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다변수 미분 전체 문제

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98문제 · 2 / 5쪽

21.CLP-3 · 2.4절 · 13번대학 수준우리말 번역

f(x)f(x) 와 g(x)g(x) 가 xx 에 대한 두 함수이고 f′′(7)=−2f''(7) = -2 이고 g′′(−4)=−1g''(-4) = -1 을 만족시킨다고 하자. z=h(s,t)=f(2s+3t)+g(s−6t)z = h(s,t) = f(2s + 3t) + g(s - 6t) 가 ss 와 tt 에 대한 함수일 때, s=2s = 2 이고 t=1t = 1 일 때 ∂2z∂t2\frac{\partial^2 z}{\partial t^2} 의 값을 구하세요.

영어 원문 보기

Let f(x)f(x) and g(x)g(x) be two functions of xx satisfying f′′(7)=−2f''(7) = -2 and g′′(−4)=−1g''(-4) = -1. If z=h(s,t)=f(2s+3t)+g(s−6t)z = h(s,t) = f(2s + 3t) + g(s - 6t) is a function of ss and tt, find the value of ∂2z∂t2\frac{\partial^2 z}{\partial t^2} when s=2s = 2 and t=1t = 1.

답 쓰고 채점
정답·풀이 보기

연쇄 법칙에 의해

∂h∂t(s,t)=∂∂t[f(2s+3t)]+∂∂t[g(s−6t)]=f′(2s+3t)∂∂t(2s+3t)+g(s−6t)∂∂t(s−6t)=3f′(2s+3t)−6g′(s−6t)∂2h∂t2(s,t)=3∂∂t[f′(2s+3t)]−6∂∂t[g′(s−6t)]=3 f′′(2s+3t)∂∂t(2s+3t)−6 g′′(s−6t)∂∂t(s−6t)=9f′′(2s+3t)+36g′′(s−6t)\begin{aligned} \frac{\partial h}{\partial t}(s,t) &=\frac{\partial }{\partial t}\big[f(2s + 3t)\big] + \frac{\partial }{\partial t}\big[g(s - 6t)\big] \\ &=f'(2s + 3t)\frac{\partial }{\partial t}(2s+3t) + g(s - 6t)\frac{\partial }{\partial t}(s-6t) \\ &= 3f'(2s + 3t) - 6g'(s - 6t) \\ \frac{\partial^2 h}{\partial t^2}(s,t) &= 3\frac{\partial }{\partial t}\big[f'(2s + 3t)\big] - 6\frac{\partial }{\partial t}\big[ g'(s - 6t) \big] \\ &= 3\,f''(2s + 3t)\frac{\partial }{\partial t}(2s+3t) - 6\,g''(s - 6t) \frac{\partial }{\partial t}(s-6t) \\ &= 9f''(2s+3t) + 36g''(s-6t) \end{aligned}

특히

∂2h∂t2(2,1)=9f′′(7)+36g′′(−4)=9(−2)+36(−1)=−54\begin{aligned} \frac{\partial^2 h}{\partial t^2}(2,1) =9f''(7) +36g''(-4) =9(-2) +36(-1) =-54 \end{aligned}

이다.

원본 교재 풀이(영어)

By the chain rule,

∂h∂t(s,t)=∂∂t[f(2s+3t)]+∂∂t[g(s−6t)]=f′(2s+3t)∂∂t(2s+3t)+g(s−6t)∂∂t(s−6t)=3f′(2s+3t)−6g′(s−6t)∂2h∂t2(s,t)=3∂∂t[f′(2s+3t)]−6∂∂t[g′(s−6t)]=3 f′′(2s+3t)∂∂t(2s+3t)−6 g′′(s−6t)∂∂t(s−6t)=9f′′(2s+3t)+36g′′(s−6t)\begin{aligned} \frac{\partial h}{\partial t}(s,t) &=\frac{\partial }{\partial t}\big[f(2s + 3t)\big] + \frac{\partial }{\partial t}\big[g(s - 6t)\big] \\ &=f'(2s + 3t)\frac{\partial }{\partial t}(2s+3t) + g(s - 6t)\frac{\partial }{\partial t}(s-6t) \\ &= 3f'(2s + 3t) - 6g'(s - 6t) \\ \frac{\partial^2 h}{\partial t^2}(s,t) &= 3\frac{\partial }{\partial t}\big[f'(2s + 3t)\big] - 6\frac{\partial }{\partial t}\big[ g'(s - 6t) \big] \\ &= 3\,f''(2s + 3t)\frac{\partial }{\partial t}(2s+3t) - 6\,g''(s - 6t) \frac{\partial }{\partial t}(s-6t) \\ &= 9f''(2s+3t) + 36g''(s-6t) \end{aligned}

In particular

∂2h∂t2(2,1)=9f′′(7)+36g′′(−4)=9(−2)+36(−1)=−54\begin{aligned} \frac{\partial^2 h}{\partial t^2}(2,1) =9f''(7) +36g''(-4) =9(-2) +36(-1) =-54 \end{aligned}

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 12번
# 다변수 연쇄법칙계산보통자동 분류
22.CLP-3 · 2.4절 · 14번대학 수준우리말 번역

w=f(xz,yz)w = f (xz, yz) 라고 하자. 여기서 ff 는 미분가능한 함수이다. 다음을 보여라.

x∂w∂x+y∂w∂y=z∂w∂zx\frac{\partial w}{\partial x} + y\frac{\partial w}{\partial y} = z\frac{\partial w}{\partial z}

영어 원문 보기

Suppose that w=f(xz,yz)w = f (xz, yz), where ff is a differentiable function. Show that

x∂w∂x+y∂w∂y=z∂w∂zx\frac{\partial w}{\partial x} + y\frac{\partial w}{\partial y} = z\frac{\partial w}{\partial z}

정답·풀이 보기

먼저 w(x,y,z)w(x,y,z) 의 1계 편도함수를 구한다. u(x,y,z)=xzu(x,y,z)=xz, v(x,y,z)=yzv(x,y,z)=yz 라 하면 w(x,y,z)=f(u(x,y,z),v(x,y,z))w(x,y,z) = f\big(u(x,y,z), v(x,y,z)\big) 이다. 연쇄 법칙에 의해

∂w∂x(x,y,z)=∂∂x[f(u(x,y,z),v(x,y,z))]=∂f∂u(u(x,y,z),v(x,y,z))∂u∂x(x,y,z)+∂f∂v(u(x,y,z),v(x,y,z))∂v∂x(x,y,z)=z∂f∂u(xz,yz)∂w∂y(x,y,z)=∂∂y[f(u(x,y,z),v(x,y,z))]=∂f∂u(u(x,y,z),v(x,y,z))∂u∂y(x,y,z)+∂f∂v(u(x,y,z),v(x,y,z))∂v∂y(x,y,z)=z∂f∂v(xz,yz)∂w∂z(x,y,z)=∂∂z[f(u(x,y,z),v(x,y,z))]=∂f∂u(u(x,y,z),v(x,y,z))∂u∂z(x,y,z)+∂f∂v(u(x,y,z),v(x,y,z))∂v∂z(x,y,z)=x∂f∂u(xz,yz)+y∂f∂v(xz,yz)\begin{aligned} \frac{\partial w}{\partial x}(x,y,z) &= \frac{\partial }{\partial x}\big[f \big(u(x,y,z), v(x,y,z)\big)\big]\\ &=\frac{\partial f}{\partial u}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial u}{\partial x}(x,y,z) +\frac{\partial f}{\partial v}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial v}{\partial x}(x,y,z) \\ &=z\frac{\partial f}{\partial u}(xz, yz) \\ \frac{\partial w}{\partial y}(x,y,z) &= \frac{\partial }{\partial y}\big[f \big(u(x,y,z), v(x,y,z)\big)\big]\\ &=\frac{\partial f}{\partial u}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial u}{\partial y}(x,y,z) +\frac{\partial f}{\partial v}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial v}{\partial y}(x,y,z) \\ &=z\frac{\partial f}{\partial v}(xz, yz) \\ \frac{\partial w}{\partial z}(x,y,z) &= \frac{\partial }{\partial z}\big[f \big(u(x,y,z), v(x,y,z)\big)\big]\\ &=\frac{\partial f}{\partial u}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial u}{\partial z}(x,y,z) +\frac{\partial f}{\partial v}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial v}{\partial z}(x,y,z) \\ &=x\frac{\partial f}{\partial u}(xz, yz) + y\frac{\partial f}{\partial v}(xz, yz) \end{aligned}

따라서

x∂w∂x+y∂w∂y=xz∂f∂u(xz,yz)+yz∂f∂v(xz,yz)=z[x∂f∂u(xz,yz)+y∂f∂v(xz,yz)]=z∂w∂z\begin{aligned} x\frac{\partial w}{\partial x} + y\frac{\partial w}{\partial y} =xz\frac{\partial f}{\partial u}(xz, yz) + yz\frac{\partial f}{\partial v}(xz, yz) =z\left[x\frac{\partial f}{\partial u}(xz, yz) + y\frac{\partial f}{\partial v}(xz, yz)\right] =z\frac{\partial w}{\partial z} \end{aligned}

이므로 주어진 등식이 성립한다.

원본 교재 풀이(영어)

We'll first compute the first order partial derivatives of w(x,y,z)w(x,y,z). Write u(x,y,z)=xzu(x,y,z)=xz and v(x,y,z)=yzv(x,y,z)=yz so that w(x,y,z)=f(u(x,y,z),v(x,y,z))w(x,y,z) = f\big(u(x,y,z), v(x,y,z)\big). By the chain rule,

∂w∂x(x,y,z)=∂∂x[f(u(x,y,z),v(x,y,z))]=∂f∂u(u(x,y,z),v(x,y,z))∂u∂x(x,y,z)+∂f∂v(u(x,y,z),v(x,y,z))∂v∂x(x,y,z)=z∂f∂u(xz,yz)∂w∂y(x,y,z)=∂∂y[f(u(x,y,z),v(x,y,z))]=∂f∂u(u(x,y,z),v(x,y,z))∂u∂y(x,y,z)+∂f∂v(u(x,y,z),v(x,y,z))∂v∂y(x,y,z)=z∂f∂v(xz,yz)∂w∂z(x,y,z)=∂∂z[f(u(x,y,z),v(x,y,z))]=∂f∂u(u(x,y,z),v(x,y,z))∂u∂z(x,y,z)+∂f∂v(u(x,y,z),v(x,y,z))∂v∂z(x,y,z)=x∂f∂u(xz,yz)+y∂f∂v(xz,yz)\begin{aligned} \frac{\partial w}{\partial x}(x,y,z) &= \frac{\partial }{\partial x}\big[f \big(u(x,y,z), v(x,y,z)\big)\big]\\ &=\frac{\partial f}{\partial u}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial u}{\partial x}(x,y,z) +\frac{\partial f}{\partial v}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial v}{\partial x}(x,y,z) \\ &=z\frac{\partial f}{\partial u}(xz, yz) \\ \frac{\partial w}{\partial y}(x,y,z) &= \frac{\partial }{\partial y}\big[f \big(u(x,y,z), v(x,y,z)\big)\big]\\ &=\frac{\partial f}{\partial u}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial u}{\partial y}(x,y,z) +\frac{\partial f}{\partial v}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial v}{\partial y}(x,y,z) \\ &=z\frac{\partial f}{\partial v}(xz, yz) \\ \frac{\partial w}{\partial z}(x,y,z) &= \frac{\partial }{\partial z}\big[f \big(u(x,y,z), v(x,y,z)\big)\big]\\ &=\frac{\partial f}{\partial u}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial u}{\partial z}(x,y,z) +\frac{\partial f}{\partial v}\big(u(x,y,z), v(x,y,z)\big)\frac{\partial v}{\partial z}(x,y,z) \\ &=x\frac{\partial f}{\partial u}(xz, yz) + y\frac{\partial f}{\partial v}(xz, yz) \end{aligned}

So

x∂w∂x+y∂w∂y=xz∂f∂u(xz,yz)+yz∂f∂v(xz,yz)=z[x∂f∂u(xz,yz)+y∂f∂v(xz,yz)]=z∂w∂z\begin{aligned} x\frac{\partial w}{\partial x} + y\frac{\partial w}{\partial y} =xz\frac{\partial f}{\partial u}(xz, yz) + yz\frac{\partial f}{\partial v}(xz, yz) =z\left[x\frac{\partial f}{\partial u}(xz, yz) + y\frac{\partial f}{\partial v}(xz, yz)\right] =z\frac{\partial w}{\partial z} \end{aligned}

as desired.

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 22번
# 다변수 연쇄법칙증명·논술보통자동 분류
23.CLP-3 · 2.4절 · 15번대학 수준우리말 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}

영어 원문 보기

Suppose z=f(x,y)z = f (x, y) has continuous second order partial derivatives, and x=rcos⁡tx = r \cos t, y=rsin⁡ty = r \sin t. Express the following partial derivatives in terms rr, tt, and partial derivatives of ff.

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

정답·풀이 보기

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.

원본 교재 풀이(영어)

By definition z(r,t)=f(rcos⁡t , rsin⁡t)z(r,t) = f(r\cos t\,,\,r\sin t).

(a) By the chain rule

∂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) By linearity, the product rule and the chain rule

∂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}

with all of the partial derivatives of ff evaluated at (rcos⁡t , rsin⁡t)(r\cos t\,,\,r\sin t).

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 25번
# 다변수 연쇄법칙활용보통자동 분류
24.CLP-3 · 2.4절 · 16번대학 수준우리말 번역

z=f(x,y)z = f(x, y) 라 하자. 여기서 f(x,y)f(x, y) 는 연속인 이계 편도함수를 가지며,

fx(2,1)=5,fy(2,1)=−2,fxx(2,1)=2,fxy(2,1)=1,fyy(2,1)=−4f_x (2, 1) = 5, \qquad f_y(2, 1) =-2, \qquad f_{xx}(2, 1) = 2,\qquad f_{xy}(2, 1) = 1, \qquad f_{yy}(2, 1) = -4

이다.

x(t)=2t2x(t)=2t^2, y(t)=t3y(t)=t^3 이고 t=1t=1 일 때, d2dt2z(x(t),y(t)) \frac{\mathrm{d^2}}{\mathrm{d}{t}^2} z\big(x(t),y(t)\big) 의 값을 구하세요.

영어 원문 보기

Let z=f(x,y)z = f(x, y), where f(x,y)f(x, y) has continuous second-order partial derivatives, and

fx(2,1)=5,fy(2,1)=−2,fxx(2,1)=2,fxy(2,1)=1,fyy(2,1)=−4f_x (2, 1) = 5, \qquad f_y(2, 1) =-2, \qquad f_{xx}(2, 1) = 2,\qquad f_{xy}(2, 1) = 1, \qquad f_{yy}(2, 1) = -4

Find d2dt2z(x(t),y(t)) \frac{\mathrm{d^2}}{\mathrm{d}{t}^2} z\big(x(t),y(t)\big) when x(t)=2t2x(t)=2t^2, y(t)=t3y(t)=t^3 and t=1t=1.

답 쓰고 채점
정답·풀이 보기

x(t)=2t2x(t)=2t^2, y(t)=t3y(t)=t^3 에 대해 w(t)=z(x(t),y(t))=f(x(t),y(t))w(t) = z\big(x(t),y(t)\big) = f\big(x(t),y(t)\big) 라 하자. d2wdt2(1)\frac{\mathrm{d^2}w}{\mathrm{d}{t}^2}(1) 을 계산하면 된다. 연쇄 법칙에 의해

dwdt(t)=ddtf(x(t),y(t))=fx(x(t) , y(t)) dxdt(t)+fy(x(t) , y(t)) dydt(t)=4t fx(x(t) , y(t))+3t2 fy(x(t) , y(t))\begin{aligned} \frac{\mathrm{d}w}{\mathrm{d}t}(t)&= \frac{\mathrm{d}}{\mathrm{d}t} f\big(x(t),y(t)\big) \\ &= f_x(x(t)\,,\,y(t))\,\frac{\mathrm{d}x}{\mathrm{d}t}(t) +f_y(x(t)\,,\,y(t))\,\frac{\mathrm{d}y}{\mathrm{d}t}(t) \\ &= 4t\,f_x(x(t)\,,\,y(t)) +3t^2\,f_y(x(t)\,,\,y(t)) \end{aligned}

이다. 선형성, 곱의 미분법, 연쇄 법칙에 의해

d2dt2f(x(t),y(t))=ddt[4t fx(x(t),y(t))]+ddt[3t2 fy(x(t),y(t))]=4 fx(x(t),y(t))+4tddt[fx(x(t),y(t))]+6t fy(x(t),y(t))+3t2ddt[fy(x(t),y(t))]=4 fx(2t2 , t3)+4t[fxx(x(t),y(t)) dxdt(t)+fxy(x(t),y(t)) dydt(t)]=+6t fy(2t2 , t3)+3t2[fyx(x(t),y(t)) dxdt(t)+fyy(x(t),y(t)) dydt(t)]=4 fx(2t2 , t3)+16t2 fxx(2t2 , t3)+12t3 fxy(2t2 , t3)=+6t fy(2t2 , t3)+12t3 fyx(2t2 , t3)+9t4 fyy(2t2 , t3)\begin{aligned} \frac{\mathrm{d^2}}{\mathrm{d}{t}^2} f\big(x(t),y(t)\big) &= \frac{\mathrm{d}}{\mathrm{d}t}\left[4t\,f_x\big(x(t),y(t)\big) \right] +\frac{\mathrm{d}}{\mathrm{d}t}\left[3t^2\,f_y\big(x(t),y(t)\big) \right] \\ &= 4\,f_x\big(x(t),y(t)\big) + 4t \frac{\mathrm{d}}{\mathrm{d}t}\left[f_x\big(x(t),y(t)\big) \right] \\& +6t\,f_y\big(x(t),y(t)\big) + 3t^2\frac{\mathrm{d}}{\mathrm{d}t}\left[f_y\big(x(t),y(t)\big) \right] \\ &= 4\,f_x(2t^2\,,\,t^3) + 4t\Big[f_{xx}\big(x(t),y(t)\big)\,\frac{\mathrm{d}x}{\mathrm{d}t}(t) + f_{xy}\big(x(t),y(t)\big)\,\frac{\mathrm{d}y}{\mathrm{d}t}(t)\Big] \\ &\phantom{=} + 6t\,f_y(2t^2\,,\,t^3) + 3t^2\Big[f_{yx}\big(x(t),y(t)\big)\,\frac{\mathrm{d}x}{\mathrm{d}t}(t) + f_{yy}\big(x(t),y(t)\big)\,\frac{\mathrm{d}y}{\mathrm{d}t}(t)\Big] \\ &= 4\,f_x(2t^2\,,\,t^3) + 16t^2\,f_{xx}(2t^2\,,\,t^3) + 12t^3\,f_{xy}(2t^2\,,\,t^3) \\ &\phantom{=} + 6t\,f_y(2t^2\,,\,t^3) + 12t^3\,f_{yx}(2t^2\,,\,t^3) + 9t^4\,f_{yy}(2t^2\,,\,t^3) \end{aligned}

이다. 특히 t=1t=1 일 때, fxy(2,1)=fyx(2,1)f_{xy}(2, 1)=f_{yx}(2, 1) 이므로

d2dt2f(x(t),y(t))∣t=1=4 (5)+16 (2)+12 (1)=+6 (−2)+12 (1)+9 (−4)=28\begin{aligned} \left.\frac{\mathrm{d^2}}{\mathrm{d}{t}^2} f\big(x(t),y(t)\big) \right|_{t=1} &= 4\,(5) + 16\,(2) + 12\,(1) \\ &\phantom{=} + 6\,(-2) + 12\,(1) + 9\,(-4) \\ &=28 \end{aligned}

이다.

원본 교재 풀이(영어)

Write w(t)=z(x(t),y(t))=f(x(t),y(t))w(t) = z\big(x(t),y(t)\big) = f\big(x(t),y(t)\big) with x(t)=2t2x(t)=2t^2, y(t)=t3y(t)=t^3. We are to compute d2wdt2(1)\frac{\mathrm{d^2}w}{\mathrm{d}{t}^2}(1). By the chain rule

dwdt(t)=ddtf(x(t),y(t))=fx(x(t) , y(t)) dxdt(t)+fy(x(t) , y(t)) dydt(t)=4t fx(x(t) , y(t))+3t2 fy(x(t) , y(t))\begin{aligned} \frac{\mathrm{d}w}{\mathrm{d}t}(t)&= \frac{\mathrm{d}}{\mathrm{d}t} f\big(x(t),y(t)\big) \\ &= f_x(x(t)\,,\,y(t))\,\frac{\mathrm{d}x}{\mathrm{d}t}(t) +f_y(x(t)\,,\,y(t))\,\frac{\mathrm{d}y}{\mathrm{d}t}(t) \\ &= 4t\,f_x(x(t)\,,\,y(t)) +3t^2\,f_y(x(t)\,,\,y(t)) \end{aligned}

By linearity, the product rule, and the chain rule,

d2dt2f(x(t),y(t))=ddt[4t fx(x(t),y(t))]+ddt[3t2 fy(x(t),y(t))]=4 fx(x(t),y(t))+4tddt[fx(x(t),y(t))]+6t fy(x(t),y(t))+3t2ddt[fy(x(t),y(t))]=4 fx(2t2 , t3)+4t[fxx(x(t),y(t)) dxdt(t)+fxy(x(t),y(t)) dydt(t)]=+6t fy(2t2 , t3)+3t2[fyx(x(t),y(t)) dxdt(t)+fyy(x(t),y(t)) dydt(t)]=4 fx(2t2 , t3)+16t2 fxx(2t2 , t3)+12t3 fxy(2t2 , t3)=+6t fy(2t2 , t3)+12t3 fyx(2t2 , t3)+9t4 fyy(2t2 , t3)\begin{aligned} \frac{\mathrm{d^2}}{\mathrm{d}{t}^2} f\big(x(t),y(t)\big) &= \frac{\mathrm{d}}{\mathrm{d}t}\left[4t\,f_x\big(x(t),y(t)\big) \right] +\frac{\mathrm{d}}{\mathrm{d}t}\left[3t^2\,f_y\big(x(t),y(t)\big) \right] \\ &= 4\,f_x\big(x(t),y(t)\big) + 4t \frac{\mathrm{d}}{\mathrm{d}t}\left[f_x\big(x(t),y(t)\big) \right] \\& +6t\,f_y\big(x(t),y(t)\big) + 3t^2\frac{\mathrm{d}}{\mathrm{d}t}\left[f_y\big(x(t),y(t)\big) \right] \\ &= 4\,f_x(2t^2\,,\,t^3) + 4t\Big[f_{xx}\big(x(t),y(t)\big)\,\frac{\mathrm{d}x}{\mathrm{d}t}(t) + f_{xy}\big(x(t),y(t)\big)\,\frac{\mathrm{d}y}{\mathrm{d}t}(t)\Big] \\ &\phantom{=} + 6t\,f_y(2t^2\,,\,t^3) + 3t^2\Big[f_{yx}\big(x(t),y(t)\big)\,\frac{\mathrm{d}x}{\mathrm{d}t}(t) + f_{yy}\big(x(t),y(t)\big)\,\frac{\mathrm{d}y}{\mathrm{d}t}(t)\Big] \\ &= 4\,f_x(2t^2\,,\,t^3) + 16t^2\,f_{xx}(2t^2\,,\,t^3) + 12t^3\,f_{xy}(2t^2\,,\,t^3) \\ &\phantom{=} + 6t\,f_y(2t^2\,,\,t^3) + 12t^3\,f_{yx}(2t^2\,,\,t^3) + 9t^4\,f_{yy}(2t^2\,,\,t^3) \end{aligned}

In particular, when t=1t=1, and since fxy(2,1)=fyx(2,1)f_{xy}(2, 1)=f_{yx}(2, 1),

d2dt2f(x(t),y(t))∣t=1=4 (5)+16 (2)+12 (1)=+6 (−2)+12 (1)+9 (−4)=28\begin{aligned} \left.\frac{\mathrm{d^2}}{\mathrm{d}{t}^2} f\big(x(t),y(t)\big) \right|_{t=1} &= 4\,(5) + 16\,(2) + 12\,(1) \\ &\phantom{=} + 6\,(-2) + 12\,(1) + 9\,(-4) \\ &=28 \end{aligned}

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 24번
# 다변수 연쇄법칙활용보통자동 분류
25.CLP-3 · 2.4절 · 17번대학 수준우리말 번역

함수 F(x,y,z)F(x,y,z) 가 등식 ∂F∂z=∂2F∂x2+∂2F∂y2\frac{\partial F}{\partial z} = \frac{\partial^2 F}{\partial x^2} + \frac{\partial^2 F}{\partial y^2} 을 만족시키고, 혼합 편도함수 ∂2F∂x∂y\frac{\partial^2 F}{\partial x \partial y} 와 ∂2F∂y∂x\frac{\partial^2 F}{\partial y \partial x} 가 서로 같다고 하자. AA 를 어떤 상수라 하고 G(γ,s,t)=F(γ+s,γ−s,At)G(\gamma, s, t) = F (\gamma + s, \gamma-s, At) 라 하자. ∂G∂t=∂2G∂γ2+∂2G∂s2\frac{\partial G}{\partial t} = \frac{\partial^2 G}{\partial \gamma^2} + \frac{\partial^2 G}{\partial s^2} 이 되도록 하는 AA 의 값을 구하세요.

영어 원문 보기

Assume that the function F(x,y,z)F(x,y,z) satisfies the equation ∂F∂z=∂2F∂x2+∂2F∂y2\frac{\partial F}{\partial z} = \frac{\partial^2 F}{\partial x^2} + \frac{\partial^2 F}{\partial y^2} and the mixed partial derivatives ∂2F∂x∂y\frac{\partial^2 F}{\partial x \partial y} and ∂2F∂y∂x\frac{\partial^2 F}{\partial y \partial x} are equal. Let AA be some constant and let G(γ,s,t)=F(γ+s,γ−s,At)G(\gamma, s, t) = F (\gamma + s, \gamma-s, At). Find the value of AA such that ∂G∂t=∂2G∂γ2+∂2G∂s2\frac{\partial G}{\partial t} = \frac{\partial^2 G}{\partial \gamma^2} + \frac{\partial^2 G}{\partial s^2}.

답 쓰고 채점
정답·풀이 보기

연쇄 법칙에 의해

∂G∂t(γ,s,t)=∂∂t[F(γ+s,γ−s,At)]=∂F∂x(γ+s,γ−s,At) ∂∂t(γ+s)+∂F∂y(γ+s,γ−s,At) ∂∂t(γ−s)+∂F∂z(γ+s,γ−s,At) ∂∂t(At)=A ∂F∂z(γ+s,γ−s,At)\begin{aligned} \frac{\partial G}{\partial t}(\gamma ,s,t) &= \frac{\partial }{\partial t} \Big[F (\gamma + s, \gamma-s, At)\Big] \\ &=\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial t}(\gamma + s) +\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial t}(\gamma - s) \\& +\frac{\partial F}{\partial z}(\gamma + s, \gamma-s, At)\,\frac{\partial }{\partial t}(At) \\ &= A\,\frac{\partial F}{\partial z}(\gamma + s, \gamma-s, At) \end{aligned}

이고

∂G∂γ(γ,s,t)=∂∂γ[F(γ+s,γ−s,At)]=∂F∂x(γ+s,γ−s,At) ∂∂γ(γ+s)+∂F∂y(γ+s,γ−s,At) ∂∂γ(γ−s)+∂F∂z(γ+s,γ−s,At) ∂∂γ(At)=∂F∂x(γ+s,γ−s,At)+∂F∂y(γ+s,γ−s,At)(E1)\begin{aligned} \frac{\partial G}{\partial \gamma }(\gamma ,s,t) &= \frac{\partial }{\partial \gamma } \Big[F (\gamma + s, \gamma-s, At)\Big] \\ &=\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial \gamma }(\gamma + s) +\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial \gamma }(\gamma - s) \\& +\frac{\partial F}{\partial z}(\gamma + s, \gamma-s, At)\,\frac{\partial }{\partial \gamma }(At) \\ &= \frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At) +\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \tag{E1} \end{aligned}

이고

∂G∂s(γ,s,t)=∂∂s[F(γ+s,γ−s,At)]=∂F∂x(γ+s,γ−s,At) ∂∂s(γ+s)+∂F∂y(γ+s,γ−s,At) ∂∂s(γ−s)+∂F∂z(γ+s,γ−s,At) ∂∂s(At)=∂F∂x(γ+s,γ−s,At)−∂F∂y(γ+s,γ−s,At)(E2)\begin{aligned} \frac{\partial G}{\partial s}(\gamma ,s,t) &= \frac{\partial }{\partial s} \Big[F (\gamma + s, \gamma-s, At)\Big] \\ &=\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial s}(\gamma + s) +\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial s}(\gamma - s) \\& +\frac{\partial F}{\partial z}(\gamma + s, \gamma-s, At)\,\frac{\partial }{\partial s}(At) \\ &= \frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At) -\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \tag{E2} \end{aligned}

이다.

다음 식의 우변에 있는 네 항에 연쇄 법칙을 적용하면 이계도함수를 구할 수 있다.

∂2G∂γ2(γ,s,t)=∂∂γ[∂G∂γ(γ,s,t)]=∂∂γ[∂F∂x(γ+s,γ−s,At)]+∂∂γ[∂F∂y(γ+s,γ−s,At)]∂2G∂s2(γ,s,t)=∂∂s[∂G∂s(γ,s,t)]=∂∂s[∂F∂x(γ+s,γ−s,At)]−∂∂s[∂F∂y(γ+s,γ−s,At)]\begin{aligned} \frac{\partial^2G}{\partial\gamma ^2}(\gamma ,s,t) &=\frac{\partial }{\partial \gamma }\Big[\frac{\partial G}{\partial \gamma }(\gamma , s, t)\Big] = \frac{\partial }{\partial \gamma }\Big[\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\Big] + \frac{\partial }{\partial \gamma }\Big[\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \Big] \\ \frac{\partial^2G}{\partial s^2}(\gamma ,s,t) &=\frac{\partial }{\partial s}\Big[\frac{\partial G}{\partial s}(\gamma , s, t)\Big] = \frac{\partial }{\partial s}\Big[\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\Big] - \frac{\partial }{\partial s}\Big[\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \Big] \end{aligned}

다른 방법으로, (E1)과 (E2)에서 FF 를 ∂F∂x\frac{\partial F}{\partial x} 로 바꾸면 다음을 얻는다.

∂∂γ[∂F∂x(γ+s,γ−s,At)]=∂2F∂x2(γ+s,γ−s,At)+∂2F∂y∂x(γ+s,γ−s,At)∂∂s[∂F∂x(γ+s,γ−s,At)]=∂2F∂x2(γ+s,γ−s,At)−∂2F∂y∂x(γ+s,γ−s,At)\begin{aligned} \frac{\partial }{\partial \gamma }\Big[\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\Big] &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) \\ \frac{\partial }{\partial s}\Big[\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At) \Big] &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) -\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) \end{aligned}

(E1)과 (E2)에서 FF 를 ∂F∂y\frac{\partial F}{\partial y} 로 바꾸면 다음을 얻는다.

∂∂γ[∂F∂y(γ+s,γ−s,At)]=∂2F∂x∂y(γ+s,γ−s,At)+∂2F∂y2(γ+s,γ−s,At)∂∂s[∂F∂y(γ+s,γ−s,At)]=∂2F∂x∂y(γ+s,γ−s,At)−∂2F∂y2(γ+s,γ−s,At)\begin{aligned} \frac{\partial }{\partial \gamma }\Big[\frac{\partial F}{\partial y}(\gamma + s, \gamma-s,At)\Big] &= \frac{\partial^2 F}{\partial x\partial y}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s,At) \\ \frac{\partial }{\partial s}\Big[\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \Big] &= \frac{\partial^2 F}{\partial x\partial y}(\gamma + s, \gamma-s, At) -\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At) \end{aligned}

따라서

∂2G∂γ2(γ,s,t)=∂2F∂x2(γ+s,γ−s,At)+∂2F∂y∂x(γ+s,γ−s,At)=+∂2F∂x∂y(γ+s,γ−s,At)+∂2F∂y2(γ+s,γ−s,At)=∂2F∂x2(γ+s,γ−s,At)+2∂2F∂y∂x(γ+s,γ−s,At)+∂2F∂y2(γ+s,γ−s,At)\begin{aligned} \frac{\partial^2G}{\partial\gamma ^2}(\gamma ,s,t) &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) \\ &\phantom{=}+ \frac{\partial^2 F}{\partial x\partial y}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At) \\ &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) +2\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At) \end{aligned}

이고

∂2G∂s2(γ,s,t)=∂2F∂x2(γ+s,γ−s,At)−∂2F∂y∂x(γ+s,γ−s,At)=−[∂2F∂x∂y(γ+s,γ−s,At)−∂2F∂y2(γ+s,γ−s,At)]=∂2F∂x2(γ+s,γ−s,At)−2∂2F∂y∂x(γ+s,γ−s,At)+∂2F∂y2(γ+s,γ−s,At)\begin{aligned} \frac{\partial^2G}{\partial s^2}(\gamma ,s,t) &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) -\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) \\ &\phantom{=}-\Big[ \frac{\partial^2 F}{\partial x\partial y}(\gamma + s, \gamma-s, At) -\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At)\Big] \\ &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) -2\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At) \end{aligned}

이다.

그러므로 변수를 생략하고 나타내면,

∂2G∂γ2+∂2G∂s2−∂G∂t=2∂2F∂x2+2∂2F∂y2−A∂F∂z=2∂F∂z−A∂F∂z=0\begin{aligned} \frac{\partial^2 G}{\partial \gamma^2} + \frac{\partial^2 G}{\partial s^2} -\frac{\partial G}{\partial t} &=2\frac{\partial^2 F}{\partial x^2} + 2\frac{\partial^2 F}{\partial y^2} -A \frac{\partial F}{\partial z} =2\frac{\partial F}{\partial z}-A \frac{\partial F}{\partial z} =0 \end{aligned}

이다. 이는 A=2A=2 이면 성립한다.

원본 교재 풀이(영어)

By the chain rule

∂G∂t(γ,s,t)=∂∂t[F(γ+s,γ−s,At)]=∂F∂x(γ+s,γ−s,At) ∂∂t(γ+s)+∂F∂y(γ+s,γ−s,At) ∂∂t(γ−s)+∂F∂z(γ+s,γ−s,At) ∂∂t(At)=A ∂F∂z(γ+s,γ−s,At)\begin{aligned} \frac{\partial G}{\partial t}(\gamma ,s,t) &= \frac{\partial }{\partial t} \Big[F (\gamma + s, \gamma-s, At)\Big] \\ &=\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial t}(\gamma + s) +\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial t}(\gamma - s) \\& +\frac{\partial F}{\partial z}(\gamma + s, \gamma-s, At)\,\frac{\partial }{\partial t}(At) \\ &= A\,\frac{\partial F}{\partial z}(\gamma + s, \gamma-s, At) \end{aligned}

and

∂G∂γ(γ,s,t)=∂∂γ[F(γ+s,γ−s,At)]=∂F∂x(γ+s,γ−s,At) ∂∂γ(γ+s)+∂F∂y(γ+s,γ−s,At) ∂∂γ(γ−s)+∂F∂z(γ+s,γ−s,At) ∂∂γ(At)=∂F∂x(γ+s,γ−s,At)+∂F∂y(γ+s,γ−s,At)(E1)\begin{aligned} \frac{\partial G}{\partial \gamma }(\gamma ,s,t) &= \frac{\partial }{\partial \gamma } \Big[F (\gamma + s, \gamma-s, At)\Big] \\ &=\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial \gamma }(\gamma + s) +\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial \gamma }(\gamma - s) \\& +\frac{\partial F}{\partial z}(\gamma + s, \gamma-s, At)\,\frac{\partial }{\partial \gamma }(At) \\ &= \frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At) +\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \tag{E1} \end{aligned}

and

∂G∂s(γ,s,t)=∂∂s[F(γ+s,γ−s,At)]=∂F∂x(γ+s,γ−s,At) ∂∂s(γ+s)+∂F∂y(γ+s,γ−s,At) ∂∂s(γ−s)+∂F∂z(γ+s,γ−s,At) ∂∂s(At)=∂F∂x(γ+s,γ−s,At)−∂F∂y(γ+s,γ−s,At)(E2)\begin{aligned} \frac{\partial G}{\partial s}(\gamma ,s,t) &= \frac{\partial }{\partial s} \Big[F (\gamma + s, \gamma-s, At)\Big] \\ &=\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial s}(\gamma + s) +\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At)\, \frac{\partial }{\partial s}(\gamma - s) \\& +\frac{\partial F}{\partial z}(\gamma + s, \gamma-s, At)\,\frac{\partial }{\partial s}(At) \\ &= \frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At) -\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \tag{E2} \end{aligned}

We can evaluate the second derivatives by applying the chain rule to the four terms on the right hand sides of

∂2G∂γ2(γ,s,t)=∂∂γ[∂G∂γ(γ,s,t)]=∂∂γ[∂F∂x(γ+s,γ−s,At)]+∂∂γ[∂F∂y(γ+s,γ−s,At)]∂2G∂s2(γ,s,t)=∂∂s[∂G∂s(γ,s,t)]=∂∂s[∂F∂x(γ+s,γ−s,At)]−∂∂s[∂F∂y(γ+s,γ−s,At)]\begin{aligned} \frac{\partial^2G}{\partial\gamma ^2}(\gamma ,s,t) &=\frac{\partial }{\partial \gamma }\Big[\frac{\partial G}{\partial \gamma }(\gamma , s, t)\Big] = \frac{\partial }{\partial \gamma }\Big[\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\Big] + \frac{\partial }{\partial \gamma }\Big[\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \Big] \\ \frac{\partial^2G}{\partial s^2}(\gamma ,s,t) &=\frac{\partial }{\partial s}\Big[\frac{\partial G}{\partial s}(\gamma , s, t)\Big] = \frac{\partial }{\partial s}\Big[\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\Big] - \frac{\partial }{\partial s}\Big[\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \Big] \end{aligned}

Alternatively, we can observe that replacing FF by ∂F∂x\frac{\partial F}{\partial x} in (E1) and (E2) gives

∂∂γ[∂F∂x(γ+s,γ−s,At)]=∂2F∂x2(γ+s,γ−s,At)+∂2F∂y∂x(γ+s,γ−s,At)∂∂s[∂F∂x(γ+s,γ−s,At)]=∂2F∂x2(γ+s,γ−s,At)−∂2F∂y∂x(γ+s,γ−s,At)\begin{aligned} \frac{\partial }{\partial \gamma }\Big[\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At)\Big] &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) \\ \frac{\partial }{\partial s}\Big[\frac{\partial F}{\partial x}(\gamma + s, \gamma-s, At) \Big] &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) -\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) \end{aligned}

replacing FF by ∂F∂y\frac{\partial F}{\partial y} in (E1) and (E2) gives

∂∂γ[∂F∂y(γ+s,γ−s,At)]=∂2F∂x∂y(γ+s,γ−s,At)+∂2F∂y2(γ+s,γ−s,At)∂∂s[∂F∂y(γ+s,γ−s,At)]=∂2F∂x∂y(γ+s,γ−s,At)−∂2F∂y2(γ+s,γ−s,At)\begin{aligned} \frac{\partial }{\partial \gamma }\Big[\frac{\partial F}{\partial y}(\gamma + s, \gamma-s,At)\Big] &= \frac{\partial^2 F}{\partial x\partial y}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s,At) \\ \frac{\partial }{\partial s}\Big[\frac{\partial F}{\partial y}(\gamma + s, \gamma-s, At) \Big] &= \frac{\partial^2 F}{\partial x\partial y}(\gamma + s, \gamma-s, At) -\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At) \end{aligned}

Consequently

∂2G∂γ2(γ,s,t)=∂2F∂x2(γ+s,γ−s,At)+∂2F∂y∂x(γ+s,γ−s,At)=+∂2F∂x∂y(γ+s,γ−s,At)+∂2F∂y2(γ+s,γ−s,At)=∂2F∂x2(γ+s,γ−s,At)+2∂2F∂y∂x(γ+s,γ−s,At)+∂2F∂y2(γ+s,γ−s,At)\begin{aligned} \frac{\partial^2G}{\partial\gamma ^2}(\gamma ,s,t) &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) \\ &\phantom{=}+ \frac{\partial^2 F}{\partial x\partial y}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At) \\ &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) +2\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At) \end{aligned}

and

∂2G∂s2(γ,s,t)=∂2F∂x2(γ+s,γ−s,At)−∂2F∂y∂x(γ+s,γ−s,At)=−[∂2F∂x∂y(γ+s,γ−s,At)−∂2F∂y2(γ+s,γ−s,At)]=∂2F∂x2(γ+s,γ−s,At)−2∂2F∂y∂x(γ+s,γ−s,At)+∂2F∂y2(γ+s,γ−s,At)\begin{aligned} \frac{\partial^2G}{\partial s^2}(\gamma ,s,t) &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) -\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) \\ &\phantom{=}-\Big[ \frac{\partial^2 F}{\partial x\partial y}(\gamma + s, \gamma-s, At) -\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At)\Big] \\ &= \frac{\partial^2 F}{\partial x^2}(\gamma + s, \gamma-s, At) -2\frac{\partial^2 F}{\partial y\partial x}(\gamma + s, \gamma-s, At) +\frac{\partial^2 F}{\partial y^2}(\gamma + s, \gamma-s, At) \end{aligned}

So, suppressing the arguments,

∂2G∂γ2+∂2G∂s2−∂G∂t=2∂2F∂x2+2∂2F∂y2−A∂F∂z=2∂F∂z−A∂F∂z=0\begin{aligned} \frac{\partial^2 G}{\partial \gamma^2} + \frac{\partial^2 G}{\partial s^2} -\frac{\partial G}{\partial t} &=2\frac{\partial^2 F}{\partial x^2} + 2\frac{\partial^2 F}{\partial y^2} -A \frac{\partial F}{\partial z} =2\frac{\partial F}{\partial z}-A \frac{\partial F}{\partial z} =0 \end{aligned}

if A=2A=2.

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 16번
# 다변수 연쇄법칙계산보통자동 분류
26.CLP-3 · 2.4절 · 18번대학 수준우리말 번역

f(x)f(x) 를 미분가능한 함수라 하고, f′(0)=10f'(0) = 10 이 주어졌다고 하자. g(s,t)=f(as−bt)g(s,t) = f (as - bt) 라 하자. 여기서 aa 와 bb 는 상수이다. 점 (s,t)=(b,a)(s,t) = (b,a) 에서 ∂g∂s\frac{\partial g}{\partial s} 의 값을 구하세요. 즉, ∂g∂s∣(b,a)\frac{\partial g}{\partial s}\big|_{(b,a)} 를 구하세요.

영어 원문 보기

Let f(x)f(x) be a differentiable function, and suppose it is given that f′(0)=10f'(0) = 10. Let g(s,t)=f(as−bt)g(s,t) = f (as - bt), where aa and bb are constants. Evaluate ∂g∂s\frac{\partial g}{\partial s} at the point (s,t)=(b,a)(s,t) = (b,a), that is, find ∂g∂s∣(b,a)\frac{\partial g}{\partial s}\big|_{(b,a)}.

답 쓰고 채점
정답·풀이 보기

연쇄 법칙에 의해

∂g∂s(s,t)=∂∂s[f(as−bt)]=f′(as−bt)∂∂s(as−bt)=af′(as−bt)\begin{aligned} \frac{\partial g}{\partial s}(s,t) = \frac{\partial }{\partial s}\big[f(as-bt)\big] =f'(as-bt)\frac{\partial }{\partial s}(as-bt) = af'(as-bt) \end{aligned}

특히

∂g∂s(b,a)=af′(ab−ba)=af′(0)=10a\begin{aligned} \frac{\partial g}{\partial s}(b,a) = af'(ab-ba) =af'(0) =10 a \end{aligned}

원본 교재 풀이(영어)

By the chain rule

∂g∂s(s,t)=∂∂s[f(as−bt)]=f′(as−bt)∂∂s(as−bt)=af′(as−bt)\begin{aligned} \frac{\partial g}{\partial s}(s,t) = \frac{\partial }{\partial s}\big[f(as-bt)\big] =f'(as-bt)\frac{\partial }{\partial s}(as-bt) = af'(as-bt) \end{aligned}

In particular

∂g∂s(b,a)=af′(ab−ba)=af′(0)=10a\begin{aligned} \frac{\partial g}{\partial s}(b,a) = af'(ab-ba) =af'(0) =10 a \end{aligned}

한 번 더 — 비슷한 문제 풀기OpenStax 3권 · 4.5절 · 23번
# 다변수 연쇄법칙계산보통자동 분류
27.CLP-3 · 2.4절 · 19번대학 수준우리말 번역

f(u,v)f(u,v) 를 두 변수의 미분가능한 함수라 하고, zz 를 f(xz,yz)=0f(xz,yz) = 0 으로 음함수로 정의된 xx 와 yy 의 미분가능한 함수라 하자. 다음을 보이세요.

x∂z∂x+y∂z∂y=−zx\frac{\partial z}{\partial x}+y\frac{\partial z}{\partial y} = -z

영어 원문 보기

Let f(u,v)f(u,v) be a differentiable function of two variables, and let zz be a differentiable function of xx and yy defined implicitly by f(xz,yz)=0f(xz,yz) = 0. Show that

x∂z∂x+y∂z∂y=−zx\frac{\partial z}{\partial x}+y\frac{\partial z}{\partial y} = -z

정답·풀이 보기

함수 z(x,y)z(x,y) 는 모든 xx 와 yy 에 대해

f(x z(x,y) , y z(x,y))=0(∗)f\big(x\,z(x,y)\,,\, y\,z(x,y)\big) =0 \tag{$*$}

을 만족한다. 연쇄 법칙에 의해

∂∂x[f(x z(x,y) , y z(x,y))]=fu(x z(x,y) , y z(x,y))∂∂x[x z(x,y)]+fv(x z(x,y) , y z(x,y))∂∂x[y z(x,y)]=fu(x z(x,y) , y z(x,y)) [z(x,y)+x zx(x,y)]+fv(x z(x,y) , y z(x,y)) y zx(x,y)∂∂y[f(x z(x,y) , y z(x,y))]=fu(x z(x,y) , y z(x,y))∂∂y[x z(x,y)]+fv(x z(x,y) , y z(x,y))∂∂y[y z(x,y)]=fu(x z(x,y) , y z(x,y)) x zy(x,y)+fv(x z(x,y) , y z(x,y)) [z(x,y)+y zy(x,y)]\begin{aligned} &\frac{\partial }{\partial x}\big[f\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\big] \\[-0.05in] &=f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\frac{\partial }{\partial x}\big[x\,z(x,y)\big] + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\frac{\partial }{\partial x}\big[y\,z(x,y)\big] \\ &=f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\,\big[z(x,y)+x\,z_x(x,y)\big] + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\,y\,z_x(x,y) \\ &\frac{\partial }{\partial y}\big[f\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\big] \\[-0.05in] &=f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\frac{\partial }{\partial y}\big[x\,z(x,y)\big] + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\frac{\partial }{\partial y}\big[y\,z(x,y)\big] \\ &=f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\, x\,z_y(x,y) + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\, \big[z(x,y)+y\,z_y(x,y)\big] \end{aligned}

이므로 (∗)(*) 를 xx 에 대해, 그리고 yy 에 대해 미분하면

fu(x z(x,y) , y z(x,y)) [z(x,y)+x zx(x,y)]+fv(x z(x,y) , y z(x,y)) yzx(x,y)=0fu(x z(x,y) , y z(x,y)) x zy(x,y)+fv(x z(x,y) , y z(x,y)) [z(x,y)+y zy(x,y)]=0\begin{aligned} f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\,\big[z(x,y)+x\,z_x(x,y)\big] + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\,y z_x(x,y) &=0 \\ f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\, x\,z_y(x,y) + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\, \big[z(x,y)+y\,z_y(x,y)\big] &=0 \end{aligned}

이고, 인수를 생략하여 나타내면

fu [z+x zx]+fv yzx=0fu x zy+fv [z+y zy]=0\begin{aligned} f_u\,\big[z+x\,z_x\big] + f_v\,y z_x &=0 \\ f_u\, x\,z_y + f_v\,\big[z+y\,z_y\big] &=0 \end{aligned}

이다. 첫 번째 식을 zxz_x 에 대해, 두 번째 식을 zyz_y 에 대해 풀면

zx=−z fux fu+y fvzy=−z fvx fu+y fv\begin{aligned} z_x & = -\frac{z\,f_u}{x\,f_u+y\,f_v} \\ z_y & = -\frac{z\,f_v}{x\,f_u+y\,f_v} \end{aligned}

이므로

x∂z∂x+y∂z∂y=−xz fux fu+y fv−yz fvx fu+y fv=−z (x fu+y fv)x fu+y fv=−z\begin{aligned} x\frac{\partial z}{\partial x}+y\frac{\partial z}{\partial y} = -\frac{xz\,f_u}{x\,f_u+y\,f_v} -\frac{yz\,f_v}{x\,f_u+y\,f_v} =-\frac{z\,(x\,f_u+y\,f_v)}{x\,f_u+y\,f_v} = -z \end{aligned}

이다. 따라서 주어진 등식이 성립한다.

참고: 이는 물론 x fu+y fvx\,f_u+y\,f_v 가 0이 아니라는 가정 아래에서이다. 연쇄 법칙에 의해 이 가정은 ∂∂z[f(xz,yz)]\frac{\partial }{\partial z}\big[f(xz,yz)\big] 가 0이 아니라는 가정과 같다. 이는 다시 f(xz,yz)=0f(xz,yz)=0 을 xx 와 yy 의 함수로서 zz 에 대해 풀 수 있다는 진술과 거의 같지만, 완전히 같지는 않다.

원본 교재 풀이(영어)

We are told that the function z(x,y)z(x,y) obeys

f(x z(x,y) , y z(x,y))=0(∗)f\big(x\,z(x,y)\,,\, y\,z(x,y)\big) =0 \tag{$*$}

for all xx and yy. By the chain rule,

∂∂x[f(x z(x,y) , y z(x,y))]=fu(x z(x,y) , y z(x,y))∂∂x[x z(x,y)]+fv(x z(x,y) , y z(x,y))∂∂x[y z(x,y)]=fu(x z(x,y) , y z(x,y)) [z(x,y)+x zx(x,y)]+fv(x z(x,y) , y z(x,y)) y zx(x,y)∂∂y[f(x z(x,y) , y z(x,y))]=fu(x z(x,y) , y z(x,y))∂∂y[x z(x,y)]+fv(x z(x,y) , y z(x,y))∂∂y[y z(x,y)]=fu(x z(x,y) , y z(x,y)) x zy(x,y)+fv(x z(x,y) , y z(x,y)) [z(x,y)+y zy(x,y)]\begin{aligned} &\frac{\partial }{\partial x}\big[f\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\big] \\[-0.05in] &=f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\frac{\partial }{\partial x}\big[x\,z(x,y)\big] + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\frac{\partial }{\partial x}\big[y\,z(x,y)\big] \\ &=f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\,\big[z(x,y)+x\,z_x(x,y)\big] + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\,y\,z_x(x,y) \\ &\frac{\partial }{\partial y}\big[f\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\big] \\[-0.05in] &=f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\frac{\partial }{\partial y}\big[x\,z(x,y)\big] + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\frac{\partial }{\partial y}\big[y\,z(x,y)\big] \\ &=f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\, x\,z_y(x,y) + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\, \big[z(x,y)+y\,z_y(x,y)\big] \end{aligned}

so differentiating (∗)(*) with respect to xx and with respect to yy gives

fu(x z(x,y) , y z(x,y)) [z(x,y)+x zx(x,y)]+fv(x z(x,y) , y z(x,y)) yzx(x,y)=0fu(x z(x,y) , y z(x,y)) x zy(x,y)+fv(x z(x,y) , y z(x,y)) [z(x,y)+y zy(x,y)]=0\begin{aligned} f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\,\big[z(x,y)+x\,z_x(x,y)\big] + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\,y z_x(x,y) &=0 \\ f_u\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\, x\,z_y(x,y) + f_v\big(x\,z(x,y)\,,\, y\,z(x,y)\big)\, \big[z(x,y)+y\,z_y(x,y)\big] &=0 \end{aligned}

or, leaving out the arguments,

fu [z+x zx]+fv yzx=0fu x zy+fv [z+y zy]=0\begin{aligned} f_u\,\big[z+x\,z_x\big] + f_v\,y z_x &=0 \\ f_u\, x\,z_y + f_v\,\big[z+y\,z_y\big] &=0 \end{aligned}

Solving the first equation for zxz_x and the second for zyz_y gives

zx=−z fux fu+y fvzy=−z fvx fu+y fv\begin{aligned} z_x & = -\frac{z\,f_u}{x\,f_u+y\,f_v} \\ z_y & = -\frac{z\,f_v}{x\,f_u+y\,f_v} \end{aligned}

so that

x∂z∂x+y∂z∂y=−xz fux fu+y fv−yz fvx fu+y fv=−z (x fu+y fv)x fu+y fv=−z\begin{aligned} x\frac{\partial z}{\partial x}+y\frac{\partial z}{\partial y} = -\frac{xz\,f_u}{x\,f_u+y\,f_v} -\frac{yz\,f_v}{x\,f_u+y\,f_v} =-\frac{z\,(x\,f_u+y\,f_v)}{x\,f_u+y\,f_v} = -z \end{aligned}

as desired.

Remark: This is of course under the assumption that x fu+y fvx\,f_u+y\,f_v is nonzero. That is equivalent, by the chain rule, to the assumption that ∂∂z[f(xz,yz)]\frac{\partial }{\partial z}\big[f(xz,yz)\big] is non zero. That, in turn, is almost, but not quite, equivalent to the statement that f(xz,yz)=0f(xz,yz)=0 is can be solved for zz as a function of xx and yy.

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 18번
# 다변수 연쇄법칙증명·논술보통자동 분류
28.CLP-3 · 2.4절 · 20번대학 수준우리말 번역

어떤 두 번 미분가능한 함수 u=u(x,y)u = u(x, y) 에 대하여 w(s,t)=u(2s+3t,3s−2t)w(s,t) = u(2s + 3t, 3s - 2t) 라 하자.

(a) wssw_{ss} 를 uxxu_{xx}, uxyu_{xy}, uyyu_{yy} 로 나타내세요 (uxy=uyxu_{xy} = u_{yx} 라고 가정해도 됩니다). (b) uxx+uyy=0u_{xx} + u_{yy} = 0 이라 하자. 상수 AA 가 얼마일 때 wss=Awttw_{ss} = Aw_{tt} 가 되는지 구하세요.

영어 원문 보기

Let w(s,t)=u(2s+3t,3s−2t)w(s,t) = u(2s + 3t, 3s - 2t) for some twice differentiable function u=u(x,y)u = u(x, y).

(a) Find wssw_{ss} in terms of uxxu_{xx}, uxyu_{xy} , and uyyu_{yy} (you can assume that uxy=uyxu_{xy} = u_{yx}). (b) Suppose uxx+uyy=0u_{xx} + u_{yy} = 0. For what constant AA will wss=Awttw_{ss} = Aw_{tt}?

정답·풀이 보기

(a) 연쇄 법칙에 의해

ws(s,t)=∂∂s[u(2s+3t,3s−2t)]=ux(2s+3t,3s−2t)∂∂s(2s+3t)+uy(2s+3t,3s−2t)∂∂s(3s−2t)=2 ux(2s+3t,3s−2t)+3 uy(2s+3t,3s−2t)\begin{aligned} w_s(s,t) &=\frac{\partial }{\partial s}\big[u(2s + 3t, 3s - 2t)\big] \\ &= u_x(2s + 3t, 3s - 2t)\frac{\partial }{\partial s}\big(2s + 3t\big) +u_y(2s + 3t, 3s - 2t)\frac{\partial }{\partial s}\big(3s - 2t\big) \\ &= 2\,u_x(2s + 3t, 3s - 2t) +3\,u_y(2s + 3t, 3s - 2t) \end{aligned}

이고

wss(s,t)=2∂∂s[ux(2s+3t,3s−2t)]+3∂∂s[uy(2s+3t,3s−2t)]=[4uxx(2s+3t,3s−2t)+6uxy(2s+3t,3s−2t)]+[6uyx(2s+3t,3s−2t)+9uyy(2s+3t,3s−2t)]=4 uxx(2s+3t,3s−2t)+12 uxy(2s+3t,3s−2t)+9 uyy(2s+3t,3s−2t)\begin{aligned} w_{ss}(s,t) &= 2\frac{\partial }{\partial s}\big[u_x(2s + 3t, 3s - 2t)\big] + 3\frac{\partial }{\partial s}\big[u_y(2s + 3t, 3s - 2t)\big] \\ &= \big[4u_{xx}(2s + 3t, 3s - 2t) +6u_{xy}(2s + 3t, 3s - 2t) \big] \\& + \big[6u_{yx}(2s + 3t, 3s - 2t) +9u_{yy}(2s + 3t, 3s - 2t) \big] \\ &=4\,u_{xx}(2s + 3t, 3s - 2t) +12\,u_{xy}(2s + 3t, 3s - 2t) +9\,u_{yy}(2s + 3t, 3s - 2t) \end{aligned}

이다.

(b) 다시 연쇄 법칙에 의해

wt(s,t)=∂∂t[u(2s+3t,3s−2t)]=ux(2s+3t,3s−2t)∂∂t(2s+3t)+uy(2s+3t,3s−2t)∂∂t(3s−2t)=3 ux(2s+3t,3s−2t)−2 uy(2s+3t,3s−2t)\begin{aligned} w_t(s,t) &=\frac{\partial }{\partial t}\big[u(2s + 3t, 3s - 2t)\big] \\ &= u_x(2s + 3t, 3s - 2t)\frac{\partial }{\partial t}\big(2s + 3t\big) +u_y(2s + 3t, 3s - 2t)\frac{\partial }{\partial t}\big(3s - 2t\big) \\ &= 3\,u_x(2s + 3t, 3s - 2t) -2\, u_y(2s + 3t, 3s - 2t) \end{aligned}

이고

wtt(s,t)=3∂∂t[ux(2s+3t,3s−2t)]−2∂∂t[uy(2s+3t,3s−2t)]=[9uxx(2s+3t,3s−2t)−6uxy(2s+3t,3s−2t)]−[6uyx(2s+3t,3s−2t)−4uyy(2s+3t,3s−2t)]=9 uxx(2s+3t,3s−2t)−12 uxy(2s+3t,3s−2t)+4 uyy(2s+3t,3s−2t)\begin{aligned} w_{tt}(s,t) &= 3\frac{\partial }{\partial t}\big[u_x(2s + 3t, 3s - 2t)\big] - 2\frac{\partial }{\partial t}\big[u_y(2s + 3t, 3s - 2t)\big] \\ &= \big[9u_{xx}(2s + 3t, 3s - 2t) -6u_{xy}(2s + 3t, 3s - 2t) \big] \\& - \big[6u_{yx}(2s + 3t, 3s - 2t) -4u_{yy}(2s + 3t, 3s - 2t) \big] \\ &=9\,u_{xx}(2s + 3t, 3s - 2t) -12\,u_{xy}(2s + 3t, 3s - 2t) +4\,u_{yy}(2s + 3t, 3s - 2t) \end{aligned}

이다.

따라서 임의의 상수 AA 에 대해

wss−Awtt=(4−9A)uxx+(12+12A)uxy+(9−4A)uyy\begin{aligned} w_{ss} - Aw_{tt} &= (4-9A) u_{xx} +(12+12A) u_{xy} + (9-4A) u_{yy} \end{aligned}

이다.

uxx+uyy=0u_{xx} + u_{yy}=0 이 주어졌으므로, A=−1A=-1 이면 이 값은 원하는 대로 0이 된다. (이때 (4−9A)=(9−4A)=13(4-9A)=(9-4A)=13 이다.)

원본 교재 풀이(영어)

(a) By the chain rule

ws(s,t)=∂∂s[u(2s+3t,3s−2t)]=ux(2s+3t,3s−2t)∂∂s(2s+3t)+uy(2s+3t,3s−2t)∂∂s(3s−2t)=2 ux(2s+3t,3s−2t)+3 uy(2s+3t,3s−2t)\begin{aligned} w_s(s,t) &=\frac{\partial }{\partial s}\big[u(2s + 3t, 3s - 2t)\big] \\ &= u_x(2s + 3t, 3s - 2t)\frac{\partial }{\partial s}\big(2s + 3t\big) +u_y(2s + 3t, 3s - 2t)\frac{\partial }{\partial s}\big(3s - 2t\big) \\ &= 2\,u_x(2s + 3t, 3s - 2t) +3\,u_y(2s + 3t, 3s - 2t) \end{aligned}

and

wss(s,t)=2∂∂s[ux(2s+3t,3s−2t)]+3∂∂s[uy(2s+3t,3s−2t)]=[4uxx(2s+3t,3s−2t)+6uxy(2s+3t,3s−2t)]+[6uyx(2s+3t,3s−2t)+9uyy(2s+3t,3s−2t)]=4 uxx(2s+3t,3s−2t)+12 uxy(2s+3t,3s−2t)+9 uyy(2s+3t,3s−2t)\begin{aligned} w_{ss}(s,t) &= 2\frac{\partial }{\partial s}\big[u_x(2s + 3t, 3s - 2t)\big] + 3\frac{\partial }{\partial s}\big[u_y(2s + 3t, 3s - 2t)\big] \\ &= \big[4u_{xx}(2s + 3t, 3s - 2t) +6u_{xy}(2s + 3t, 3s - 2t) \big] \\& + \big[6u_{yx}(2s + 3t, 3s - 2t) +9u_{yy}(2s + 3t, 3s - 2t) \big] \\ &=4\,u_{xx}(2s + 3t, 3s - 2t) +12\,u_{xy}(2s + 3t, 3s - 2t) +9\,u_{yy}(2s + 3t, 3s - 2t) \end{aligned}

(b) Again by the chain rule

wt(s,t)=∂∂t[u(2s+3t,3s−2t)]=ux(2s+3t,3s−2t)∂∂t(2s+3t)+uy(2s+3t,3s−2t)∂∂t(3s−2t)=3 ux(2s+3t,3s−2t)−2 uy(2s+3t,3s−2t)\begin{aligned} w_t(s,t) &=\frac{\partial }{\partial t}\big[u(2s + 3t, 3s - 2t)\big] \\ &= u_x(2s + 3t, 3s - 2t)\frac{\partial }{\partial t}\big(2s + 3t\big) +u_y(2s + 3t, 3s - 2t)\frac{\partial }{\partial t}\big(3s - 2t\big) \\ &= 3\,u_x(2s + 3t, 3s - 2t) -2\, u_y(2s + 3t, 3s - 2t) \end{aligned}

and

wtt(s,t)=3∂∂t[ux(2s+3t,3s−2t)]−2∂∂t[uy(2s+3t,3s−2t)]=[9uxx(2s+3t,3s−2t)−6uxy(2s+3t,3s−2t)]−[6uyx(2s+3t,3s−2t)−4uyy(2s+3t,3s−2t)]=9 uxx(2s+3t,3s−2t)−12 uxy(2s+3t,3s−2t)+4 uyy(2s+3t,3s−2t)\begin{aligned} w_{tt}(s,t) &= 3\frac{\partial }{\partial t}\big[u_x(2s + 3t, 3s - 2t)\big] - 2\frac{\partial }{\partial t}\big[u_y(2s + 3t, 3s - 2t)\big] \\ &= \big[9u_{xx}(2s + 3t, 3s - 2t) -6u_{xy}(2s + 3t, 3s - 2t) \big] \\& - \big[6u_{yx}(2s + 3t, 3s - 2t) -4u_{yy}(2s + 3t, 3s - 2t) \big] \\ &=9\,u_{xx}(2s + 3t, 3s - 2t) -12\,u_{xy}(2s + 3t, 3s - 2t) +4\,u_{yy}(2s + 3t, 3s - 2t) \end{aligned}

Consquently, for any constant AA,

wss−Awtt=(4−9A)uxx+(12+12A)uxy+(9−4A)uyy\begin{aligned} w_{ss} - Aw_{tt} &= (4-9A) u_{xx} +(12+12A) u_{xy} + (9-4A) u_{yy} \end{aligned}

Given that uxx+uyy=0u_{xx} + u_{yy}=0, this will be zero, as desired, if A=−1A=-1. (Then (4−9A)=(9−4A)=13(4-9A)=(9-4A)=13.)

한 번 더 — 비슷한 문제 풀기OpenStax 3권 · 4.5절 · 15번
# 다변수 연쇄법칙계산보통자동 분류
29.CLP-3 · 2.4절 · 22번대학 수준우리말 번역

정의에 따르면, 미분가능한 함수 f(x,y)f(x,y) 의 점 (x0 , y0)\big( x_0\,,\,y_0\big) 에서의 기울기 벡터는 다음과 같다.

∇f(x0,y0)=<∂f∂x(x0 , y0) , ∂f∂y(x0 , y0)>{ \boldsymbol{\nabla} } f(x_0,y_0) =\left< \frac{\partial f}{\partial x}\big( x_0\,,\,y_0\big)\,,\, \frac{\partial f}{\partial y}\big( x_0\,,\,y_0\big)\right>

다음을 알고 있다고 하자.

∇f(3,6)=<7,8>{ \boldsymbol{\nabla} } f(3,6)=\left< 7,8\right>

또한

∇g(1,2)=<−1,4>,{ \boldsymbol{\nabla} } g(1,2)=\left< -1,4\right>,

이고

∇h(1,2)=<−5,10>.{ \boldsymbol{\nabla} } h(1,2)=\left< -5,10\right>.

이라고 하자.

g(1,2)=3g(1,2)=3, h(1,2)=6h(1,2)=6 이고 z(s,t)=f(g(s,t),h(s,t))z(s,t)=f\big(g(s,t),h(s,t)\big) 일 때, 다음을 구하세요.

∇z(1,2){ \boldsymbol{\nabla} } z(1,2)

영어 원문 보기

By definition, the gradient of the differentiable function f(x,y)f(x,y) at the point (x0 , y0)\big( x_0\,,\,y_0\big) is

∇f(x0,y0)=<∂f∂x(x0 , y0) , ∂f∂y(x0 , y0)>{ \boldsymbol{\nabla} } f(x_0,y_0) =\left< \frac{\partial f}{\partial x}\big( x_0\,,\,y_0\big)\,,\, \frac{\partial f}{\partial y}\big( x_0\,,\,y_0\big)\right>

Suppose that we know

∇f(3,6)=<7,8>{ \boldsymbol{\nabla} } f(3,6)=\left< 7,8\right>

Suppose also that

∇g(1,2)=<−1,4>,{ \boldsymbol{\nabla} } g(1,2)=\left< -1,4\right>,

and

∇h(1,2)=<−5,10>.{ \boldsymbol{\nabla} } h(1,2)=\left< -5,10\right>.

Assuming g(1,2)=3g(1,2)=3, h(1,2)=6h(1,2)=6, and z(s,t)=f(g(s,t),h(s,t))z(s,t)=f\big(g(s,t),h(s,t)\big), find

∇z(1,2){ \boldsymbol{\nabla} } z(1,2)

정답·풀이 보기

연쇄 법칙에 의해

∂z∂s(s,t)=∂∂sf(g(s,t),h(s,t))=∂f∂x(g(s,t),h(s,t))∂g∂s(s,t)+∂f∂y(g(s,t),h(s,t))∂h∂s(s,t)∂z∂t(s,t)=∂∂tf(g(s,t),h(s,t))=∂f∂x(g(s,t),h(s,t))∂g∂t(s,t)+∂f∂y(g(s,t),h(s,t))∂h∂t(s,t)\begin{aligned} \frac{\partial z}{\partial s}(s,t) &=\frac{\partial }{\partial s}f\big(g(s,t),h(s,t)\big) &&=\frac{\partial f}{\partial x}\big(g(s,t),h(s,t)\big) \frac{\partial g}{\partial s}(s,t) +\frac{\partial f}{\partial y}\big(g(s,t),h(s,t)\big) \frac{\partial h}{\partial s}(s,t) \\ \frac{\partial z}{\partial t}(s,t) &=\frac{\partial }{\partial t}f\big(g(s,t),h(s,t)\big) &&=\frac{\partial f}{\partial x}\big(g(s,t),h(s,t)\big) \frac{\partial g}{\partial t}(s,t) +\frac{\partial f}{\partial y}\big(g(s,t),h(s,t)\big) \frac{\partial h}{\partial t}(s,t) \end{aligned}

특히

∂z∂s(1,2)=∂f∂x(g(1,2),h(1,2))∂g∂s(1,2)+∂f∂y(g(1,2),h(1,2))∂h∂s(1,2)=∂f∂x(3,6)∂g∂s(1,2)+∂f∂y(3,6))∂h∂s(1,2)=7×(−1)+8×(−5)=−47∂z∂t(1,2)=∂f∂x(g(1,2),h(1,2))∂g∂t(1,2)+∂f∂y(g(1,2),h(1,2))∂h∂t(1,2)=7×4+8×10=108\begin{aligned} \frac{\partial z}{\partial s}(1,2) &=\frac{\partial f}{\partial x}\big(g(1,2),h(1,2)\big) \frac{\partial g}{\partial s}(1,2) +\frac{\partial f}{\partial y}\big(g(1,2),h(1,2)\big) \frac{\partial h}{\partial s}(1,2) \\ &=\frac{\partial f}{\partial x}(3,6) \frac{\partial g}{\partial s}(1,2) +\frac{\partial f}{\partial y}(3,6)) \frac{\partial h}{\partial s}(1,2) \\ &=7\times(-1)+8\times(-5) =-47\\ \frac{\partial z}{\partial t}(1,2) &=\frac{\partial f}{\partial x}\big(g(1,2),h(1,2)\big) \frac{\partial g}{\partial t}(1,2) +\frac{\partial f}{\partial y}\big(g(1,2),h(1,2)\big) \frac{\partial h}{\partial t}(1,2) \\ &=7\times4+8\times 10 =108 \end{aligned}

따라서 ∇z(1,2)=<−47,108>{ \boldsymbol{\nabla} } z(1,2)=\left< -47,108\right> 이다.

원본 교재 풀이(영어)

By the chain rule

∂z∂s(s,t)=∂∂sf(g(s,t),h(s,t))=∂f∂x(g(s,t),h(s,t))∂g∂s(s,t)+∂f∂y(g(s,t),h(s,t))∂h∂s(s,t)∂z∂t(s,t)=∂∂tf(g(s,t),h(s,t))=∂f∂x(g(s,t),h(s,t))∂g∂t(s,t)+∂f∂y(g(s,t),h(s,t))∂h∂t(s,t)\begin{aligned} \frac{\partial z}{\partial s}(s,t) &=\frac{\partial }{\partial s}f\big(g(s,t),h(s,t)\big) &&=\frac{\partial f}{\partial x}\big(g(s,t),h(s,t)\big) \frac{\partial g}{\partial s}(s,t) +\frac{\partial f}{\partial y}\big(g(s,t),h(s,t)\big) \frac{\partial h}{\partial s}(s,t) \\ \frac{\partial z}{\partial t}(s,t) &=\frac{\partial }{\partial t}f\big(g(s,t),h(s,t)\big) &&=\frac{\partial f}{\partial x}\big(g(s,t),h(s,t)\big) \frac{\partial g}{\partial t}(s,t) +\frac{\partial f}{\partial y}\big(g(s,t),h(s,t)\big) \frac{\partial h}{\partial t}(s,t) \end{aligned}

In particular

∂z∂s(1,2)=∂f∂x(g(1,2),h(1,2))∂g∂s(1,2)+∂f∂y(g(1,2),h(1,2))∂h∂s(1,2)=∂f∂x(3,6)∂g∂s(1,2)+∂f∂y(3,6))∂h∂s(1,2)=7×(−1)+8×(−5)=−47∂z∂t(1,2)=∂f∂x(g(1,2),h(1,2))∂g∂t(1,2)+∂f∂y(g(1,2),h(1,2))∂h∂t(1,2)=7×4+8×10=108\begin{aligned} \frac{\partial z}{\partial s}(1,2) &=\frac{\partial f}{\partial x}\big(g(1,2),h(1,2)\big) \frac{\partial g}{\partial s}(1,2) +\frac{\partial f}{\partial y}\big(g(1,2),h(1,2)\big) \frac{\partial h}{\partial s}(1,2) \\ &=\frac{\partial f}{\partial x}(3,6) \frac{\partial g}{\partial s}(1,2) +\frac{\partial f}{\partial y}(3,6)) \frac{\partial h}{\partial s}(1,2) \\ &=7\times(-1)+8\times(-5) =-47\\ \frac{\partial z}{\partial t}(1,2) &=\frac{\partial f}{\partial x}\big(g(1,2),h(1,2)\big) \frac{\partial g}{\partial t}(1,2) +\frac{\partial f}{\partial y}\big(g(1,2),h(1,2)\big) \frac{\partial h}{\partial t}(1,2) \\ &=7\times4+8\times 10 =108 \end{aligned}

Hence ∇z(1,2)=<−47,108>{ \boldsymbol{\nabla} } z(1,2)=\left< -47,108\right>.

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 23번
# 다변수 연쇄법칙계산보통자동 분류
30.CLP-3 · 2.4절 · 23번대학 수준우리말 번역

(a) ff 를 실수 전체에서 정의된 임의의 미분가능한 함수라 하자. 평면 전체에서 다음과 같이 정의된 함수 ww 가

w(x,y)=e−yf(x−y)w(x,y)=e^{-y}f(x-y)

편미분방정식

w+∂w∂x+∂w∂y=0w+\frac{\partial w}{\partial x}+\frac{\partial w}{\partial y}=0

을 만족시킴을 보이세요. (b) 방정식 x=u3−3uv2x=u^3-3uv^2, y=3u2v−v3y=3u^2v-v^3, z=u2−v2z=u^2-v^2 은 zz 를 xx 와 yy 의 함수로 정의한다. 점 (x,y)=(2,11)(x,y)=(2,11) 에 대응하는 점 (u,v)=(2,1)(u,v)=(2,1) 에서 ∂z∂x\frac{\partial z}{\partial x} 의 값을 구하세요.

영어 원문 보기

(a) Let ff be an arbitrary differentiable function defined on the entire real line. Show that the function ww defined on the entire plane as

w(x,y)=e−yf(x−y)w(x,y)=e^{-y}f(x-y)

satisfies the partial differential equation:

w+∂w∂x+∂w∂y=0w+\frac{\partial w}{\partial x}+\frac{\partial w}{\partial y}=0 (b) The equations x=u3−3uv2x=u^3-3uv^2, y=3u2v−v3y=3u^2v-v^3 and z=u2−v2z=u^2-v^2 define zz as a function of xx and yy. Determine ∂z∂x\frac{\partial z}{\partial x} at the point (u,v)=(2,1)(u,v)=(2,1) which corresponds to the point (x,y)=(2,11)(x,y)=(2,11).

정답·풀이 보기

(a) 곱의 미분법과 연쇄 법칙에 의해

wx(x,y)=∂∂x[e−yf(x−y)]=e−y∂∂x[f(x−y)]=e−yf′(x−y)∂∂x(x−y)=e−yf′(x−y)wy(x,y)=∂∂y[e−yf(x−y)]=−e−yf(x−y)+e−y∂∂y[f(x−y)]=−e−yf(x−y)+e−yf′(x−y)∂∂y(x−y)=−e−yf(x−y)−e−yf′(x−y)\begin{aligned} w_x(x,y) &= \frac{\partial }{\partial x}\big[e^{-y}f(x-y)\big] = e^{-y} \frac{\partial }{\partial x}\big[f(x-y)\big] = e^{-y} f'(x-y)\frac{\partial }{\partial x}(x-y) \\ &= e^{-y}f'(x-y) \\% w_y(x,y) &= \frac{\partial }{\partial y}\big[e^{-y}f(x-y)\big] = -e^{-y}f(x-y) + e^{-y} \frac{\partial }{\partial y}\big[f(x-y)\big] \\ &= -e^{-y}f(x-y) + e^{-y} f'(x-y)\frac{\partial }{\partial y}(x-y) \\ &= -e^{-y}f(x-y)-e^{-y}f'(x-y) \end{aligned}

이므로

w+∂w∂x+∂w∂y=e−yf(x−y)+e−yf′(x−y)−e−yf(x−y)−e−yf′(x−y)=0w+\frac{\partial w}{\partial x}+\frac{\partial w}{\partial y} =e^{-y}f(x-y)+e^{-y}f'(x-y)-e^{-y}f(x-y)-e^{-y}f'(x-y) =0

이다. 따라서 성립한다.

(b) x=u3−3uv2x=u^3-3uv^2, y=3u2v−v3y=3u^2v-v^3 을 xx, yy 가 주어진 매개변수이고 uu, vv 가 미지수인 두 방정식으로 생각하자. 문제는 적어도 (u,v)=(2,1)(u,v)=(2,1), (x,y)=(2,11)(x,y)=(2,11) 근처에서 이 두 방정식을 uu, vv 에 대해 xx, yy 로 풀 수 있음을 암묵적으로 알려 준다. 즉, 함수 u(x,y)u(x,y) 와 v(x,y)v(x,y) 가 다음 식으로 정해진다는 것을 알려 준다.

x=u(x,y)3−3u(x,y) v(x,y)2y=3u(x,y)2v(x,y)−v(x,y)3x=u(x,y)^3-3u(x,y)\,v(x,y)^2\qquad y=3u(x,y)^2v(x,y)-v(x,y)^3

등식 x=u(x,y)3−3u(x,y)v(x,y)2x=u(x,y)^3-3u(x,y)v(x,y)^2 의 양변에 ∂∂x\frac{\partial }{\partial x} 를 취하면

1=3 u(x,y)2 ∂u∂x(x,y)−3∂u∂x(x,y) v(x,y)2−6 u(x,y) v(x,y) ∂v∂x(x,y)\begin{aligned} 1&=3\,u(x,y)^2\,\frac{\partial u}{\partial x}(x,y) -3\frac{\partial u}{\partial x}(x,y)\,v(x,y)^2 -6\,u(x,y)\,v(x,y)\,\frac{\partial v}{\partial x}(x,y) \\[0.05in] \end{aligned}

이다. 다음으로 y=3u(x,y)2v(x,y)−v(x,y)3y=3u(x,y)^2v(x,y)-v(x,y)^3 의 양변에 ∂∂x\frac{\partial }{\partial x} 를 취하면

0=6 u(x,y) ∂u∂x(x,y) v(x,y)+3 u(x,y)2 ∂v∂x(x,y)−3 v(x,y)2 ∂v∂x(x,y)\begin{aligned} 0&=6\,u(x,y)\,\frac{\partial u}{\partial x}(x,y)\,v(x,y) +3\,u(x,y)^2\,\frac{\partial v}{\partial x}(x,y) -3\,v(x,y)^2\,\frac{\partial v}{\partial x}(x,y) \end{aligned}

이다. x=2x=2, y=11y=11, u=2u=2, v=1v=1 을 대입하면

1=12∂u∂x(2,11)−3∂u∂x(2,11)−12∂v∂x(2,11)=9∂u∂x(2,11)−12∂v∂x(2,11)0=12∂u∂x(2,11)+12∂v∂x(2,11)−3∂v∂x(2,11)=12∂u∂x(2,11)+9∂v∂x(2,11)\begin{aligned} 1&=12\frac{\partial u}{\partial x}(2,11) -3\frac{\partial u}{\partial x}(2,11) -12\frac{\partial v}{\partial x}(2,11) &&=9\frac{\partial u}{\partial x}(2,11) -12\frac{\partial v}{\partial x}(2,11)\\[0.05in] 0&=12\frac{\partial u}{\partial x}(2,11) +12\frac{\partial v}{\partial x}(2,11) -3\frac{\partial v}{\partial x}(2,11) &&=12\frac{\partial u}{\partial x}(2,11) +9\frac{\partial v}{\partial x}(2,11) \end{aligned}

이다. 두 번째 식에서 ∂v∂x(2,11)=−43∂u∂x(2,11)\frac{\partial v}{\partial x}(2,11) =-\frac{4}{3}\frac{\partial u}{\partial x}(2,11) 이다. 이를 첫 번째 식에 대입하면

1=9∂u∂x(2,11)−12[−43∂u∂x(2,11)]=25∂u∂x(2,11)1=9\frac{\partial u}{\partial x}(2,11) -12\left[-\frac{4}{3}\frac{\partial u}{\partial x}(2,11)\right] = 25\frac{\partial u}{\partial x}(2,11)

이므로 ∂u∂x(2,11)=125\frac{\partial u}{\partial x}(2,11)=\frac{1}{25} 이고 ∂v∂x(2,11)=−475\frac{\partial v}{\partial x}(2,11)=-\frac{4}{75} 이다. 또한 문제에서 z(x,y)=u(x,y)2−v(x,y)2z(x,y)=u(x,y)^2-v(x,y)^2 임을 알 수 있다. 따라서

∂z∂x(x,y)=2u(x,y)∂u∂x(x,y)−2v(x,y)∂v∂x(x,y)  ⟹  ∂z∂x(2,11)=4∂u∂x(2,11)−2∂v∂x(2,11)=4125+2475=2075=415\begin{aligned} &\frac{\partial z}{\partial x}(x,y) =2u(x,y)\frac{\partial u}{\partial x}(x,y) -2v(x,y)\frac{\partial v}{\partial x}(x,y)\\ \implies & \frac{\partial z}{\partial x}(2,11) =4\frac{\partial u}{\partial x}(2,11) -2\frac{\partial v}{\partial x}(2,11) =4\frac{1}{25}+2\frac{4}{75}=\frac{20}{75} =\frac{4}{15} \end{aligned}

이다.

원본 교재 풀이(영어)

(a) By the product and chain rules

wx(x,y)=∂∂x[e−yf(x−y)]=e−y∂∂x[f(x−y)]=e−yf′(x−y)∂∂x(x−y)=e−yf′(x−y)wy(x,y)=∂∂y[e−yf(x−y)]=−e−yf(x−y)+e−y∂∂y[f(x−y)]=−e−yf(x−y)+e−yf′(x−y)∂∂y(x−y)=−e−yf(x−y)−e−yf′(x−y)\begin{aligned} w_x(x,y) &= \frac{\partial }{\partial x}\big[e^{-y}f(x-y)\big] = e^{-y} \frac{\partial }{\partial x}\big[f(x-y)\big] = e^{-y} f'(x-y)\frac{\partial }{\partial x}(x-y) \\ &= e^{-y}f'(x-y) \\% w_y(x,y) &= \frac{\partial }{\partial y}\big[e^{-y}f(x-y)\big] = -e^{-y}f(x-y) + e^{-y} \frac{\partial }{\partial y}\big[f(x-y)\big] \\ &= -e^{-y}f(x-y) + e^{-y} f'(x-y)\frac{\partial }{\partial y}(x-y) \\ &= -e^{-y}f(x-y)-e^{-y}f'(x-y) \end{aligned}

Hence

w+∂w∂x+∂w∂y=e−yf(x−y)+e−yf′(x−y)−e−yf(x−y)−e−yf′(x−y)=0w+\frac{\partial w}{\partial x}+\frac{\partial w}{\partial y} =e^{-y}f(x-y)+e^{-y}f'(x-y)-e^{-y}f(x-y)-e^{-y}f'(x-y) =0

as desired.

(b) Think of x=u3−3uv2x=u^3-3uv^2, y=3u2v−v3y=3u^2v-v^3 as two equations in the two unknowns uu, vv with xx, yy just being given parameters. The question implicitly tells us that those two equations can be solved for uu, vv in terms of xx, yy, at least near (u,v)=(2,1)(u,v)=(2,1), (x,y)=(2,11)(x,y)=(2,11). That is, the question implicitly tells us that the functions u(x,y)u(x,y) and v(x,y)v(x,y) are determined by

x=u(x,y)3−3u(x,y) v(x,y)2y=3u(x,y)2v(x,y)−v(x,y)3x=u(x,y)^3-3u(x,y)\,v(x,y)^2\qquad y=3u(x,y)^2v(x,y)-v(x,y)^3

Applying ∂∂x\frac{\partial }{\partial x} to both sides of the equation x=u(x,y)3−3u(x,y)v(x,y)2x=u(x,y)^3-3u(x,y)v(x,y)^2 gives

1=3 u(x,y)2 ∂u∂x(x,y)−3∂u∂x(x,y) v(x,y)2−6 u(x,y) v(x,y) ∂v∂x(x,y)\begin{aligned} 1&=3\,u(x,y)^2\,\frac{\partial u}{\partial x}(x,y) -3\frac{\partial u}{\partial x}(x,y)\,v(x,y)^2 -6\,u(x,y)\,v(x,y)\,\frac{\partial v}{\partial x}(x,y) \\[0.05in] \end{aligned}

Then applying ∂∂x\frac{\partial }{\partial x} to both sides of y=3u(x,y)2v(x,y)−v(x,y)3y=3u(x,y)^2v(x,y)-v(x,y)^3 gives

0=6 u(x,y) ∂u∂x(x,y) v(x,y)+3 u(x,y)2 ∂v∂x(x,y)−3 v(x,y)2 ∂v∂x(x,y)\begin{aligned} 0&=6\,u(x,y)\,\frac{\partial u}{\partial x}(x,y)\,v(x,y) +3\,u(x,y)^2\,\frac{\partial v}{\partial x}(x,y) -3\,v(x,y)^2\,\frac{\partial v}{\partial x}(x,y) \end{aligned}

Substituting in x=2x=2, y=11y=11, u=2u=2, v=1v=1 gives

1=12∂u∂x(2,11)−3∂u∂x(2,11)−12∂v∂x(2,11)=9∂u∂x(2,11)−12∂v∂x(2,11)0=12∂u∂x(2,11)+12∂v∂x(2,11)−3∂v∂x(2,11)=12∂u∂x(2,11)+9∂v∂x(2,11)\begin{aligned} 1&=12\frac{\partial u}{\partial x}(2,11) -3\frac{\partial u}{\partial x}(2,11) -12\frac{\partial v}{\partial x}(2,11) &&=9\frac{\partial u}{\partial x}(2,11) -12\frac{\partial v}{\partial x}(2,11)\\[0.05in] 0&=12\frac{\partial u}{\partial x}(2,11) +12\frac{\partial v}{\partial x}(2,11) -3\frac{\partial v}{\partial x}(2,11) &&=12\frac{\partial u}{\partial x}(2,11) +9\frac{\partial v}{\partial x}(2,11) \end{aligned}

From the second equation ∂v∂x(2,11)=−43∂u∂x(2,11)\frac{\partial v}{\partial x}(2,11) =-\frac{4}{3}\frac{\partial u}{\partial x}(2,11). Substituting into the first equation gives

1=9∂u∂x(2,11)−12[−43∂u∂x(2,11)]=25∂u∂x(2,11)1=9\frac{\partial u}{\partial x}(2,11) -12\left[-\frac{4}{3}\frac{\partial u}{\partial x}(2,11)\right] = 25\frac{\partial u}{\partial x}(2,11)

so that ∂u∂x(2,11)=125\frac{\partial u}{\partial x}(2,11)=\frac{1}{25} and ∂v∂x(2,11)=−475\frac{\partial v}{\partial x}(2,11)=-\frac{4}{75}. The question also tells us that z(x,y)=u(x,y)2−v(x,y)2z(x,y)=u(x,y)^2-v(x,y)^2. Hence

∂z∂x(x,y)=2u(x,y)∂u∂x(x,y)−2v(x,y)∂v∂x(x,y)  ⟹  ∂z∂x(2,11)=4∂u∂x(2,11)−2∂v∂x(2,11)=4125+2475=2075=415\begin{aligned} &\frac{\partial z}{\partial x}(x,y) =2u(x,y)\frac{\partial u}{\partial x}(x,y) -2v(x,y)\frac{\partial v}{\partial x}(x,y)\\ \implies & \frac{\partial z}{\partial x}(2,11) =4\frac{\partial u}{\partial x}(2,11) -2\frac{\partial v}{\partial x}(2,11) =4\frac{1}{25}+2\frac{4}{75}=\frac{20}{75} =\frac{4}{15} \end{aligned}

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 20번
# 다변수 연쇄법칙증명·논술보통자동 분류
31.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 문제 풀기CLP-3 · 2.4절 · 15번
# 다변수 연쇄법칙계산보통자동 분류
32.CLP-3 · 2.4절 · 25번대학 수준우리말 번역

f(u,v)f(u,v) 를 미분가능한 함수라 하고, u=x+yu=x+y , v=x−yv=x-y 라 하자. 다음을 만족하는 상수 α\alpha 를 구하세요.

(fx)2+(fy)2=α((fu)2+(fv)2)\begin{aligned} (f_x)^2+(f_y)^2=\alpha \big((f_u)^2+(f_v)^2\big) \end{aligned}

영어 원문 보기

Let f(u,v)f(u,v) be a differentiable function, and let u=x+yu=x+y and v=x−yv=x-y. Find a constant, α\alpha , such that

(fx)2+(fy)2=α((fu)2+(fv)2)\begin{aligned} (f_x)^2+(f_y)^2=\alpha \big((f_u)^2+(f_v)^2\big) \end{aligned}

정답·풀이 보기

이 문제는 나쁜(그러나 흔히 쓰는) 표기를 사용하고 있다. 하나의 기호 ff 가 서로 다른 두 함수, 즉 f(u,v)f(u,v) 와 f(x,y)=f(u,v)∣u=x+y,v=x−yf(x,y)=f(u,v)\big|_{u=x+y,v=x-y} 에 쓰였기 때문이다. 더 나은 표현은 다음과 같다.

  • f(u,v)f(u,v) 와 F(x,y)F(x,y) 를 F(x,y)=f(x+y,x−y)F(x,y)=f(x+y,x-y) 를 만족하는 미분가능한 함수라 하자. 다음을 만족하는 상수 α\alpha 를 구하세요.

Fx(x,y)2+Fy(x,y)2=α{fu(x+y,x−y)2+fv(x+y,x−y)2}F_x(x,y)^2+F_y(x,y)^2=\alpha \big\{f_u(x+y,x-y)^2+f_v(x+y,x-y)^2\big\}

연쇄 법칙에 의해

∂F∂x(x,y)=fu(x+y,x−y)∂∂x(x+y)+fv(x+y,x−y)∂∂x(x−y)=fu(x+y,x−y)+fv(x+y,x−y)∂F∂y(x,y)=fu(x+y,x−y)∂∂y(x+y)+fv(x+y,x−y)∂∂y(x−y)=fu(x+y,x−y)−fv(x+y,x−y)\begin{aligned} \frac{\partial F}{\partial x}(x,y) &=f_u(x+y,x-y)\frac{\partial }{\partial x}(x+y) +f_v(x+y,x-y)\frac{\partial }{\partial x}(x-y) \\ &=f_u(x+y,x-y)+f_v(x+y,x-y)\\ \frac{\partial F}{\partial y}(x,y) &=f_u(x+y,x-y)\frac{\partial }{\partial y}(x+y) +f_v(x+y,x-y)\frac{\partial }{\partial y}(x-y) \\ &=f_u(x+y,x-y)-f_v(x+y,x-y) \end{aligned}

따라서

Fx(x,y)2+Fy(x,y)2=[fu(x+y,x−y)+fv(x+y,x−y)]2+[fu(x+y,x−y)−fv(x+y,x−y)]2=2fu(x+y,x−y)2+2fv(x+y,x−y)2\begin{aligned} F_x(x,y)^2+F_y(x,y)^2 &=\Big[f_u(x+y,x-y)+f_v(x+y,x-y)\Big]^2 \\ & +\Big[f_u(x+y,x-y)-f_v(x+y,x-y)\Big]^2\\ &=2f_u(x+y,x-y)^2+2f_v(x+y,x-y)^2 \end{aligned}

그러므로 α=2\alpha =2 이면 된다.

원본 교재 풀이(영어)

This question uses bad (but standard) notation, in that the one symbol ff is used for two different functions, namely f(u,v)f(u,v) and f(x,y)=f(u,v)∣u=x+y,v=x−yf(x,y)=f(u,v)\big|_{u=x+y,v=x-y}. A better wording is

  • Let f(u,v)f(u,v) and F(x,y)F(x,y) be differentiable functions such that F(x,y)=f(x+y,x−y)F(x,y)=f(x+y,x-y). Find a constant, α\alpha , such that

Fx(x,y)2+Fy(x,y)2=α{fu(x+y,x−y)2+fv(x+y,x−y)2}F_x(x,y)^2+F_y(x,y)^2=\alpha \big\{f_u(x+y,x-y)^2+f_v(x+y,x-y)^2\big\}

By the chain rule

∂F∂x(x,y)=fu(x+y,x−y)∂∂x(x+y)+fv(x+y,x−y)∂∂x(x−y)=fu(x+y,x−y)+fv(x+y,x−y)∂F∂y(x,y)=fu(x+y,x−y)∂∂y(x+y)+fv(x+y,x−y)∂∂y(x−y)=fu(x+y,x−y)−fv(x+y,x−y)\begin{aligned} \frac{\partial F}{\partial x}(x,y) &=f_u(x+y,x-y)\frac{\partial }{\partial x}(x+y) +f_v(x+y,x-y)\frac{\partial }{\partial x}(x-y) \\ &=f_u(x+y,x-y)+f_v(x+y,x-y)\\ \frac{\partial F}{\partial y}(x,y) &=f_u(x+y,x-y)\frac{\partial }{\partial y}(x+y) +f_v(x+y,x-y)\frac{\partial }{\partial y}(x-y) \\ &=f_u(x+y,x-y)-f_v(x+y,x-y) \end{aligned}

Hence

Fx(x,y)2+Fy(x,y)2=[fu(x+y,x−y)+fv(x+y,x−y)]2+[fu(x+y,x−y)−fv(x+y,x−y)]2=2fu(x+y,x−y)2+2fv(x+y,x−y)2\begin{aligned} F_x(x,y)^2+F_y(x,y)^2 &=\Big[f_u(x+y,x-y)+f_v(x+y,x-y)\Big]^2 \\ & +\Big[f_u(x+y,x-y)-f_v(x+y,x-y)\Big]^2\\ &=2f_u(x+y,x-y)^2+2f_v(x+y,x-y)^2 \end{aligned}

So α=2\alpha =2 does the job.

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.4절 · 14번
# 다변수 연쇄법칙계산보통자동 분류
33.CLP-3 · 2.5절 · 7번대학 수준우리말 번역

지정된 점에서 지정된 함수의 그래프에 대한 접평면의 방정식과 법선의 방정식을 구하세요.

(a) f(x,y)=x2−y2f(x,y)=x^2-y^2, 점 (−2,1)(-2,1) (b) f(x,y)=exyf(x,y)=e^{xy}, 점 (2,0)(2,0)

영어 원문 보기

Find the equations of the tangent plane and the normal line to the graph of the specified function at the specified point.

(a) f(x,y)=x2−y2f(x,y)=x^2-y^2 at (−2,1)(-2,1) (b) f(x,y)=exyf(x,y)=e^{xy} at (2,0)(2,0)

정답·풀이 보기

(a) 주어진 그래프는 z=f(x,y)=x2−y2z=f(x,y)=x^2-y^2 또는 F(x,y,z)=x2−y2−z=0F(x,y,z)=x^2-y^2-z=0 이다. f(−2,1)=3f(-2,1)=3 임을 알 수 있다. 벡터

∇F(−2,1,3)=<Fx(x,y,z),Fy(x,y,z),Fz(x,y,z)>∣(x,y,z)=(−2,1,3)=<2x,−2y,−1>∣(x,y,z)=(−2,1,3)=<−4,−2,−1>\begin{aligned} { \boldsymbol{\nabla} } F(-2,1,3) &= \left< F_x(x,y,z),F_y(x,y,z),F_z(x,y,z)\right>\Big|_{(x,y,z)=(-2,1,3)} \\ &= \left< 2x,-2y,-1\right>\Big|_{(x,y,z)=(-2,1,3)} \\ &= \left< -4,-2,-1\right> \end{aligned}

는 (−2,1,3)(-2,1,3) 에서 그래프의 법선 벡터이다. 따라서 접평면은

−4(x+2)−2(y−1)−(z−3)=0 또는 4x+2y+z=−3-4(x+2)-2(y-1)-(z-3)=0\text{ 또는 } 4x+2y+z=-3

이고, 법선은

<x,y,z>=<−2,1,3>+t<4,2,1>\left< x,y,z\right>=\left< -2,1,3\right>+t\left< 4,2,1\right>

이다.

(b) 주어진 그래프는 z=f(x,y)=exyz=f(x,y)=e^{xy} 또는 F(x,y,z)=exy−z=0F(x,y,z)=e^{xy}-z=0 이다. f(2,0)=1f(2,0)=1 임을 알 수 있다. 벡터

∇F(2,0,1)=<Fx(x,y,z),Fy(x,y,z),Fz(x,y,z)>∣(x,y,z)=(2,0,1)=<yexy,xexy,−1>∣(x,y,z)=(2,0,1)=<0,2,−1>\begin{aligned} { \boldsymbol{\nabla} } F(2,0,1) &= \left< F_x(x,y,z),F_y(x,y,z),F_z(x,y,z)\right>\Big|_{(x,y,z)=(2,0,1)} \\ &= \left< ye^{xy},xe^{xy},-1\right>\Big|_{(x,y,z)=(2,0,1)} \\ &= \left< 0,2,-1\right> \end{aligned}

는 (2,0,1)(2,0,1) 에서 그래프의 법선 벡터이다. 따라서 접평면은

0(x−2)+2(y−0)−(z−1)=0 또는 2y−z=−10(x-2)+2(y-0)-(z-1)=0\text{ 또는 } 2y-z=-1

이고, 법선은

<x,y,z>=<2,0,1>+t<0,2,−1>\left< x,y,z\right>=\left< 2,0,1\right>+t\left< 0,2,-1\right>

이다.

원본 교재 풀이(영어)

(a) The specified graph is z=f(x,y)=x2−y2z=f(x,y)=x^2-y^2 or F(x,y,z)=x2−y2−z=0F(x,y,z)=x^2-y^2-z=0. Observe that f(−2,1)=3f(-2,1)=3. The vector

∇F(−2,1,3)=<Fx(x,y,z),Fy(x,y,z),Fz(x,y,z)>∣(x,y,z)=(−2,1,3)=<2x,−2y,−1>∣(x,y,z)=(−2,1,3)=<−4,−2,−1>\begin{aligned} { \boldsymbol{\nabla} } F(-2,1,3) &= \left< F_x(x,y,z),F_y(x,y,z),F_z(x,y,z)\right>\Big|_{(x,y,z)=(-2,1,3)} \\ &= \left< 2x,-2y,-1\right>\Big|_{(x,y,z)=(-2,1,3)} \\ &= \left< -4,-2,-1\right> \end{aligned}

is a normal vector to the graph at (−2,1,3)(-2,1,3). So the tangent plane is

−4(x+2)−2(y−1)−(z−3)=0 or 4x+2y+z=−3-4(x+2)-2(y-1)-(z-3)=0\text{ or } 4x+2y+z=-3

and the normal line is

<x,y,z>=<−2,1,3>+t<4,2,1>\left< x,y,z\right>=\left< -2,1,3\right>+t\left< 4,2,1\right>

(b) The specified graph is z=f(x,y)=exyz=f(x,y)=e^{xy} or F(x,y,z)=exy−z=0F(x,y,z)=e^{xy}-z=0. Observe that f(2,0)=1f(2,0)=1. The vector

∇F(2,0,1)=<Fx(x,y,z),Fy(x,y,z),Fz(x,y,z)>∣(x,y,z)=(2,0,1)=<yexy,xexy,−1>∣(x,y,z)=(2,0,1)=<0,2,−1>\begin{aligned} { \boldsymbol{\nabla} } F(2,0,1) &= \left< F_x(x,y,z),F_y(x,y,z),F_z(x,y,z)\right>\Big|_{(x,y,z)=(2,0,1)} \\ &= \left< ye^{xy},xe^{xy},-1\right>\Big|_{(x,y,z)=(2,0,1)} \\ &= \left< 0,2,-1\right> \end{aligned}

is a normal vector to the graph at (2,0,1)(2,0,1). So the tangent plane is

0(x−2)+2(y−0)−(z−1)=0 or 2y−z=−10(x-2)+2(y-0)-(z-1)=0\text{ or } 2y-z=-1

and the normal line is

<x,y,z>=<2,0,1>+t<0,2,−1>\left< x,y,z\right>=\left< 2,0,1\right>+t\left< 0,2,-1\right>

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.5절 · 1번
# 접평면과 선형근사그래프·표 해석보통자동 분류
34.CLP-3 · 2.5절 · 11번대학 수준우리말 번역

곡면 x2+9y2+4z2=17x^2 + 9y^2 + 4z^2 = 17 위의 점 중에서 접평면이 평면 x−8z=0x - 8z = 0 과 평행한 점을 모두 구하세요.

영어 원문 보기

Find all the points on the surface x2+9y2+4z2=17x^2 + 9y^2 + 4z^2 = 17 where the tangent plane is parallel to the plane x−8z=0x - 8z = 0.

정답·풀이 보기

곡면 x2+9y2+4z2=17x^2 + 9y^2 + 4z^2 = 17 의 점 (x,y,z)(x,y,z) 에서의 법선벡터는 <2x , 18y , 8z>\left< 2x\,,\, 18y\,,\,8z\right> 이다. 평면 x−8z=0x - 8z = 0 의 법선벡터는 <1 , 0 , −8>\left< 1\,,\,0\,,\,-8\right> 이다. 따라서 <2x , 18y , 8z>\left< 2x\,,\, 18y\,,\,8z\right> 가 <1 , 0 , −8>\left< 1\,,\,0\,,\,-8\right> 과 평행해야 하며, 즉 <1 , 0 , −8>\left< 1\,,\,0\,,\,-8\right> 의 0이 아닌 상수배여야 한다. 이는 x≠0x\ne 0 이고 y=0y=0, z=−2xz=-2x 일 때마다 성립한다. 또한 (x,y,z)(x,y,z) 가 곡면 x2+9y2+4z2=17x^2 + 9y^2 + 4z^2 = 17 위에 있어야 한다. 따라서 y=0y=0, z=−2xz=-2x 이고

17=x2+9y2+4z2=x2+4(−2x)2=17x2  ⟹  x=±1\begin{aligned} 17= x^2 + 9y^2 + 4z^2 =x^2 +4(-2x)^2=17x^2 \implies x=\pm 1 \end{aligned}

이어야 한다.

따라서 조건을 만족하는 점은 ±(1,0,−2)\pm(1,0,-2) 이다.

원본 교재 풀이(영어)

A normal vector to the surface x2+9y2+4z2=17x^2 + 9y^2 + 4z^2 = 17 at the point (x,y,z)(x,y,z) is <2x , 18y , 8z>\left< 2x\,,\, 18y\,,\,8z\right>. A normal vector to the plane x−8z=0x - 8z = 0 is <1 , 0 , −8>\left< 1\,,\,0\,,\,-8\right>. So we want <2x , 18y , 8z>\left< 2x\,,\, 18y\,,\,8z\right> to be parallel to <1 , 0 , −8>\left< 1\,,\,0\,,\,-8\right>, i.e. to be a nonzero constant times <1 , 0 , −8>\left< 1\,,\,0\,,\,-8\right>. This is the case whenever y=0y=0 and z=−2xz=-2x with x≠0x\ne 0. In addition, we want (x,y,z)(x,y,z) to lie on the surface x2+9y2+4z2=17x^2 + 9y^2 + 4z^2 = 17. So we want y=0y=0, z=−2xz=-2x and

17=x2+9y2+4z2=x2+4(−2x)2=17x2  ⟹  x=±1\begin{aligned} 17= x^2 + 9y^2 + 4z^2 =x^2 +4(-2x)^2=17x^2 \implies x=\pm 1 \end{aligned}

So the allowed points are ±(1,0,−2)\pm(1,0,-2).

한 번 더 — 비슷한 문제 풀기APEX · 12.7절 · 2번
# 접평면과 선형근사계산보통자동 분류
35.CLP-3 · 2.5절 · 13번대학 수준우리말 번역

쌍곡면 z2=4x2+y2−1z^2=4x^2+y^2-1 위의 점 중에서 접평면이 평면 2x−y+z=02x-y+z=0 과 평행한 점을 모두 구하세요.

영어 원문 보기

Find all points on the hyperboloid z2=4x2+y2−1z^2=4x^2+y^2-1 where the tangent plane is parallel to the plane 2x−y+z=02x-y+z=0.

정답·풀이 보기

(x0,y0,z0)(x_0,y_0,z_0) 을 쌍곡면 z2=4x2+y2−1z^2=4x^2+y^2-1 위의 점으로서 접평면이 평면 2x−y+z=02x-y+z=0 과 평행한 점이라 하자. 평면 2x−y+z=02x-y+z=0 의 법선벡터는 <2,−1,1>\left< 2,-1,1\right> 이다. 쌍곡면은 G(x,y,z)=4x2+y2−z2−1G(x,y,z)=4x^2+y^2-z^2-1 이고 ∇G(x,y,z)=<8x,2y,−2z>{ \boldsymbol{\nabla} } G(x,y,z) = \left< 8x,2y,-2z\right> 이므로, (x0,y0,z0)(x_0,y_0,z_0) 에서 쌍곡면의 법선벡터는 ∇G(x0,y0,z0)=<8x0,2y0,−2z0>{ \boldsymbol{\nabla} } G(x_0,y_0,z_0)=\left< 8x_0,2y_0,-2z_0\right> 이다. 따라서 (x0,y0,z0)(x_0,y_0,z_0) 이 주어진 조건을 만족할 필요충분조건은 다음을 만족하는 0이 아닌 tt 가 존재하는 것이다.

<8x0,2y0,−2z0>=t<2,−1,1> 그리고 z02=4x02+y02−1  ⟺  x0=t4, y0=z0=−t2 그리고 z02=4x02+y02−1  ⟺  t24=t24+t24−1 그리고 x0=t4, y0=z0=−t2  ⟺  t=±2(x0,y0,z0)=±(12,−1,−1)\begin{aligned} &\left< 8x_0,2y_0,-2z_0\right> =t\left< 2,-1,1\right> \text{ 그리고 } z_0^2=4x_0^2+y_0^2-1\\ &\iff x_0=\frac{t}{4},\ y_0=z_0=-\frac{t}{2}\text{ 그리고 } z_0^2=4x_0^2+y_0^2-1\\ &\iff \frac{t^2}{4}= \frac{t^2}{4}+ \frac{t^2}{4}-1\text{ 그리고 } x_0=\frac{t}{4},\ y_0=z_0=-\frac{t}{2}\\ & \iff t=\pm 2\qquad (x_0,y_0,z_0)=\pm \big(\tfrac{1}{2},-1,-1\big) \end{aligned}

원본 교재 풀이(영어)

Let (x0,y0,z0)(x_0,y_0,z_0) be a point on the hyperboloid z2=4x2+y2−1z^2=4x^2+y^2-1 where the tangent plane is parallel to the plane 2x−y+z=02x-y+z=0. A normal vector to the plane 2x−y+z=02x-y+z=0 is <2,−1,1>\left< 2,-1,1\right>. Because the hyperboloid is G(x,y,z)=4x2+y2−z2−1G(x,y,z)=4x^2+y^2-z^2-1 and ∇G(x,y,z)=<8x,2y,−2z>{ \boldsymbol{\nabla} } G(x,y,z) = \left< 8x,2y,-2z\right>, a normal vector to the hyperboloid at (x0,y0,z0)(x_0,y_0,z_0) is ∇G(x0,y0,z0)=<8x0,2y0,−2z0>{ \boldsymbol{\nabla} } G(x_0,y_0,z_0)=\left< 8x_0,2y_0,-2z_0\right>. So (x0,y0,z0)(x_0,y_0,z_0) satisfies the required conditions if and only if there is a nonzero tt obeying

<8x0,2y0,−2z0>=t<2,−1,1> and z02=4x02+y02−1  ⟺  x0=t4, y0=z0=−t2 and z02=4x02+y02−1  ⟺  t24=t24+t24−1 and x0=t4, y0=z0=−t2  ⟺  t=±2(x0,y0,z0)=±(12,−1,−1)\begin{aligned} &\left< 8x_0,2y_0,-2z_0\right> =t\left< 2,-1,1\right> \text{ and } z_0^2=4x_0^2+y_0^2-1\\ &\iff x_0=\frac{t}{4},\ y_0=z_0=-\frac{t}{2}\text{ and } z_0^2=4x_0^2+y_0^2-1\\ &\iff \frac{t^2}{4}= \frac{t^2}{4}+ \frac{t^2}{4}-1\text{ and } x_0=\frac{t}{4},\ y_0=z_0=-\frac{t}{2}\\ & \iff t=\pm 2\qquad (x_0,y_0,z_0)=\pm \big(\tfrac{1}{2},-1,-1\big) \end{aligned}

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.5절 · 11번
# 접평면과 선형근사계산보통자동 분류
36.CLP-3 · 2.5절 · 14번대학 수준우리말 번역

두 곡면  z2=4x2+9y2 \ z^2=4x^2+9y^2\ 과  6x+3y+2z=5 \ 6x+3y+2z=5\ 의 교선에 접하고 길이가 3\sqrt{3} 인 벡터를 점  (2,1,−5)\ (2,1,-5) 에서 구하세요.

영어 원문 보기

Find a vector of length 3\sqrt{3} which is tangent to the curve of intersection of the surfaces  z2=4x2+9y2 \ z^2=4x^2+9y^2\ and  6x+3y+2z=5 \ 6x+3y+2z=5\ at  (2,1,−5)\ (2,1,-5).

정답·풀이 보기

점 (2,1,−5)(2,1,-5) 에서 곡면 F(x,y,z)=4x2+9y2−z2=0F(x,y,z)=4x^2+9y^2-z^2=0 에 수직인 벡터 하나는 다음과 같다.

∇F(2,1,−5)=<8x,18y,−2z>∣(2,1,−5)=<16,18,10>\begin{aligned} { \boldsymbol{\nabla} } F(2,1,-5) = \left< 8x,18y,-2z\right>\Big|_{(2,1,-5)}=\left< 16,18,10\right> \end{aligned}

점 (2,1,−5)(2,1,-5) 에서 곡면 G(x,y,z)=6x+3y+2z=5G(x,y,z)=6x+3y+2z=5 에 수직인 벡터 하나는 다음과 같다.

∇G(2,1,−5)=<6,3,2>\begin{aligned} { \boldsymbol{\nabla} } G(2,1,-5) = \left< 6,3,2\right> \end{aligned}

이제

  • 곡선은 곡면 z2=4x2+9y2z^2=4x^2+9y^2 위에 있다. 따라서 점 (2,1,−5)(2,1,-5) 에서 곡선의 접벡터는 법선벡터 12<16,18,10>=<8,9,5>\frac{1}{2}\left< 16,18,10\right>=\left< 8,9,5\right> 에 수직이다.
  • 곡선은 곡면 6x+3y+2z=56x+3y+2z=5 위에도 있다. 따라서 점 (2,1,−5)(2,1,-5) 에서 곡선의 접벡터는 법선벡터 <6,3,2>\left< 6,3,2\right> 에도 수직이다.
  • 따라서 점 (2,1,−5)(2,1,-5) 에서 곡선의 접벡터는 다음 벡터와 평행하다.

<8,9,5>×<6,3,2>=det⁡[ı^ȷ^k^895632]=<3,14,−30>\begin{aligned} \left< 8,9,5\right>\times \left< 6,3,2\right> =\det\left[\begin{matrix} \hat{\boldsymbol{\imath}} & \hat{\boldsymbol{\jmath}} & \hat{\mathbf{k}} \\ 8 & 9 & 5 \\ 6 & 3 & 2 \end{matrix}\right] =\left< 3,14,-30\right> \end{aligned}

구하는 벡터는 다음과 같다.

±3<3,14,−30>∣<3,14,−30>∣=±31105<3,14,−30>\pm\sqrt{3}\frac{\left< 3,14,-30\right>}{|\left< 3,14,-30\right>|} =\pm\sqrt{\frac{3}{1105}}\left< 3,14,-30\right>

원본 교재 풀이(영어)

One vector normal to the surface F(x,y,z)=4x2+9y2−z2=0F(x,y,z)=4x^2+9y^2-z^2=0 at (2,1,−5)(2,1,-5) is

∇F(2,1,−5)=<8x,18y,−2z>∣(2,1,−5)=<16,18,10>\begin{aligned} { \boldsymbol{\nabla} } F(2,1,-5) = \left< 8x,18y,-2z\right>\Big|_{(2,1,-5)}=\left< 16,18,10\right> \end{aligned}

One vector normal to the surface G(x,y,z)=6x+3y+2z=5G(x,y,z)=6x+3y+2z=5 at (2,1,−5)(2,1,-5) is

∇G(2,1,−5)=<6,3,2>\begin{aligned} { \boldsymbol{\nabla} } G(2,1,-5) = \left< 6,3,2\right> \end{aligned}

Now

  • The curve lies in the surface z2=4x2+9y2z^2=4x^2+9y^2. So the tangent vector to the curve at (2,1,−5)(2,1,-5) is perpendicular to the normal vector 12<16,18,10>=<8,9,5>\frac{1}{2}\left< 16,18,10\right>=\left< 8,9,5\right>.
  • The curve also lies in the surface 6x+3y+2z=56x+3y+2z=5. So the tangent vector to the curve at (2,1,−5)(2,1,-5) is also perpendicular to the normal vector <6,3,2>\left< 6,3,2\right>.
  • So the tangent vector to the curve at (2,1,−5)(2,1,-5) is parallel to

<8,9,5>×<6,3,2>=det⁡[ı^ȷ^k^895632]=<3,14,−30>\begin{aligned} \left< 8,9,5\right>\times \left< 6,3,2\right> =\det\left[\begin{matrix} \hat{\boldsymbol{\imath}} & \hat{\boldsymbol{\jmath}} & \hat{\mathbf{k}} \\ 8 & 9 & 5 \\ 6 & 3 & 2 \end{matrix}\right] =\left< 3,14,-30\right> \end{aligned}

The desired vectors are

±3<3,14,−30>∣<3,14,−30>∣=±31105<3,14,−30>\pm\sqrt{3}\frac{\left< 3,14,-30\right>}{|\left< 3,14,-30\right>|} =\pm\sqrt{\frac{3}{1105}}\left< 3,14,-30\right>

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.5절 · 15번
# 접평면과 선형근사계산보통자동 분류
37.CLP-3 · 2.6절 · 3번대학 수준우리말 번역

계산기나 컴퓨터를 사용하지 않고 f(x,y)=sin⁡(πxy+ln⁡y)f(x,y)=\sin(\pi xy+\ln y) 의 (0.01,1.05)(0.01,1.05) 에서의 근삿값을 구하세요.

영어 원문 보기

Find an approximate value for f(x,y)=sin⁡(πxy+ln⁡y)f(x,y)=\sin(\pi xy+\ln y) at (0.01,1.05)(0.01,1.05) without using a calculator or computer.

답 쓰고 채점
정답·풀이 보기

선형 근사 f(0.01,1.05)≈f(0,1)+fx(0,1)(0.01)+fy(0,1)(0.05)f(0.01,1.05)\approx f(0,1)+f_x(0,1)(0.01)+f_y(0,1)(0.05) 를 적용한다. 이때

f(x,y)=sin⁡(πxy+ln⁡y)f(0,1)=sin⁡0=0fx(x,y)=πycos⁡(πxy+ln⁡y)fx(0,1)=πcos⁡0=πfy(x,y)=(πx+1y)cos⁡(πxy+ln⁡y)fy(0,1)=cos⁡0=1\begin{aligned} f(x,y)&=\sin(\pi xy+\ln y) & f(0,1)&=\sin 0=0\\ f_x(x,y)&=\pi y\cos(\pi xy+\ln y) & f_x(0,1)&=\pi\cos 0=\pi\\ f_y(x,y)&=\left(\pi x+\frac{1}{y}\right)\cos(\pi xy+\ln y) & f_y(0,1)&=\cos 0=1 \end{aligned}

이다. 따라서

f(0.01,1.05)≈f(0,1)+fx(0,1)(0.01)+fy(0,1)(0.05)=0+π(0.01)+1(0.05)=0.01 π+0.05≈0.0814\begin{aligned} f(0.01,1.05)&\approx f(0,1)+f_x(0,1)(0.01)+f_y(0,1)(0.05) =0+\pi(0.01)+1(0.05) \\ &=0.01\,\pi + 0.05 \approx 0.0814 \end{aligned}

이다.

원본 교재 풀이(영어)

Apply the linear approximation f(0.01,1.05)≈f(0,1)+fx(0,1)(0.01)+fy(0,1)(0.05)f(0.01,1.05)\approx f(0,1)+f_x(0,1)(0.01)+f_y(0,1)(0.05), with

f(x,y)=sin⁡(πxy+ln⁡y)f(0,1)=sin⁡0=0fx(x,y)=πycos⁡(πxy+ln⁡y)fx(0,1)=πcos⁡0=πfy(x,y)=(πx+1y)cos⁡(πxy+ln⁡y)fy(0,1)=cos⁡0=1\begin{aligned} f(x,y)&=\sin(\pi xy+\ln y) & f(0,1)&=\sin 0=0\\ f_x(x,y)&=\pi y\cos(\pi xy+\ln y) & f_x(0,1)&=\pi\cos 0=\pi\\ f_y(x,y)&=\left(\pi x+\frac{1}{y}\right)\cos(\pi xy+\ln y) & f_y(0,1)&=\cos 0=1 \end{aligned}

This gives

f(0.01,1.05)≈f(0,1)+fx(0,1)(0.01)+fy(0,1)(0.05)=0+π(0.01)+1(0.05)=0.01 π+0.05≈0.0814\begin{aligned} f(0.01,1.05)&\approx f(0,1)+f_x(0,1)(0.01)+f_y(0,1)(0.05) =0+\pi(0.01)+1(0.05) \\ &=0.01\,\pi + 0.05 \approx 0.0814 \end{aligned}

한 번 더 — 비슷한 문제 풀기OpenStax 3권 · 4.4절 · 39번
# 접평면과 선형근사계산보통자동 분류
38.CLP-3 · 2.6절 · 4번대학 수준우리말 번역

f(x,y)=x2yx4+2y2\displaystyle f(x,y)=\frac{x^2y}{x^4+2y^2} 라 하자. 계산기나 컴퓨터를 사용하지 않고 f(−0.9 , 1.1)f (-0.9\,,\, 1.1) 의 근삿값을 구하세요.

영어 원문 보기

Let f(x,y)=x2yx4+2y2\displaystyle f(x,y)=\frac{x^2y}{x^4+2y^2}. Find an approximate value for f(−0.9 , 1.1)f (-0.9\,,\, 1.1) without using a calculator or computer.

답 쓰고 채점
정답·풀이 보기

(x,y)=(−1,1)(x,y)=(-1,1) 에서 f(x,y)f(x,y) 의 1계 미분계수가 필요하다. 그래서 먼저 이를 구한다.

fx(x,y)=2xyx4+2y2−x2y(4x3)(x4+2y2)2fx(−1,1)=−23+432=−29fy(x,y)=x2x4+2y2−x2y(4y)(x4+2y2)2fy(−1,1)=13−432=−19\begin{aligned} f_x(x,y)&=\frac{2xy}{x^4+2y^2}-\frac{x^2y(4x^3)}{{(x^4+2y^2)}^2}\qquad & f_x(-1,1)&=-\frac{2}{3} +\frac{4}{3^2}=-\frac{2}{9} \\ f_y(x,y)&=\frac{x^2}{x^4+2y^2}-\frac{x^2y(4y)}{{(x^4+2y^2)}^2}\qquad & f_y(-1,1)&=\frac{1}{3} -\frac{4}{3^2}=-\frac{1}{9} \end{aligned}

(−1,1)(-1,1) 근처에서 f(x,y)f(x,y) 의 선형 근사는 다음과 같다.

f(x,y)≈=f(−1,1)+fx(−1,1) (x+1)+fy(−1,1) (y−1)=13−29 (x+1)−19 (y−1)\begin{aligned} f(x,y)\approx=f(-1,1) + f_x(-1,1)\,(x+1) + f_y(-1,1)\,(y-1) =\frac{1}{3} -\frac{2}{9}\,(x+1) -\frac{1}{9}\,(y-1) \end{aligned}

특히

f(−0.9,1.1)≈13−29 (0.1)−19 (0.1)=2790=0.3\begin{aligned} f(-0.9,1.1)\approx \frac{1}{3} -\frac{2}{9}\,(0.1) -\frac{1}{9}\,(0.1) =\frac{27}{90}=0.3 \end{aligned}

원본 교재 풀이(영어)

We are going to need the first order derivatives of f(x,y)f(x,y) at (x,y)=(−1,1)(x,y)=(-1,1). So we find them first.

fx(x,y)=2xyx4+2y2−x2y(4x3)(x4+2y2)2fx(−1,1)=−23+432=−29fy(x,y)=x2x4+2y2−x2y(4y)(x4+2y2)2fy(−1,1)=13−432=−19\begin{aligned} f_x(x,y)&=\frac{2xy}{x^4+2y^2}-\frac{x^2y(4x^3)}{{(x^4+2y^2)}^2}\qquad & f_x(-1,1)&=-\frac{2}{3} +\frac{4}{3^2}=-\frac{2}{9} \\ f_y(x,y)&=\frac{x^2}{x^4+2y^2}-\frac{x^2y(4y)}{{(x^4+2y^2)}^2}\qquad & f_y(-1,1)&=\frac{1}{3} -\frac{4}{3^2}=-\frac{1}{9} \end{aligned}

The linear approximation to f(x,y)f(x,y) about (−1,1)(-1,1) is

f(x,y)≈=f(−1,1)+fx(−1,1) (x+1)+fy(−1,1) (y−1)=13−29 (x+1)−19 (y−1)\begin{aligned} f(x,y)\approx=f(-1,1) + f_x(-1,1)\,(x+1) + f_y(-1,1)\,(y-1) =\frac{1}{3} -\frac{2}{9}\,(x+1) -\frac{1}{9}\,(y-1) \end{aligned}

In particular

f(−0.9,1.1)≈13−29 (0.1)−19 (0.1)=2790=0.3\begin{aligned} f(-0.9,1.1)\approx \frac{1}{3} -\frac{2}{9}\,(0.1) -\frac{1}{9}\,(0.1) =\frac{27}{90}=0.3 \end{aligned}

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.6절 · 3번
# 접평면과 선형근사계산보통자동 분류
39.CLP-3 · 2.6절 · 6번대학 수준우리말 번역

직각삼각형의 한 변의 길이를 측정했더니 33 이고 최대 오차는 ±0.1\pm 0.1 이며, 다른 한 변의 길이는 44 이고 최대 오차는 ±0.2\pm 0.2 이다. 선형 근사를 이용하여 이 직각삼각형의 빗변의 길이를 계산할 때 생길 수 있는 최대 오차를 어림하세요.

영어 원문 보기

One side of a right triangle is measured to be 33 with a maximum possible error of ±0.1\pm 0.1, and the other side is measured to be 44 with a maximum possible error of ±0.2\pm 0.2. Use the linear approximation to estimate the maximum possible error in calculating the length of the hypotenuse of the right triangle.

답 쓰고 채점
정답·풀이 보기

두 변의 길이를 xx, yy 라 하면 x=3±0.1x=3\pm 0.1, y=4±0.2y=4\pm 0.2 이다. 그러면 빗변의 길이는 f(x,y)=x2+y2f(x,y)=\sqrt{x^2+y^2} 이다. 다음과 같다.

f(x,y)=x2+y2f(3,4)=5fx(x,y)=xx2+y2fx(3,4)=35fy(x,y)=yx2+y2fy(3,4)=45\begin{aligned} f(x,y)&=\sqrt{x^2+y^2} & f(3,4)&=5 \\ f_x(x,y)&=\frac{x}{\sqrt{x^2+y^2}}\qquad & f_x(3,4)&=\frac{3}{5} \\ f_y(x,y)&=\frac{y}{\sqrt{x^2+y^2}} & f_y(3,4)&=\frac{4}{5} \end{aligned}

선형 근사에 의해

f(x,y)≈f(3,4)+fx(3,4) (x−3)+fy(3,4) (y−4)=5+35 (x−3)+45 (y−4)\begin{aligned} f(x,y)\approx f(3,4) + f_x(3,4)\,(x-3) + f_y(3,4)\,(y-4) =5 +\frac{3}{5}\,(x-3) +\frac{4}{5}\,(y-4) \end{aligned}

따라서 빗변의 길이를 계산할 때 생기는 최대 오차의 근삿값은

35 (0.1)+45 (0.2)=1.15=0.22\begin{aligned} \frac{3}{5}\,(0.1) +\frac{4}{5}\,(0.2) =\frac{1.1}{5} = 0.22 \end{aligned}

이다.

원본 교재 풀이(영어)

Denote by xx and yy the lengths of sides with x=3±0.1x=3\pm 0.1 and y=4±0.2y=4\pm 0.2. Then the length of the hypotenuse is f(x,y)=x2+y2f(x,y)=\sqrt{x^2+y^2}. Note that

f(x,y)=x2+y2f(3,4)=5fx(x,y)=xx2+y2fx(3,4)=35fy(x,y)=yx2+y2fy(3,4)=45\begin{aligned} f(x,y)&=\sqrt{x^2+y^2} & f(3,4)&=5 \\ f_x(x,y)&=\frac{x}{\sqrt{x^2+y^2}}\qquad & f_x(3,4)&=\frac{3}{5} \\ f_y(x,y)&=\frac{y}{\sqrt{x^2+y^2}} & f_y(3,4)&=\frac{4}{5} \end{aligned}

By the linear approximation

f(x,y)≈f(3,4)+fx(3,4) (x−3)+fy(3,4) (y−4)=5+35 (x−3)+45 (y−4)\begin{aligned} f(x,y)\approx f(3,4) + f_x(3,4)\,(x-3) + f_y(3,4)\,(y-4) =5 +\frac{3}{5}\,(x-3) +\frac{4}{5}\,(y-4) \end{aligned}

So the approximate maximum error in calculating the length of the hypotenuse is

35 (0.1)+45 (0.2)=1.15=0.22\begin{aligned} \frac{3}{5}\,(0.1) +\frac{4}{5}\,(0.2) =\frac{1.1}{5} = 0.22 \end{aligned}

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.6절 · 7번
# 접평면과 선형근사계산보통자동 분류
40.CLP-3 · 2.6절 · 7번대학 수준우리말 번역

저항이 R1R_1, R2R_2 인 두 저항을 병렬로 연결하면, 합성 저항 R 은 방정식 1R=1R1+1R2\frac{1}{R} =\frac{1}{R_1}+\frac{1}{R_2} 을 만족시킨다. 선형 근사를 이용하여 R1R_1 이 22 옴에서 1.91.9 옴으로 감소하고 R2R_2 가 8 옴에서 8.1 옴으로 증가할 때 RR 의 변화량을 어림하세요.

영어 원문 보기

If two resistors of resistance R1R_1 and R2R_2 are wired in parallel, then the resulting resistance R satisfies the equation 1R=1R1+1R2\frac{1}{R} =\frac{1}{R_1}+\frac{1}{R_2}. Use the linear approximation to estimate the change in RR if R1R_1 decreases from 22 to 1.91.9 ohms and R2R_2 increases from 8 to 8.1 ohms.

답 쓰고 채점
정답·풀이 보기

함수 R(R1,R2)R(R_1,R_2) 는 다음 식으로 음함수로 정의된다.

1R(R1,R2)=1R1+1R2(∗)\frac{1}{R(R_1,R_2)} =\frac{1}{R_1}+\frac{1}{R_2} \tag{$*$}

특히

1R(2,8)=12+18=58  ⟹  R(2,8)=85\frac{1}{R(2,8)} = \frac{1}{2}+\frac{1}{8} = \frac{5}{8} \implies R(2,8) = \frac{8}{5}

다음 선형 근사를 이용하고자 한다.

R(R1,R2)≈R(2,8)+∂R∂R1(2,8) (R1−2)+∂R∂R2(2,8) (R2−8)R(R_1,R_2) \approx R(2,8) + \frac{\partial R}{\partial R_1}(2,8)\,(R_1-2) + \frac{\partial R}{\partial R_2}(2,8)\,(R_2-8)

그러기 위해서는 편도함수 ∂R∂R1(2,8)\frac{\partial R}{\partial R_1}(2,8) 와 ∂R∂R2(2,8)\frac{\partial R}{\partial R_2}(2,8) 가 필요하다. 이를 구하기 위해 (∗)(*) 를 R1R_1 과 R2R_2 에 대해 각각 미분한다.

−1R(R1,R2)2∂R∂R1(R1,R2)=−1R12−1R(R1,R2)2∂R∂R2(R1,R2)=−1R22\begin{aligned} -\frac{1}{R(R_1,R_2)^2}\frac{\partial R}{\partial R_1}(R_1,R_2) &= -\frac{1}{R_1^2} \\ -\frac{1}{R(R_1,R_2)^2}\frac{\partial R}{\partial R_2}(R_1,R_2) &= -\frac{1}{R_2^2} \\ \end{aligned}

R1=2R_1=2, R2=8R_2=8 을 대입하면

−1(8/5)2∂R∂R1(2,8)=−14  ⟹  ∂R∂R1(2,8)=1625−1(8/5)2∂R∂R2(2,8)=−164  ⟹  ∂R∂R2(2,8)=125\begin{aligned} -\frac{1}{(8/5)^2}\frac{\partial R}{\partial R_1}(2,8) &= -\frac{1}{4} &\quad\implies\quad & &\frac{\partial R}{\partial R_1}(2,8) &=\frac{16}{25} \\ -\frac{1}{(8/5)^2}\frac{\partial R}{\partial R_2}(2,8) &= -\frac{1}{64} &\quad\implies\quad & &\frac{\partial R}{\partial R_2}(2,8) &=\frac{1}{25} \end{aligned}

따라서 RR 의 변화량은 다음과 같다.

R(1.9,8.1)−R(2,8)≈1625(−0.1)+125(0.1)=−15250=−0.06\begin{aligned} R(1.9,8.1)-R(2,8) \approx \frac{16}{25} (-0.1) + \frac{1}{25}(0.1) =-\frac{15}{250} = -0.06 \end{aligned}

원본 교재 풀이(영어)

The function R(R1,R2)R(R_1,R_2) is defined implictly by

1R(R1,R2)=1R1+1R2(∗)\frac{1}{R(R_1,R_2)} =\frac{1}{R_1}+\frac{1}{R_2} \tag{$*$}

In particular

1R(2,8)=12+18=58  ⟹  R(2,8)=85\frac{1}{R(2,8)} = \frac{1}{2}+\frac{1}{8} = \frac{5}{8} \implies R(2,8) = \frac{8}{5}

We wish to use the linear approximation

R(R1,R2)≈R(2,8)+∂R∂R1(2,8) (R1−2)+∂R∂R2(2,8) (R2−8)R(R_1,R_2) \approx R(2,8) + \frac{\partial R}{\partial R_1}(2,8)\,(R_1-2) + \frac{\partial R}{\partial R_2}(2,8)\,(R_2-8)

To do so, we need the partial derivatives ∂R∂R1(2,8)\frac{\partial R}{\partial R_1}(2,8) and ∂R∂R2(2,8)\frac{\partial R}{\partial R_2}(2,8). To find them, we differentiate (∗)(*) with respect to R1R_1 and R2R_2:

−1R(R1,R2)2∂R∂R1(R1,R2)=−1R12−1R(R1,R2)2∂R∂R2(R1,R2)=−1R22\begin{aligned} -\frac{1}{R(R_1,R_2)^2}\frac{\partial R}{\partial R_1}(R_1,R_2) &= -\frac{1}{R_1^2} \\ -\frac{1}{R(R_1,R_2)^2}\frac{\partial R}{\partial R_2}(R_1,R_2) &= -\frac{1}{R_2^2} \\ \end{aligned}

Setting R1=2R_1=2 and R2=8R_2=8 gives

−1(8/5)2∂R∂R1(2,8)=−14  ⟹  ∂R∂R1(2,8)=1625−1(8/5)2∂R∂R2(2,8)=−164  ⟹  ∂R∂R2(2,8)=125\begin{aligned} -\frac{1}{(8/5)^2}\frac{\partial R}{\partial R_1}(2,8) &= -\frac{1}{4} &\quad\implies\quad & &\frac{\partial R}{\partial R_1}(2,8) &=\frac{16}{25} \\ -\frac{1}{(8/5)^2}\frac{\partial R}{\partial R_2}(2,8) &= -\frac{1}{64} &\quad\implies\quad & &\frac{\partial R}{\partial R_2}(2,8) &=\frac{1}{25} \end{aligned}

So the specified change in RR is

R(1.9,8.1)−R(2,8)≈1625(−0.1)+125(0.1)=−15250=−0.06\begin{aligned} R(1.9,8.1)-R(2,8) \approx \frac{16}{25} (-0.1) + \frac{1}{25}(0.1) =-\frac{15}{250} = -0.06 \end{aligned}

한 번 더 — 비슷한 문제 풀기CLP-3 · 2.6절 · 4번
# 접평면과 선형근사계산보통자동 분류