Derivatives of parametric functions

A ball thrown into the air does not sit still waiting to be described as yy in terms of xx — at every instant tt it has a horizontal position x(t)x(t) and a height y(t)y(t), and both are changing together. A huge class of curves — projectile paths, planetary orbits, circles, parabolas traced by a moving point — are most naturally written this way, as a pair x=f(t)x = f(t), y=g(t)y = g(t) tied to a common parameter tt, rather than as one explicit equation y=y(x)y = y(x). This article asks the natural follow-up question: if you cannot easily write yy as a function of xx, how do you still find the slope dydx\dfrac{dy}{dx} of the path? The answer turns out to need nothing beyond the chain rule, applied in a slightly unfamiliar direction, and it becomes the standard tool for differentiating any curve given parametrically.

The core insight

When a curve is given as x=f(t)x=f(t) and y=g(t)y=g(t), the slope is found without ever eliminating tt, simply as dydx=dy/dtdx/dt\dfrac{dy}{dx}=\dfrac{dy/dt}{dx/dt}.

The core idea

Two functions, one parameter. A parametric curve hands you xx and yy separately, each as a function of a third variable tt. Neither equation alone describes the curve; together, as tt sweeps through its range, the point (x(t),y(t))(x(t), y(t)) traces the path.

Why not just eliminate tt? For simple curves — say x=at2x = at^2, y=2aty = 2at — you could solve the first equation for tt and substitute into the second to recover an explicit y(x)y(x). But for curves built from trigonometric expressions in tt, this elimination is often messy or impossible in closed form. Differentiating directly through tt sidesteps that difficulty entirely.

The governing formula. Provided ff and gg are differentiable and dxdt≠0\dfrac{dx}{dt} \neq 0, yy can be regarded as a function of xx implicitly, through tt, and

dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}

where: dy/dtdy/dt is the rate of change of yy with respect to the parameter, dx/dtdx/dt is the rate of change of xx with respect to the same parameter, and the ratio of the two gives the actual slope of the curve at that point — generally still expressed in terms of tt, which is the expected form of the answer.

Reading the geometry. As the parameter tt increases by a small amount, the point (x,y)(x,y) shifts by (dx,dy)(dx, dy); the slope of the little displacement is exactly dy/dxdy/dx, and writing both displacements through their common rate of change with tt is what makes the ratio formula work.

Where this leads next. Once dydx\dfrac{dy}{dx} is expressed in terms of tt, it is itself a function of tt, and the syllabus's very next topic asks for the second derivative d2ydx2\dfrac{d^2y}{dx^2} of a parametric curve. That calculation reuses exactly the same idea one level up: differentiate dydx\dfrac{dy}{dx} with respect to tt, then divide by dxdt\dfrac{dx}{dt} again, rather than differentiating the messy ratio directly with respect to xx. Seeing parametric differentiation as "one clean ratio, repeatable" is what makes that later topic straightforward instead of intimidating.

Figure
A curve traced by a moving point with position given by x of t and y of t, and a tangent line at one point showing the slope as the ratio of dy dt to dx dt
A parametric curve traced by a moving point, with its tangent slope point at parameter t tangent, slope dy/dx t small t large x = f(t), y = g(t) — the same t drives both coordinates
Derivation ADeriving dy/dx for a parametrically defined curve

The goal is to show, using only the chain rule and the fact that inverse rates of change are reciprocals, that the slope of a curve given by x=f(t)x = f(t) and y=g(t)y = g(t) can be found as dydx=dy/dtdx/dt\dfrac{dy}{dx} = \dfrac{dy/dt}{dx/dt} without ever solving for yy explicitly in terms of xx — the single formula used throughout this topic.

Step 1. Treat yy as depending on xx through the intermediate variable tt. Since x=f(t)x = f(t) is itself differentiable and (where dx/dt≠0dx/dt \neq 0) invertible, tt can in principle be written as a function of xx, so yy is a composite function of xx via tt: y=g(t(x))y = g(t(x)).

Step 2. Apply the chain rule to this composite function. Differentiating yy with respect to xx gives dydx=dydt⋅dtdx\dfrac{dy}{dx} = \dfrac{dy}{dt}\cdot\dfrac{dt}{dx} — exactly the same chain-rule pattern used for any function of a function, just with tt playing the role of the intermediate variable.

Step 3. Replace dtdx\dfrac{dt}{dx} using the inverse-function relationship between tt and xx. Because x=f(t)x = f(t), the derivative of tt with respect to xx is the reciprocal of the derivative of xx with respect to tt: dtdx=1dx/dt\dfrac{dt}{dx} = \dfrac{1}{dx/dt}, valid wherever dx/dt≠0dx/dt \neq 0.

Step 4. Substitute this reciprocal back into Step 2. dydx=dydt⋅1dx/dt=dy/dtdx/dt\dfrac{dy}{dx} = \dfrac{dy}{dt}\cdot\dfrac{1}{dx/dt} = \dfrac{dy/dt}{dx/dt}, which is the required formula. It shows the "cross-cancelling" of dtdt is not a notational trick but the honest result of the chain rule combined with the inverse-derivative rule.

Worked example

If x=at2x = at^2 and y=2aty = 2at — the standard parametrisation of a parabola — find dydx\dfrac{dy}{dx}, then use it to write the equation of the tangent at t=2t = 2, taking a=1a = 1.

Step 1. Differentiate xx with respect to tt: dxdt=2at\dfrac{dx}{dt} = 2at.

Step 2. Differentiate yy with respect to tt: dydt=2a\dfrac{dy}{dt} = 2a.

Step 3. Divide to get the slope: dydx=dy/dtdx/dt=2a2at=1t\dfrac{dy}{dx} = \dfrac{dy/dt}{dx/dt} = \dfrac{2a}{2at} = \dfrac{1}{t} (for t≠0t \neq 0). This is the standard slope of the parabola y2=4axy^2 = 4ax at the point (at2,2at)(at^2, 2at).

Step 4. Evaluate at t=2t = 2, a=1a = 1: the point is (x,y)=(1⋅4,2⋅1⋅2)=(4,4)(x,y) = (1\cdot4, 2\cdot1\cdot2) = (4,4), and the slope is 1t=12\dfrac{1}{t} = \dfrac{1}{2}. The tangent line through (4,4)(4,4) with slope 12\tfrac12 is y−4=12(x−4)y - 4 = \tfrac12(x-4), which simplifies to y=12x+2y = \tfrac12 x + 2.

The tangent to the parabola x=t2x=t^2, y=2ty=2t at t=2t=2 is y=12x+2y = \dfrac{1}{2}x + 2.

Competitive stretch

For the trigonometric pair x=cos⁡θ−cos⁡2θx = \cos\theta - \cos2\theta, y=sin⁡θ−sin⁡2θy = \sin\theta - \sin2\theta, the same three steps give dxdθ=−sin⁡θ+2sin⁡2θ\dfrac{dx}{d\theta} = -\sin\theta + 2\sin2\theta and dydθ=cos⁡θ−2cos⁡2θ\dfrac{dy}{d\theta} = \cos\theta - 2\cos2\theta, so dydx=cos⁡θ−2cos⁡2θ2sin⁡2θ−sin⁡θ\dfrac{dy}{dx} = \dfrac{\cos\theta - 2\cos2\theta}{2\sin2\theta - \sin\theta} — left in terms of θ\theta, since there is no simpler closed form in xx alone. Notice that no elimination of θ\theta was attempted here: unlike the parabola, this curve mixes two different multiples of the same angle, and solving either equation for θ\theta alone is not realistic. This is exactly the situation the formula is built for — it delivers a usable slope regardless of whether the parameter could ever be eliminated.

Common traps

  • Trying to eliminate the parameter first. Solving for tt and substituting is usually unnecessary and sometimes impossible in closed form; go straight through dy/dtdx/dt\dfrac{dy/dt}{dx/dt}.
  • Inverting the ratio. Writing dydx=dx/dtdy/dt\dfrac{dy}{dx} = \dfrac{dx/dt}{dy/dt} instead of dy/dtdx/dt\dfrac{dy/dt}{dx/dt} — always differentiate yy on top, xx on the bottom, both with respect to the same parameter.
  • Forgetting the condition dx/dt≠0dx/dt \neq 0. Wherever dx/dt=0dx/dt = 0, the formula breaks down (a vertical tangent, undefined slope).
  • Mixing parameters. Differentiating xx with respect to tt but yy with respect to a different variable in a problem that uses two parameter names.
  • Dividing before simplifying trig terms. For curves built from sums or differences of sines and cosines at different multiples of the parameter, applying a sum-to-product identity to dx/dtdx/dt and dy/dtdy/dt first — before forming the ratio — usually gives a far cleaner final slope than dividing the raw derivatives directly.

Ask the tutor: If you want to see how a sum-to-product identity can turn a messy trigonometric parametric derivative into a clean one, walk through it with the AI tutor step by step.

Why does dy/dx equal dy/dt divided by dx/dt and not the other way around?

It comes straight from the chain rule: dydx=dydt⋅dtdx\dfrac{dy}{dx} = \dfrac{dy}{dt}\cdot\dfrac{dt}{dx}, and since dtdx\dfrac{dt}{dx} is the reciprocal of dxdt\dfrac{dx}{dt}, this becomes dydt⋅1dx/dt=dy/dtdx/dt\dfrac{dy}{dt}\cdot\dfrac{1}{dx/dt} = \dfrac{dy/dt}{dx/dt}. The yy-rate always sits on top because yy is the quantity you are ultimately differentiating; the xx-rate sits on the bottom because xx plays the role of the independent variable, reached only via the reciprocal relationship with tt.

Do I always need to eliminate the parameter before differentiating?

No — and for most syllabus problems you should not even try. Elimination is only worth attempting when it is quick and gives a clean explicit equation, which happens for a handful of standard curves like the parabola. For anything involving trigonometric functions of the parameter, elimination is typically messy or impossible, while dy/dtdx/dt\dfrac{dy/dt}{dx/dt} works directly every time, leaving the answer in terms of the parameter — which is a perfectly acceptable final form.

What does it mean if my final answer for dy/dx still has t or theta in it?

That is expected, not a sign of an unfinished answer. The slope of a parametric curve genuinely depends on where along the curve you are, and that position is specified by the parameter, so the slope naturally comes out as a function of tt (or θ\theta). You only need to convert back to xx or yy if the question explicitly asks for the slope at a numerical point, in which case you first find the parameter value corresponding to that point and substitute it in.

Before this

Where this leads