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다변수 연쇄법칙

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

CLP-3 · 2.4절 · 24번대학 수준우리말 번역

방정식

x2−ycos⁡(uv)=vx2+y2−sin⁡(uv)=4πu\begin{aligned} x^2-y\cos(uv)&=v\\ x^2+y^2-\sin(uv)&=\frac{4}{\pi}u \end{aligned}

은 (u,v)=(π2,0)(u,v)=\big(\frac{\pi}{2},0\big) 일 때의 점 (x,y)=(1,1)(x,y)=(1,1) 근처에서 xx 와 yy 를 uu 와 vv 의 함수로 암시적으로 정의한다(즉, x=x(u,v)x=x(u,v), y=y(u,v)y=y(u,v)).

(a) (u,v)=(π2,0)(u,v)=\big(\frac{\pi}{2},0\big) 에서

∂x∂u 와 ∂y∂u\frac{\partial x}{\partial u}\text{ 와 } \frac{\partial y}{\partial u}

의 값을 구하세요. (b) z=x4+y4z=x^4+y^4 일 때, 점 (u,v)=(π2,0)(u,v)=\big(\frac{\pi}{2},0\big) 에서 ∂z∂u\frac{\partial z}{\partial u} 의 값을 구하세요.

영어 원문 보기

The equations

x2−ycos⁡(uv)=vx2+y2−sin⁡(uv)=4πu\begin{aligned} x^2-y\cos(uv)&=v\\ x^2+y^2-\sin(uv)&=\frac{4}{\pi}u \end{aligned}

define xx and yy implicitly as functions of uu and vv (i.e. x=x(u,v)x=x(u,v), and y=y(u,v)y=y(u,v)) near the point (x,y)=(1,1)(x,y)=(1,1) at which (u,v)=(π2,0)(u,v)=\big(\frac{\pi}{2},0\big).

(a) Find

∂x∂u and ∂y∂u\frac{\partial x}{\partial u}\text{ and } \frac{\partial y}{\partial u}

at (u,v)=(π2,0)(u,v)=\big(\frac{\pi}{2},0\big). (b) If z=x4+y4z=x^4+y^4, determine ∂z∂u\frac{\partial z}{\partial u} at the point (u,v)=(π2,0)(u,v)=\big(\frac{\pi}{2},0\big).

정답·풀이 보기

(a) 주어진 식은

x(u,v)2−y(u,v)cos⁡(uv)=vx(u,v)2+y(u,v)2−sin⁡(uv)=4πux(u,v)^2-y(u,v)\cos(uv)=v\qquad x(u,v)^2+y(u,v)^2-\sin(uv)=\frac{4}{\pi}u

이다. 두 방정식에 ∂∂u\frac{\partial }{\partial u} 를 적용하면

2x(u,v)∂x∂u(u,v)−∂y∂u(u,v)cos⁡(uv)+v y(u,v)sin⁡(uv)=02x(u,v)∂x∂u(u,v)+2y(u,v)∂y∂u(u,v)−vcos⁡(uv)=4π\begin{aligned} 2x(u,v)\frac{\partial x}{\partial u}(u,v) -\frac{\partial y}{\partial u}(u,v)\cos(uv)+v\,y(u,v)\sin(uv)&=0 \\ 2x(u,v)\frac{\partial x}{\partial u}(u,v) +2y(u,v)\frac{\partial y}{\partial u}(u,v) -v\cos(uv)&=\frac{4}{\pi} \end{aligned}

이다. u=π2u=\frac{\pi}{2}, v=0v=0, x(π2,0)=1x\big(\frac{\pi}{2},0\big)=1, y(π2,0)=1y\big(\frac{\pi}{2},0\big)=1 을 대입하면

2∂x∂u(π2,0)−∂y∂u(π2,0)=02∂x∂u(π2,0)+2∂y∂u(π2,0)=4π\begin{aligned} 2\frac{\partial x}{\partial u}\left(\frac{\pi}{2},0\right) -\frac{\partial y}{\partial u}\left(\frac{\pi}{2},0\right)&=0 \\[0.1in] 2\frac{\partial x}{\partial u}\left(\frac{\pi}{2},0\right) +2\frac{\partial y}{\partial u}\left(\frac{\pi}{2},0\right) &=\frac{4}{\pi} \end{aligned}

이다. 첫째 방정식에서 얻은 ∂y∂u(π2,0)=2∂x∂u(π2,0)\frac{\partial y}{\partial u}\big(\frac{\pi}{2},0\big)=2\frac{\partial x}{\partial u}\big(\frac{\pi}{2},0\big) 를 둘째 방정식에 대입하면 6∂x∂u(π2,0)=4π6\frac{\partial x}{\partial u}\big(\frac{\pi}{2},0\big)=\frac{4}{\pi} 이므로 ∂x∂u(π2,0)=23π\frac{\partial x}{\partial u}\big(\frac{\pi}{2},0\big)=\frac{2}{3\pi} 이고 ∂y∂u(π2,0)=43π\frac{\partial y}{\partial u}\big(\frac{\pi}{2},0\big)=\frac{4}{3\pi} 이다.

(b) z(u,v)=x(u,v)4+y(u,v)4z(u,v)=x(u,v)^4+y(u,v)^4 으로 주어져 있다. 따라서

∂z∂u(u,v)=4x(u,v)3 ∂x∂u(u,v)+4y(u,v)3 ∂y∂u(u,v)\begin{aligned} \frac{\partial z}{\partial u}(u,v) &=4x(u,v)^3\ \frac{\partial x}{\partial u}(u,v) +4y(u,v)^3\ \frac{\partial y}{\partial u}(u,v) \end{aligned}

이다. u=π2u=\frac{\pi}{2}, v=0v=0, x(π2,0)=1x\big(\frac{\pi}{2},0\big)=1, y(π2,0)=1y\big(\frac{\pi}{2},0\big)=1 을 대입하고 (a)의 결과를 이용하면

∂z∂u(π2,0)=4 x ⁣(π2,0)3 ∂x∂u ⁣(π2,0)+4 y ⁣(π2,0)3 ∂y∂u ⁣(π2,0)=4(23π)+4(43π)=8π\begin{aligned} \frac{\partial z}{\partial u}\left(\frac{\pi}{2},0\right) &=4\,x\!\left(\frac{\pi}{2},0\right)^3\ \frac{\partial x}{\partial u}\!\left(\frac{\pi}{2},0\right) +4\,y\!\left(\frac{\pi}{2},0\right)^3\ \frac{\partial y}{\partial u}\!\left(\frac{\pi}{2},0\right) \\ &=4\left(\frac{2}{3\pi}\right) +4\left(\frac{4}{3\pi}\right) \\ &=\frac{8}{\pi} \end{aligned}

이다.

원본 교재 풀이(영어)

(a) We are told that

x(u,v)2−y(u,v)cos⁡(uv)=vx(u,v)2+y(u,v)2−sin⁡(uv)=4πux(u,v)^2-y(u,v)\cos(uv)=v\qquad x(u,v)^2+y(u,v)^2-\sin(uv)=\frac{4}{\pi}u

Applying ∂∂u\frac{\partial }{\partial u} to both equations gives

2x(u,v)∂x∂u(u,v)−∂y∂u(u,v)cos⁡(uv)+v y(u,v)sin⁡(uv)=02x(u,v)∂x∂u(u,v)+2y(u,v)∂y∂u(u,v)−vcos⁡(uv)=4π\begin{aligned} 2x(u,v)\frac{\partial x}{\partial u}(u,v) -\frac{\partial y}{\partial u}(u,v)\cos(uv)+v\,y(u,v)\sin(uv)&=0 \\ 2x(u,v)\frac{\partial x}{\partial u}(u,v) +2y(u,v)\frac{\partial y}{\partial u}(u,v) -v\cos(uv)&=\frac{4}{\pi} \end{aligned}

Setting u=π2u=\frac{\pi}{2}, v=0v=0, x(π2,0)=1x\big(\frac{\pi}{2},0\big)=1, y(π2,0)=1y\big(\frac{\pi}{2},0\big)=1 gives

2∂x∂u(π2,0)−∂y∂u(π2,0)=02∂x∂u(π2,0)+2∂y∂u(π2,0)=4π\begin{aligned} 2\frac{\partial x}{\partial u}\left(\frac{\pi}{2},0\right) -\frac{\partial y}{\partial u}\left(\frac{\pi}{2},0\right)&=0 \\[0.1in] 2\frac{\partial x}{\partial u}\left(\frac{\pi}{2},0\right) +2\frac{\partial y}{\partial u}\left(\frac{\pi}{2},0\right) &=\frac{4}{\pi} \end{aligned}

Substituting ∂y∂u(π2,0)=2∂x∂u(π2,0)\frac{\partial y}{\partial u}\big(\frac{\pi}{2},0\big)=2\frac{\partial x}{\partial u}\big(\frac{\pi}{2},0\big), from the first equation, into the second equation gives 6∂x∂u(π2,0)=4π6\frac{\partial x}{\partial u}\big(\frac{\pi}{2},0\big)=\frac{4}{\pi} so that ∂x∂u(π2,0)=23π\frac{\partial x}{\partial u}\big(\frac{\pi}{2},0\big)=\frac{2}{3\pi} and ∂y∂u(π2,0)=43π\frac{\partial y}{\partial u}\big(\frac{\pi}{2},0\big)=\frac{4}{3\pi}.

(b) We are told that z(u,v)=x(u,v)4+y(u,v)4z(u,v)=x(u,v)^4+y(u,v)^4. So

∂z∂u(u,v)=4x(u,v)3 ∂x∂u(u,v)+4y(u,v)3 ∂y∂u(u,v)\begin{aligned} \frac{\partial z}{\partial u}(u,v) &=4x(u,v)^3\ \frac{\partial x}{\partial u}(u,v) +4y(u,v)^3\ \frac{\partial y}{\partial u}(u,v) \end{aligned}

Substituting in u=π2u=\frac{\pi}{2}, v=0v=0, x(π2,0)=1x\big(\frac{\pi}{2},0\big)=1, y(π2,0)=1y\big(\frac{\pi}{2},0\big)=1 and using the results of part (a),

∂z∂u(π2,0)=4 x ⁣(π2,0)3 ∂x∂u ⁣(π2,0)+4 y ⁣(π2,0)3 ∂y∂u ⁣(π2,0)=4(23π)+4(43π)=8π\begin{aligned} \frac{\partial z}{\partial u}\left(\frac{\pi}{2},0\right) &=4\,x\!\left(\frac{\pi}{2},0\right)^3\ \frac{\partial x}{\partial u}\!\left(\frac{\pi}{2},0\right) +4\,y\!\left(\frac{\pi}{2},0\right)^3\ \frac{\partial y}{\partial u}\!\left(\frac{\pi}{2},0\right) \\ &=4\left(\frac{2}{3\pi}\right) +4\left(\frac{4}{3\pi}\right) \\ &=\frac{8}{\pi} \end{aligned}

한 번 더 — 비슷한 문제CLP-3 · 2.4절 · 15번우리말 번역

z=f(x,y)z = f (x, y) 가 연속인 이계 편도함수를 갖고, x=rcos⁡tx = r \cos t, y=rsin⁡ty = r \sin t 라 하자. 다음 편도함수를 rr, tt, 그리고 ff 의 편도함수로 나타내세요.

(a) ∂z∂t\frac{\partial z}{\partial t} (b) ∂2z∂t2\frac{\partial^2 z}{\partial t^2}

다 풀었으면 정답 확인

정의에 의해 z(r,t)=f(rcos⁡t , rsin⁡t)z(r,t) = f(r\cos t\,,\,r\sin t) 이다.

(a) 연쇄 법칙에 의해

∂z∂t(r,t)=∂∂t[f(rcos⁡t , rsin⁡t)]=∂f∂x(rcos⁡t , rsin⁡t)∂∂t(rcos⁡t)+∂f∂y(rcos⁡t , rsin⁡t)∂∂t(rsin⁡t)=−rsin⁡t ∂f∂x(rcos⁡t , rsin⁡t)+rcos⁡t ∂f∂y(rcos⁡t , rsin⁡t)\begin{aligned} \frac{\partial z}{\partial t}(r,t) &= \frac{\partial }{\partial t}\Big[f(r\cos t\,,\,r\sin t)\Big] \\ &= \frac{\partial f}{\partial x}(r\cos t\,,\,r\sin t)\frac{\partial }{\partial t}(r\cos t) +\frac{\partial f}{\partial y}(r\cos t\,,\,r\sin t)\frac{\partial }{\partial t}(r\sin t) \\ &= -r\sin t\ \frac{\partial f}{\partial x}(r\cos t\,,\,r\sin t) +r\cos t\ \frac{\partial f}{\partial y}(r\cos t\,,\,r\sin t) \end{aligned}

(b) 선형성, 곱의 미분법, 연쇄 법칙에 의해

∂2z∂t2(r,t)=−∂∂t[rsin⁡t ∂f∂x(rcos⁡t , rsin⁡t)]+∂∂t[rcos⁡t ∂f∂y(rcos⁡t , rsin⁡t)]=−rcos⁡t ∂f∂x(rcos⁡t , rsin⁡t)−rsin⁡t ∂∂t[∂f∂x(rcos⁡t , rsin⁡t)]−rsin⁡t ∂f∂y(rcos⁡t , rsin⁡t)+rcos⁡t ∂∂t[∂f∂y(rcos⁡t , rsin⁡t)]=−rcos⁡t ∂f∂x(rcos⁡t , rsin⁡t)+r2sin⁡2t ∂2f∂x2(rcos⁡t , rsin⁡t)−r2sin⁡tcos⁡t ∂2 f∂y∂x(rcos⁡t , rsin⁡t)=−rsin⁡t ∂f∂y(rcos⁡t , rsin⁡t)−r2sin⁡tcos⁡t ∂2 f∂x∂y(rcos⁡t , rsin⁡t)+r2cos⁡2t ∂2f∂y2(rcos⁡t , rsin⁡t)=−rcos⁡t ∂f∂x−rsin⁡t ∂f∂y+r2sin⁡2t ∂2f∂x2−2r2sin⁡tcos⁡t ∂2 f∂x∂y+r2cos⁡2t ∂2f∂y2\begin{aligned} \frac{\partial^2 z}{\partial t^2}(r,t) &= -\frac{\partial }{\partial t}\left[r\sin t\ \frac{\partial f}{\partial x}(r\cos t\,,\,r\sin t)\right] +\frac{\partial }{\partial t}\left[r\cos t\ \frac{\partial f}{\partial y}(r\cos t\,,\,r\sin t)\right] \\ &= -r\cos t\ \frac{\partial f}{\partial x}(r\cos t\,,\,r\sin t) -r\sin t\ \frac{\partial }{\partial t}\left[\frac{\partial f}{\partial x}(r\cos t\,,\,r\sin t)\right] \\ & -r\sin t\ \frac{\partial f}{\partial y}(r\cos t\,,\,r\sin t) +r\cos t\ \frac{\partial }{\partial t}\left[\frac{\partial f}{\partial y}(r\cos t\,,\,r\sin t)\right] \\ &= -r\cos t \ \frac{\partial f}{\partial x}(r\cos t\,,\,r\sin t) \\ & +r^2\sin^2 t\ \frac{\partial^2 f}{\partial x^2}(r\cos t\,,\,r\sin t) -r^2\sin t\cos t\ \frac{\partial^2\ f}{\partial y\partial x}(r\cos t\,,\,r\sin t) \\ &\phantom{=}-r\sin t \ \frac{\partial f}{\partial y}(r\cos t\,,\,r\sin t) \\ & -r^2\sin t\cos t\ \frac{\partial^2\ f}{\partial x\partial y}(r\cos t\,,\,r\sin t) +r^2\cos^2 t\ \frac{\partial^2 f}{\partial y^2}(r\cos t\,,\,r\sin t) \\ &= -r\cos t \ \frac{\partial f}{\partial x} -r\sin t \ \frac{\partial f}{\partial y} \\ & +r^2\sin^2 t\ \frac{\partial^2 f}{\partial x^2} -2r^2\sin t\cos t\ \frac{\partial^2\ f}{\partial x\partial y} +r^2\cos^2 t\ \frac{\partial^2 f}{\partial y^2} \end{aligned}

여기서 ff 의 모든 편도함수는 (rcos⁡t , rsin⁡t)(r\cos t\,,\,r\sin t) 에서의 값이다.

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