( t ) ) d t d x ( t ) ⟹ R ′′ ( t ) = r ′′ ( x ( t ) ) ( d t d x ( t ) ) 2 + r ′ ( x ( t ) ) d t 2 d 2 x ( t )
(c)에서
9 = ∣ R ′ ( t ) ∣ = ( 1 2 x ( t ) + x ( t ) ) d x d t ( t ) 9=|\mathbf{R}'(t)|=\Big(\frac{1}{2\sqrt{x(t)}}+\sqrt{x(t)}\Big)\frac{\mathrm{d}x}{\mathrm{d}t}(t) 9 = ∣ R ′ ( t ) ∣ = ( 2 x ( t ) 1 + x ( t ) ) d t d x ( t )
임을 보았으므로
d x d t ( t ) = 9 ( 1 2 x ( t ) + x ( t ) ) − 1 \frac{\mathrm{d}x}{\mathrm{d}t}(t)=9\left(\frac{1}{2\sqrt{x(t)}}+\sqrt{x(t)}\right)^{-1} d t d x ( t ) = 9 ( 2 x ( t ) 1 + x ( t ) ) − 1
이다. 이를 미분하면
d 2 x d t 2 ( t ) = − 9 ( 1 2 x ( t ) + x ( t ) ) − 2 ( − 1 4 x ( t ) 3 / 2 + 1 2 x ( t ) ) d x d t ( t ) \frac{d^2x}{dt^2}(t)=-9\left(\frac{1}{2\sqrt{x(t)}}+\sqrt{x(t)}\right)^{-2}
\left(-\frac{1}{4x(t)^{3/2}}+\frac{1}{2\sqrt{x(t)}}\right)\frac{\mathrm{d}x}{\mathrm{d}t}(t) d t 2 d 2 x ( t ) = − 9 ( 2 x ( t ) 1 + x ( t ) ) − 2 ( − 4 x ( t ) 3/2 1 + 2 x ( t ) 1 ) d t d x ( t )
이다. 특히 t = 0 t=0 t = 0 일 때 x ( 0 ) = 1 x(0)=1 x ( 0 ) = 1 이고 d x d t ( 0 ) = 6 \frac{\mathrm{d}x}{\mathrm{d}t}(0)=6 d t d x ( 0 ) = 6 이므로
d 2 x d t 2 ( 0 ) = − 9 ( 3 2 ) − 2 ( 1 4 ) 6 = − 6 \frac{\mathrm{d^2}x}{\mathrm{d}{t}^2}(0)=-9\left(\frac{3}{2}\right)^{-2}
\left(\frac{1}{4}\right)6=-6 d t 2 d 2 x ( 0 ) = − 9 ( 2 3 ) − 2 ( 4 1 ) 6 = − 6
이고, 따라서
R ′ ′ ( 0 ) = r ′ ′ ( 1 ) ( 6 ) 2 + r ′ ( 1 ) ( − 6 ) = 36 ( − 1 4 ȷ ^ + 1 2 k ^ ) − 6 ( ı ^ + 1 2 ȷ ^ + k ^ ) = − 6 ı ^ − 12 ȷ ^ + 12 k ^ \begin{aligned}
\mathbf{R}''(0)&=\mathbf{r}''(1)\ \big(6\big)^2+\mathbf{r}'(1)\big(-6\big)
=36\left(-\frac{1}{4}\,\hat{\boldsymbol{\jmath}}+\frac{1}{2}\,\hat{\mathbf{k}}\right)
-6\left(\hat{\boldsymbol{\imath}}+\frac{1}{2}\,\hat{\boldsymbol{\jmath}}+\hat{\mathbf{k}}\right) \\
&=-6\,\hat{\boldsymbol{\imath}}-12\,\hat{\boldsymbol{\jmath}}+12\,\hat{\mathbf{k}} \end{aligned} R ′′ ( 0 ) = r ′′ ( 1 ) ( 6 ) 2 + r ′ ( 1 ) ( − 6 ) = 36 ( − 4 1 ^ + 2 1 k ^ ) − 6 ( ^ + 2 1 ^ + k ^ ) = − 6 ^ − 12 ^ + 12 k ^
이다.