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Mathematics · Ch 10 — Differential Calculus – Differentiability and Methods of Differentiation

Derivatives of variables defined by parametric equations

10.4.6

Derivatives of variables defined by parametric equations

So far yy has been expressed either explicitly in terms of xx, or implicitly via an equation directly relating xx and yy. A third common situation is parametric equations: both xx and yy are given separately as functions of a third, auxiliary variable tt,

x=f(t),y=g(t),x = f(t), \qquad y = g(t),

called the parameter. As tt ranges over some domain [a,b][a,b], the pair (x,y)=(f(t),g(t))(x,y)=(f(t),g(t)) traces out a curve in the plane; this specification of the relationship between xx and yy via tt is described as parametric. Recovering a single direct equation connecting xx and yy alone — by eliminating tt — is called elimination of the parameter; the point of using a parameter in the first place is often that a genuinely two-variable relationship becomes much easier to describe and differentiate through one auxiliary variable tt.

Worked illustration — the circle. The circle x2+y2=r2x^2+y^2=r^2 (centre the origin, radius rr) has the parametric form x=rcos⁡t, y=rsin⁡tx=r\cos t,\ y=r\sin t; eliminating tt via cos⁡2t+sin⁡2t=1\cos^2t+\sin^2t=1 recovers x2+y2=r2x^2+y^2=r^2 exactly.

Differentiating a parametric pair. If yy is regarded as (ultimately) a function of xx through the parameter tt, the chain rule gives

dydx=dy/dtdx/dt=g′(t)f′(t)(f′(t)≠0),\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{g'(t)}{f'(t)}\qquad(f'(t)\ne0),

and symmetrically, if instead xx is regarded as a function of yy,

dxdy=dx/dtdy/dt=f′(t)g′(t)(g′(t)≠0)\frac{dx}{dy} = \frac{dx/dt}{dy/dt} = \frac{f'(t)}{g'(t)}\qquad(g'(t)\ne0)

— the two are reciprocals of each other, exactly as ordinary dy/dxdy/dx and dx/dydx/dy are.

For the circle x=rcos⁡t, y=rsin⁡tx=r\cos t,\ y=r\sin t: dxdt=−rsin⁡t\dfrac{dx}{dt}=-r\sin t and dydt=rcos⁡t\dfrac{dy}{dt}=r\cos t, so the slope of the tangent to the circle at parameter value tt is

dydx=rcos⁡t−rsin⁡t=−cot⁡t.\frac{dy}{dx} = \frac{r\cos t}{-r\sin t} = -\cot t.

Worked illustration — a non-trivial pair. For x=at2, y=2atx=at^2,\ y=2at (t≠0t\ne0): dxdt=2at\dfrac{dx}{dt}=2at and dydt=2a\dfrac{dy}{dt}=2a, so dydx=2a2at=1t\dfrac{dy}{dx}=\dfrac{2a}{2at}=\dfrac1t — no elimination of tt was needed at all to get the slope in terms of the parameter. …