← Unit 9

Parametric Equations

So far every curve has been \(y=f(x)\) — one output for each input. But a particle looping through the air, or a spiral, doesn't pass that test. The fix: let a third variable, the parameter t, drive x and y separately. Two clocks, one curve.

1. A curve written as a path

Instead of one equation, you get two: \(x(t)\) and \(y(t)\). As t advances, the point \((x(t),\,y(t))\) moves, and the trail it leaves is the curve. Drag the slider to move time forward, or hit play. Switch curves to see why one function of x could never capture these.

t = 0.00
point: (0.00, 0.00) dx/dt = 0.00 dy/dt = 0.00 slope dy/dx = 0.00

The dashed cyan line is the tangent — its slope is exactly \(\tfrac{dy}{dx}\), which we're about to compute. Notice it tilts and even goes vertical as the point moves; that's the first hint that slope in parametric land needs its own formula.

2. Eliminating the parameter: what curve is this?

Before doing any calculus, it helps to recognize the curve. If you can get rid of t and write a plain relationship between x and y, you often discover the parametric pair is just a familiar shape — a line, a parabola, a circle — in disguise.

Method 1 — solve for t, then substitute

When one equation is easy to solve for t, do that and plug into the other. Take \(x=t+1\), \(y=t^2\). Solve the first: \(t=x-1\). Substitute into the second:

So this parametric pair traces the parabola \(y=(x-1)^2\) — same curve you'd graph in Algebra II, now just "clocked" by t.

Method 2 — use a trig identity

When you see cos and sin, reach for \(\cos^2\theta+\sin^2\theta=1\). Take \(x=3\cos t\), \(y=3\sin t\). Then \(\cos t=\tfrac{x}{3}\) and \(\sin t=\tfrac{y}{3}\), so:

That's a circle of radius 3 centered at the origin. (If the coefficients differ — \(x=2\cos t\), \(y=3\sin t\) — the same trick gives \(\left(\tfrac{x}{2}\right)^2+\left(\tfrac{y}{3}\right)^2=1\), an ellipse.)

Eliminating can hide the domain

The rectangular equation may describe more of the curve than the parametric form actually traces. Example: \(x=t^2,\ y=t\) gives \(x=y^2\) — but since \(x=t^2\ge 0\) always, the parametric curve is only the right half (\(x\ge 0\)) of that sideways parabola. Always check what range of \(x\) and \(y\) the parameter really produces.

3. Slope: \(\tfrac{dy}{dx}\) from \(\tfrac{dy}{dt}\) and \(\tfrac{dx}{dt}\)

You want \(\tfrac{dy}{dx}\), but you only have x and y in terms of t. The chain rule bridges them: \(\tfrac{dy}{dt}=\tfrac{dy}{dx}\cdot\tfrac{dx}{dt}\). Solve for what you want:

In words: the rate y changes with t, divided by the rate x changes with t. The t's "cancel" the way fractions suggest. This is the slope of the tangent line to the curve at the point for that t.

Horizontal & vertical tangents

The tangent is horizontal where \(\tfrac{dy}{dt}=0\) (and \(\tfrac{dx}{dt}\neq 0\)) — the curve momentarily stops rising. It's vertical where \(\tfrac{dx}{dt}=0\) (and \(\tfrac{dy}{dt}\neq 0\)) — the slope blows up. AP loves asking for both.

4. Concavity: the second derivative

Here's where most points are lost. To get \(\tfrac{d^2y}{dx^2}\) you do not just take \(\tfrac{d^2y}{dt^2}\). The second derivative is the rate of change of the first derivative with respect to x — so you apply the exact same parametric rule again, this time to \(\tfrac{dy}{dx}\):

Read it as a recipe: take the derivative of \(\tfrac{dy}{dx}\) with respect to t, then divide by \(\tfrac{dx}{dt}\) again. The denominator is \(\tfrac{dx}{dt}\), never dt or dx alone.

The #1 parametric trap

\(\dfrac{d^2y}{dx^2}\) is NOT \(\dfrac{d^2y}{dt^2}\div\dfrac{d^2x}{dt^2}\). You must differentiate the slope \(\tfrac{dy}{dx}\) with respect to \(t\), then divide by \(\tfrac{dx}{dt}\). Forgetting that final "\(\div\,dx/dt\)" is the single most common error on this topic.

5. Arc length: Pythagoras, now both legs move

In Unit 8 you found arc length for \(y=f(x)\) by adding up tiny hypotenuses \(\sqrt{dx^2+dy^2}\), factoring out dx. Parametric arc length is the same idea — but now both x and y change with t, so factor out dt instead:

Each little step along the curve has horizontal part \((dx/dt)\,dt\) and vertical part \((dy/dt)\,dt\); the hypotenuse is \(\sqrt{(dx/dt)^2+(dy/dt)^2}\,dt\), and the integral sums them from \(t=a\) to \(t=b\). Same Pythagorean theorem as Unit 8 — it just has two moving legs now.

Watch the squares

Both derivatives get squared under the root: \((dx/dt)^2\) and \((dy/dt)^2\). And the bounds are values of t, not x — make sure your limits match the parameter.

6. Worked examples

Example 1 · slope & concavity

For \(x=t^2\), \(y=t^3\), find \(\dfrac{dy}{dx}\) and \(\dfrac{d^2y}{dx^2}\) at \(t=2\).

First derivative. So at \(t=2\), \(\dfrac{dy}{dx}=\dfrac{3(2)}{2}=3\). dy/dx = 3

Second derivative. Differentiate \(\dfrac{dy}{dx}=\dfrac{3t}{2}\) with respect to \(t\) (that's \(\tfrac{3}{2}\)), then divide by \(\dfrac{dx}{dt}=2t\): At \(t=2\): \(\dfrac{3}{4\cdot 2}=\dfrac{3}{8}\). d²y/dx² = 3/8

Example 2 · horizontal & vertical tangents

For \(x=t^2+1\), \(y=t^3-3t\), where are the tangents horizontal or vertical?

Horizontal: set \(\dfrac{dy}{dt}=3t^2-3=0\Rightarrow t=\pm 1\). Points: \((2,-2)\) at \(t=1\) and \((2,2)\) at \(t=-1\). horizontal at t = ±1

Vertical: set \(\dfrac{dx}{dt}=2t=0\Rightarrow t=0\). Point: \((1,0)\). (Check \(\dfrac{dy}{dt}=-3\neq 0\) there, so it's genuinely vertical.) vertical at t = 0

Example 3 · arc length

Find the length of \(x=t^2\), \(y=t^3\) from \(t=0\) to \(t=1\).

Set up. \(\dfrac{dx}{dt}=2t\), \(\dfrac{dy}{dt}=3t^2\), so

Simplify & integrate. Factor: \(\sqrt{4t^2+9t^4}=t\sqrt{4+9t^2}\) (since \(t\ge 0\)). Substitute \(u=4+9t^2\), \(du=18t\,dt\):

Result. \(=\tfrac{1}{27}\big(13^{3/2}-8\big)\approx 1.44\). L = (13√13 − 8)/27 ≈ 1.44

7. Quick drill

Five questions on slope, concavity, tangents, and arc length. Pick the right setup or value.

Question 1 of 5 Score: 0
← Back to
Unit 9 Hub