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Mathematics · Ch 8 — Differentials and Partial Derivatives

Function of Function Rule

8.6.1

Function of Function Rule

When the two variables x,yx,y of W(x,y)W(x,y) are themselves each functions of a single variable tt (with the same domain), the composite W(x(t),y(t))W(x(t),y(t)) ultimately depends only on tt — so it should be treatable as an ordinary one-variable function, and its derivative dWdt\dfrac{dW}{dt} should be computable. This is not a coincidence:

Theorem 8.2 (Function of Function Rule). Suppose W(x,y)W(x,y) has partial derivatives ∂W∂x,∂W∂y\dfrac{\partial W}{\partial x},\dfrac{\partial W}{\partial y}. If x,yx,y are both differentiable functions of a single variable tt, then WW is a differentiable function of tt, and

dWdt=∂W∂xdxdt+∂W∂ydydt.(16)\frac{dW}{dt} = \frac{\partial W}{\partial x}\frac{dx}{dt} + \frac{\partial W}{\partial y}\frac{dy}{dt}. \qquad(16)

The tree diagram is the standard visual aid: WW branches down to xx and yy (labelled by ∂W/∂x\partial W/\partial x and ∂W/∂y\partial W/\partial y), and each of x,yx,y branches further down to tt (labelled dx/dtdx/dt and dy/dtdy/dt); multiplying along each full branch and summing over the branches reproduces (16) exactly.

Verifying the theorem directly. For F(x,y)=x2−2y2+2xyF(x,y)=x^2-2y^2+2xy with x(t)=cos⁡t, y(t)=sin⁡tx(t)=\cos t,\,y(t)=\sin t: substituting first gives F=cos⁡2t−2sin⁡2t+2cos⁡tsin⁡tF=\cos^2t-2\sin^2t+2\cos t\sin t, a function of tt alone, whose derivative (by direct differentiation, using ddt(2cos⁡tsin⁡t)=2(cos⁡2t−sin⁡2t)\dfrac{d}{dt}(2\cos t\sin t)=2(\cos^2t-\sin^2t)) works out to −6cos⁡tsin⁡t+2(cos⁡2t−sin⁡2t)-6\cos t\sin t+2(\cos^2t-\sin^2t). Computing instead via (16): Fx=2x+2y, Fy=−4y+2xF_x=2x+2y,\,F_y=-4y+2x, dx/dt=−sin⁡t, dy/dt=cos⁡tdx/dt=-\sin t,\,dy/dt=\cos t, so

∂F∂xdxdt+∂F∂ydydt=(2x+2y)(−sin⁡t)+(2x−4y)(cos⁡t)=2(cos⁡t+sin⁡t)(−sin⁡t)+2(cos⁡t−2sin⁡t)(cos⁡t),\frac{\partial F}{\partial x}\frac{dx}{dt}+\frac{\partial F}{\partial y}\frac{dy}{dt} = (2x+2y)(-\sin t)+(2x-4y)(\cos t) = 2(\cos t+\sin t)(-\sin t)+2(\cos t-2\sin t)(\cos t),

which simplifies to the same −6cos⁡tsin⁡t+2(cos⁡2t−sin⁡2t)-6\cos t\sin t+2(\cos^2t-\sin^2t) — confirming (16). Both routes always agree, so computing both is a genuine self-check; whichever route is algebraically shorter for a given problem is the one to use in practice.

Two-parameter version. Sometimes x=x(s,t)x=x(s,t) and y=y(s,t)y=y(s,t) both depend on two parameters s,t∈Rs,t\in\mathbb R, making WW ultimately a function of s,ts,t as well:

Theorem 8.3 (Chain Rule, two parameters). If W(x,y)W(x,y) has partial derivatives, and x=x(s,t), y=y(s,t)x=x(s,t),\,y=y(s,t) both have partial derivatives with respect to ss and tt, then

∂W∂s=∂W∂x∂x∂s+∂W∂y∂y∂s,∂W∂t=∂W∂x∂x∂t+∂W∂y∂y∂t.(17, 18)\frac{\partial W}{\partial s} = \frac{\partial W}{\partial x}\frac{\partial x}{\partial s} + \frac{\partial W}{\partial y}\frac{\partial y}{\partial s}, \qquad \frac{\partial W}{\partial t} = \frac{\partial W}{\partial x}\frac{\partial x}{\partial t} + \frac{\partial W}{\partial y}\frac{\partial y}{\partial t}. \qquad(17,\,18) …