문제 은행 · 미적분 · 대학 미적분 · 다변수 미분

다변수 연쇄법칙

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

CLP-3 · 2.4절 · 7번대학 수준우리말 번역

∂3∂x∂y2f(2x+3y,xy)\frac{\partial^3}{\partial x\partial y^2}f(2x+3y,xy) 의 값을 ff 의 편도함수로 나타내어 구하세요. 연쇄 법칙과, 혼합 편도함수가 서로 같음을 나타내는 클레로의 정리를 적용할 수 있도록 ff 는 매끄러운 함수라고 가정해도 됩니다.

영어 원문 보기

Evaluate ∂3∂x∂y2f(2x+3y,xy)\frac{\partial^3}{\partial x\partial y^2}f(2x+3y,xy) in terms of partial derivatives of ff. You may assume that ff is a smooth function so that the Chain Rule and Clairaut's Theorem on the equality of the mixed partial derivatives apply.

정답·풀이 보기

정의에 따라

∂3∂x∂y2f(2x+3y,xy)=∂∂x[∂∂y(∂∂yf(2x+3y,xy))]\frac{\partial^3}{\partial x\partial y^2}f(2x+3y,xy) =\frac{\partial }{\partial x}\left[\frac{\partial }{\partial y}\left(\frac{\partial }{\partial y}f(2x+3y,xy)\right) \right]

이다.

안쪽부터 차례로 편도함수를 계산한다. F(x,y)=f(2x+3y,xy)F(x,y)=f(2x+3y,xy) 라 하면 가장 안쪽의 편도함수는 G(x,y)=∂∂yf(2x+3y,xy)=∂∂yF(x,y)G(x,y)=\frac{\partial }{\partial y}f(2x+3y,xy)=\frac{\partial }{\partial y}F(x,y) 이다. 연쇄 법칙에 의해

G(x,y)=∂∂yF(x,y)=f1(2x+3y,xy)∂∂y(2x+3y)+f2(2x+3y,xy)∂∂y(xy)=3f1(2x+3y,xy)+xf2(2x+3y,xy)\begin{aligned} G(x,y)=\frac{\partial }{\partial y}F(x,y) &=f_1(2x+3y,xy)\frac{\partial }{\partial y}(2x+3y)+f_2(2x+3y,xy)\frac{\partial }{\partial y}(xy) \\ &= 3f_1(2x+3y,xy)+xf_2(2x+3y,xy) \end{aligned}

이다.

여기서 아래첨자 11 은 두 번째 변수를 고정한 채 ff 를 첫 번째 변수에 대해 편미분한다는 뜻이고, 아래첨자 22 는 첫 번째 변수를 고정한 채 ff 를 두 번째 변수에 대해 편미분한다는 뜻이다. 다음으로 가운데 편도함수를 H(x,y)=∂∂y(∂∂yf(2x+3y,xy))H(x,y)=\frac{\partial }{\partial y}\left(\frac{\partial }{\partial y}f(2x+3y,xy)\right) 라 하면

H(x,y)=∂∂yG(x,y)=∂∂y(3f1(2x+3y,xy)+xf2(2x+3y,xy))=3∂∂y(f1(2x+3y,xy))+x∂∂y(f2(2x+3y,xy))\begin{aligned} H(x,y) &= \frac{\partial }{\partial y} G(x,y) \\ &=\frac{\partial }{\partial y}\Big(3f_1(2x+3y,xy)+xf_2(2x+3y,xy)\Big) \\ &=3\frac{\partial }{\partial y}\Big(f_1(2x+3y,xy)\Big) +x\frac{\partial }{\partial y}\Big(f_2(2x+3y,xy)\Big) \end{aligned}

이다.

연쇄 법칙을 (두 번) 쓰면

∂∂y(f1(2x+3y,xy))=f11(2x+3y,xy)∂∂y(2x+3y)+f12(2x+3y,xy)∂∂y(xy)=3f11(2x+3y,xy)+xf12(2x+3y,xy)∂∂y(f2(2x+3y,xy))=f21(2x+3y,xy)∂∂y(2x+3y)+f22(2x+3y,xy)∂∂y(xy)=3f21(2x+3y,xy)+xf22(2x+3y,xy)\begin{aligned} \frac{\partial }{\partial y}\Big(f_1(2x+3y,xy)\Big) &=f_{11}(2x+3y,xy)\frac{\partial }{\partial y}(2x+3y)+f_{12}(2x+3y,xy)\frac{\partial }{\partial y}(xy) \\ &= 3f_{11}(2x+3y,xy)+xf_{12}(2x+3y,xy) \\ \frac{\partial }{\partial y}\Big(f_2(2x+3y,xy)\Big) &=f_{21}(2x+3y,xy)\frac{\partial }{\partial y}(2x+3y)+f_{22}(2x+3y,xy)\frac{\partial }{\partial y}(xy) \\ &= 3f_{21}(2x+3y,xy)+xf_{22}(2x+3y,xy) \end{aligned}

이므로

H(x,y)=3(3f11(2x+3y,xy)+xf12(2x+3y,xy))+x(3f21(2x+3y,xy)+xf22(2x+3y,xy))=9f11(2x+3y,xy)+6xf12(2x+3y,xy)+x2f22(2x+3y,xy)\begin{aligned} H(x,y)&=3\Big(3f_{11}(2x+3y,xy)+xf_{12}(2x+3y,xy) \Big) \\[-0.05in] & +x\Big(3f_{21}(2x+3y,xy)+xf_{22}(2x+3y,xy)\Big) \\ &=9f_{11}(2x+3y,xy)+6xf_{12}(2x+3y,xy)+x^2f_{22}(2x+3y,xy) \end{aligned}

이다.

마지막 등호에서는 f21(2x+3y,xy)=f12(2x+3y,xy)f_{21}(2x+3y,xy)=f_{12}(2x+3y,xy) 임을 이용했다. 기호 f21f_{21} 은 먼저 두 번째 변수에 대해 미분한 다음 첫 번째 변수에 대해 미분한다는 뜻이다. 예를 들어 f(x,y)=e2ysin⁡xf(x,y)=e^{2y}\sin x 이면

f21(x,y)=∂∂x[∂∂y(e2ysin⁡x)]=∂∂x[2e2ysin⁡x]=2eycos⁡x\begin{aligned} f_{21}(x,y) =\frac{\partial }{\partial x} \Big[\frac{\partial }{\partial y}\big(e^{2y}\sin x\big)\Big] =\frac{\partial }{\partial x} \Big[2e^{2y}\sin x\Big] =2e^y\cos x \end{aligned}

이다.

마지막으로

∂3∂x∂y2f(2x+3y,xy)=∂∂xH(x,y)=∂∂x(9f11(2x+3y,xy)+6xf12(2x+3y,xy)+x2f22(2x+3y,xy))=9∂∂x(f11(2x+3y,xy))+6f12(2x+3y,xy)+6x∂∂x(f12(2x+3y,xy))+2xf22(2x+3y,xy)+x2∂∂x(f22(2x+3y,xy))\begin{aligned} \frac{\partial^3}{\partial x\partial y^2}f(2x+3y,xy) &=\frac{\partial }{\partial x} H(x,y) \\ &=\frac{\partial }{\partial x}\Big(9f_{11}(2x+3y,xy)+6xf_{12}(2x+3y,xy)+x^2f_{22}(2x+3y,xy)\Big)\\ &=9\frac{\partial }{\partial x}\Big(f_{11}(2x+3y,xy)\Big)\\& +6f_{12}(2x+3y,xy) +6x\frac{\partial }{\partial x}\Big(f_{12}(2x+3y,xy)\Big) \\& +2xf_{22}(2x+3y,xy) +x^2\frac{\partial }{\partial x}\Big(f_{22}(2x+3y,xy)\Big) \end{aligned}

이다.

연쇄 법칙을 세 번 적용하면

∂3∂x∂y2f(2x+3y,xy)=9(2f111+yf112)+6f12+6x(2f121+yf122)+2xf22+x2(2f221+yf222)=6 f12+2x f22+18 f111+(9y+12x) f112+(6xy+2x2) f122+x2y f222\begin{aligned} \frac{\partial^3}{\partial x\partial y^2}f(2x+3y,xy) &=9\Big(2f_{111}+yf_{112}\Big)\\& +6f_{12}+6x\Big(2f_{121}+yf_{122}\Big)\\& +2xf_{22}+x^2\Big(2f_{221}+yf_{222}\Big)\\ &=6\,f_{12}+2x\,f_{22}+18\,f_{111}+(9y+12x)\,f_{112} +(6xy+2x^2)\,f_{122}+x^2y\,f_{222} \end{aligned}

이다.

우변의 모든 함수의 인수는 (2x+3y,xy)(2x+3y,xy) 이다.

원본 교재 풀이(영어)

By definition,

∂3∂x∂y2f(2x+3y,xy)=∂∂x[∂∂y(∂∂yf(2x+3y,xy))]\frac{\partial^3}{\partial x\partial y^2}f(2x+3y,xy) =\frac{\partial }{\partial x}\left[\frac{\partial }{\partial y}\left(\frac{\partial }{\partial y}f(2x+3y,xy)\right) \right]

We'll compute the derivatives from the inside out. Let's call F(x,y)=f(2x+3y,xy)F(x,y)=f(2x+3y,xy) so that the innermost derivative is G(x,y)=∂∂yf(2x+3y,xy)=∂∂yF(x,y)G(x,y)=\frac{\partial }{\partial y}f(2x+3y,xy)=\frac{\partial }{\partial y}F(x,y). By the chain rule

G(x,y)=∂∂yF(x,y)=f1(2x+3y,xy)∂∂y(2x+3y)+f2(2x+3y,xy)∂∂y(xy)=3f1(2x+3y,xy)+xf2(2x+3y,xy)\begin{aligned} G(x,y)=\frac{\partial }{\partial y}F(x,y) &=f_1(2x+3y,xy)\frac{\partial }{\partial y}(2x+3y)+f_2(2x+3y,xy)\frac{\partial }{\partial y}(xy) \\ &= 3f_1(2x+3y,xy)+xf_2(2x+3y,xy) \end{aligned}

Here the subscript 11 means take the partial derivative of ff with respect to the first argument while holding the second argument fixed, and the subscript 22 means take the partial derivative of ff with respect to the second argument while holding the first argument fixed. Next call the middle derivative H(x,y)=∂∂y(∂∂yf(2x+3y,xy))H(x,y)=\frac{\partial }{\partial y}\left(\frac{\partial }{\partial y}f(2x+3y,xy)\right) so that

H(x,y)=∂∂yG(x,y)=∂∂y(3f1(2x+3y,xy)+xf2(2x+3y,xy))=3∂∂y(f1(2x+3y,xy))+x∂∂y(f2(2x+3y,xy))\begin{aligned} H(x,y) &= \frac{\partial }{\partial y} G(x,y) \\ &=\frac{\partial }{\partial y}\Big(3f_1(2x+3y,xy)+xf_2(2x+3y,xy)\Big) \\ &=3\frac{\partial }{\partial y}\Big(f_1(2x+3y,xy)\Big) +x\frac{\partial }{\partial y}\Big(f_2(2x+3y,xy)\Big) \end{aligned}

By the chain rule (twice),

∂∂y(f1(2x+3y,xy))=f11(2x+3y,xy)∂∂y(2x+3y)+f12(2x+3y,xy)∂∂y(xy)=3f11(2x+3y,xy)+xf12(2x+3y,xy)∂∂y(f2(2x+3y,xy))=f21(2x+3y,xy)∂∂y(2x+3y)+f22(2x+3y,xy)∂∂y(xy)=3f21(2x+3y,xy)+xf22(2x+3y,xy)\begin{aligned} \frac{\partial }{\partial y}\Big(f_1(2x+3y,xy)\Big) &=f_{11}(2x+3y,xy)\frac{\partial }{\partial y}(2x+3y)+f_{12}(2x+3y,xy)\frac{\partial }{\partial y}(xy) \\ &= 3f_{11}(2x+3y,xy)+xf_{12}(2x+3y,xy) \\ \frac{\partial }{\partial y}\Big(f_2(2x+3y,xy)\Big) &=f_{21}(2x+3y,xy)\frac{\partial }{\partial y}(2x+3y)+f_{22}(2x+3y,xy)\frac{\partial }{\partial y}(xy) \\ &= 3f_{21}(2x+3y,xy)+xf_{22}(2x+3y,xy) \end{aligned}

so that

H(x,y)=3(3f11(2x+3y,xy)+xf12(2x+3y,xy))+x(3f21(2x+3y,xy)+xf22(2x+3y,xy))=9f11(2x+3y,xy)+6xf12(2x+3y,xy)+x2f22(2x+3y,xy)\begin{aligned} H(x,y)&=3\Big(3f_{11}(2x+3y,xy)+xf_{12}(2x+3y,xy) \Big) \\[-0.05in] & +x\Big(3f_{21}(2x+3y,xy)+xf_{22}(2x+3y,xy)\Big) \\ &=9f_{11}(2x+3y,xy)+6xf_{12}(2x+3y,xy)+x^2f_{22}(2x+3y,xy) \end{aligned}

In the last equality we used that f21(2x+3y,xy)=f12(2x+3y,xy)f_{21}(2x+3y,xy)=f_{12}(2x+3y,xy). The notation f21f_{21} means first differentiate with respect to the second argument and then differentiate with respect to the first argument. For example, if f(x,y)=e2ysin⁡xf(x,y)=e^{2y}\sin x, then

f21(x,y)=∂∂x[∂∂y(e2ysin⁡x)]=∂∂x[2e2ysin⁡x]=2eycos⁡x\begin{aligned} f_{21}(x,y) =\frac{\partial }{\partial x} \Big[\frac{\partial }{\partial y}\big(e^{2y}\sin x\big)\Big] =\frac{\partial }{\partial x} \Big[2e^{2y}\sin x\Big] =2e^y\cos x \end{aligned}

Finally, we get to

∂3∂x∂y2f(2x+3y,xy)=∂∂xH(x,y)=∂∂x(9f11(2x+3y,xy)+6xf12(2x+3y,xy)+x2f22(2x+3y,xy))=9∂∂x(f11(2x+3y,xy))+6f12(2x+3y,xy)+6x∂∂x(f12(2x+3y,xy))+2xf22(2x+3y,xy)+x2∂∂x(f22(2x+3y,xy))\begin{aligned} \frac{\partial^3}{\partial x\partial y^2}f(2x+3y,xy) &=\frac{\partial }{\partial x} H(x,y) \\ &=\frac{\partial }{\partial x}\Big(9f_{11}(2x+3y,xy)+6xf_{12}(2x+3y,xy)+x^2f_{22}(2x+3y,xy)\Big)\\ &=9\frac{\partial }{\partial x}\Big(f_{11}(2x+3y,xy)\Big)\\& +6f_{12}(2x+3y,xy) +6x\frac{\partial }{\partial x}\Big(f_{12}(2x+3y,xy)\Big) \\& +2xf_{22}(2x+3y,xy) +x^2\frac{\partial }{\partial x}\Big(f_{22}(2x+3y,xy)\Big) \end{aligned}

By three applications of the chain rule

∂3∂x∂y2f(2x+3y,xy)=9(2f111+yf112)+6f12+6x(2f121+yf122)+2xf22+x2(2f221+yf222)=6 f12+2x f22+18 f111+(9y+12x) f112+(6xy+2x2) f122+x2y f222\begin{aligned} \frac{\partial^3}{\partial x\partial y^2}f(2x+3y,xy) &=9\Big(2f_{111}+yf_{112}\Big)\\& +6f_{12}+6x\Big(2f_{121}+yf_{122}\Big)\\& +2xf_{22}+x^2\Big(2f_{221}+yf_{222}\Big)\\ &=6\,f_{12}+2x\,f_{22}+18\,f_{111}+(9y+12x)\,f_{112} +(6xy+2x^2)\,f_{122}+x^2y\,f_{222} \end{aligned}

All functions on the right hand side have arguments (2x+3y,xy)(2x+3y,xy).

한 번 더 — 비슷한 문제APEX · 12.5절 · 2번우리말 번역

어떤 u⃗\vec u 에 대해 Du⃗ f=fxD_{\vec u\,} f = f_x 인가요?

다 풀었으면 정답 확인

u⃗=⟨1,0⟩\vec u = \left\langle 1,0\right\rangle

이 문제로 이어서 풀기
# 다변수 연쇄법칙계산보통자동 분류

「다변수 연쇄법칙」 문제 목록으로