문제 은행 · 미적분 · 대학 미적분 · 벡터와 공간

단위접선·법선벡터

먼저 혼자 풀어 보고, 풀이로 확인한 다음, 아래 「한 번 더」 문제로 이어서 연습하세요.

CLP-4 · 1.4절 · 6번대학 수준우리말 번역

CC 를 다음과 같은 공간곡선이라 하세요.

r(t)=(et−e−t) ı^+(et+e−t) ȷ^+2t k^\begin{aligned} \mathbf{r}(t) = \big(e^t - e^{-t}\big)\,\hat{\boldsymbol{\imath}} + \big(e^t + e^{-t}\big)\,\hat{\boldsymbol{\jmath}} +2t\,\hat{\mathbf{k}} \end{aligned}

(a) r′\mathbf{r}', r′′\mathbf{r}'' 와 CC 의 곡률을 구하세요. (b) r(0)\mathbf{r}(0) 과 r(1)\mathbf{r}(1) 사이의 곡선의 길이를 구하세요.

영어 원문 보기

Let CC be the space curve

r(t)=(et−e−t) ı^+(et+e−t) ȷ^+2t k^\begin{aligned} \mathbf{r}(t) = \big(e^t - e^{-t}\big)\,\hat{\boldsymbol{\imath}} + \big(e^t + e^{-t}\big)\,\hat{\boldsymbol{\jmath}} +2t\,\hat{\mathbf{k}} \end{aligned}

(a) Find r′\mathbf{r}', r′′\mathbf{r}'' and the curvature of CC. (b) Find the length of the curve between r(0)\mathbf{r}(0) and r(1)\mathbf{r}(1).

정답·풀이 보기

(a) 다음과 같으므로

r′(t)=(et+e−t) ı^+(et−e−t) ȷ^+2 k^dsdt(t)=∣r′(t)∣=4+2e2t+2e−2t=2(et+e−t)r′′(t)=(et−e−t) ı^+(et+e−t) ȷ^r′(t)×r′′(t)=−2(et+e−t) ı^+2(et−e−t) ȷ^+4 k^\begin{aligned} \mathbf{r}'(t)&=\big(e^t + e^{-t}\big)\,\hat{\boldsymbol{\imath}} + \big(e^t - e^{-t}\big)\,\hat{\boldsymbol{\jmath}} +2\,\hat{\mathbf{k}} & \frac{\mathrm{d}s}{\mathrm{d}t}(t) &=|\mathbf{r}'(t)|= \sqrt{4+2e^{2t}+2e^{-2t}} =\sqrt{2}\big(e^t+e^{-t}\big)\\ \mathbf{r}''(t)&=\big(e^t - e^{-t}\big)\,\hat{\boldsymbol{\imath}} + \big(e^t + e^{-t}\big)\,\hat{\boldsymbol{\jmath}} & \mathbf{r}'(t)\times\mathbf{r}''(t)&=-2\big(e^t + e^{-t}\big)\,\hat{\boldsymbol{\imath}} + 2\big(e^t - e^{-t}\big)\,\hat{\boldsymbol{\jmath}} +4\,\hat{\mathbf{k}} \end{aligned}

곡률은 다음과 같다.

κ(t)=∣v(t)×a(t)∣(dsdt)3=24+2e2t+2e−2t[4+2e2t+2e−2t]3/2=12+e2t+e−2t\begin{aligned} \kappa (t) &= \frac{|\mathbf{v}(t)\times\mathbf{a}(t)|}{\big(\frac{\mathrm{d}s}{\mathrm{d}t}\big)^3} =\frac{2\sqrt{4+2e^{2t}+2e^{-2t}}}{[4+2e^{2t}+2e^{-2t}]^{3/2}} =\frac{1}{2+e^{2t}+e^{-2t}} \end{aligned}

(b) r(0)\mathbf{r}(0) 과 r(1)\mathbf{r}(1) 사이의 CC 의 길이는 다음과 같다.

∫01dsdt(t) dt=2∫01(et+e−t) dt=2[et−e−t]01=2[e−1e]\begin{aligned} \int_0^1 \frac{\mathrm{d}s}{\mathrm{d}t}(t) \ \mathrm{d}t &= \sqrt{2} \int_0^1 (e^t+e^{-t}) \ \mathrm{d}t =\sqrt{2}\Big[e^t-e^{-t}\Big]_0^1 =\sqrt{2}\Big[e-\frac{1}{e}\Big] \end{aligned}

원본 교재 풀이(영어)

(a) As

r′(t)=(et+e−t) ı^+(et−e−t) ȷ^+2 k^dsdt(t)=∣r′(t)∣=4+2e2t+2e−2t=2(et+e−t)r′′(t)=(et−e−t) ı^+(et+e−t) ȷ^r′(t)×r′′(t)=−2(et+e−t) ı^+2(et−e−t) ȷ^+4 k^\begin{aligned} \mathbf{r}'(t)&=\big(e^t + e^{-t}\big)\,\hat{\boldsymbol{\imath}} + \big(e^t - e^{-t}\big)\,\hat{\boldsymbol{\jmath}} +2\,\hat{\mathbf{k}} & \frac{\mathrm{d}s}{\mathrm{d}t}(t) &=|\mathbf{r}'(t)|= \sqrt{4+2e^{2t}+2e^{-2t}} =\sqrt{2}\big(e^t+e^{-t}\big)\\ \mathbf{r}''(t)&=\big(e^t - e^{-t}\big)\,\hat{\boldsymbol{\imath}} + \big(e^t + e^{-t}\big)\,\hat{\boldsymbol{\jmath}} & \mathbf{r}'(t)\times\mathbf{r}''(t)&=-2\big(e^t + e^{-t}\big)\,\hat{\boldsymbol{\imath}} + 2\big(e^t - e^{-t}\big)\,\hat{\boldsymbol{\jmath}} +4\,\hat{\mathbf{k}} \end{aligned}

the curvature

κ(t)=∣v(t)×a(t)∣(dsdt)3=24+2e2t+2e−2t[4+2e2t+2e−2t]3/2=12+e2t+e−2t\begin{aligned} \kappa (t) &= \frac{|\mathbf{v}(t)\times\mathbf{a}(t)|}{\big(\frac{\mathrm{d}s}{\mathrm{d}t}\big)^3} =\frac{2\sqrt{4+2e^{2t}+2e^{-2t}}}{[4+2e^{2t}+2e^{-2t}]^{3/2}} =\frac{1}{2+e^{2t}+e^{-2t}} \end{aligned}

(b) The length of CC between r(0)\mathbf{r}(0) and r(1)\mathbf{r}(1) is

∫01dsdt(t) dt=2∫01(et+e−t) dt=2[et−e−t]01=2[e−1e]\begin{aligned} \int_0^1 \frac{\mathrm{d}s}{\mathrm{d}t}(t) \ \mathrm{d}t &= \sqrt{2} \int_0^1 (e^t+e^{-t}) \ \mathrm{d}t =\sqrt{2}\Big[e^t-e^{-t}\Big]_0^1 =\sqrt{2}\Big[e-\frac{1}{e}\Big] \end{aligned}

한 번 더 — 비슷한 문제CLP-4 · 1.4절 · 7번우리말 번역

점 (2,4,8)(2,4,8) 에서 r(t)=(t,t2,t3)\mathbf{r}(t)=(t,t^2,t^3) 의 열률을 구하세요.

답 쓰고 채점
다 풀었으면 정답 확인

점 (2,4,8)(2,4,8) 은 t=2t=2 일 때이다.

v(t)=(1,2t,3t2)v(2)=(1,4,12)a(t)=(0,2,6t)a(2)=(0,2,12)dadt(t)=(0,0,6)dadt(2)=(0,0,6)v(2)×a(2)=(24,−12,2)∣v(2)×a(2)∣=2181\begin{aligned} \mathbf{v}(t)&=(1,2t,3t^2) & \mathbf{v}(2)&=(1,4,12)\\ \mathbf{a}(t)&=(0,2,6t) & \mathbf{a}(2)&=(0,2,12)\\ \frac{\mathrm{d}\mathbf{a}}{\mathrm{d}t}(t)&=(0,0,6) & \frac{\mathrm{d}\mathbf{a}}{\mathrm{d}t}(2)&=(0,0,6)\\ && \mathbf{v}(2) \times \mathbf{a}(2)&=(24,-12,2)\\ && |\mathbf{v}(2) \times \mathbf{a}(2)|&=2\sqrt{181} \end{aligned}

이제 열률 공식을 사용한다:

τ(t)=(v(t)×a(t))⋅dadt(t)∣v(t)×a(t)∣2τ(2)=(24,−12,2)⋅(0,0,6)(2181)2=3181\begin{aligned}\tau(t)&=\dfrac{(\mathbf{v}(t) \times \mathbf{a}(t))\cdot\frac{\mathrm{d}\mathbf{a}}{\mathrm{d}t}(t)}{|\mathbf{v}(t) \times \mathbf{a}(t)|^2}\\ \tau(2)&=\frac{(24,-12,2)\cdot(0,0,6)}{(2\sqrt{181})^2}=\frac{3}{{181}} \end{aligned}

이 문제로 이어서 풀기
# 단위접선·법선벡터계산보통자동 분류
CLP-4 Vector Calculus CC BY-NC-SA 4.0우리말 번역: 빌드라인 스쿨 — AI 번역·자동 검토(원문과 같은 조건)

「단위접선·법선벡터」 문제 목록으로