3 Parametric Equations

A progressive guide to representing curves parametrically and using derivatives, integrals, and motion concepts to analyze their geometry and applications.

Representing and tracing curves

A parametrically defined point has coordinates determined by a parameter tt:

x=x(t),y=y(t),a≤t≤b.x=x(t),\qquad y=y(t),\qquad a\le t\le b.

As tt changes, the point (x(t),y(t))(x(t),y(t)) traces a path. The parameter may represent time, but it can also be an auxiliary variable chosen because it describes the curve conveniently. This approach is especially useful for paths that cannot be represented conveniently as one function y=f(x)y=f(x).

A contains more information than its rectangular equation alone. The parameter can record the starting point, direction, and of traversal. For example, consider

x=t+1,y=t2.x=t+1,\qquad y=t^2.

Solving the first equation for the parameter gives t=x−1t=x-1, so the rectangular equation is

y=(x−1)2.y=(x-1)^2.

As tt increases, x=t+1x=t+1 increases, so this parametrization traces the parabola from left to right. Another parametrization could trace the same parabola in the opposite direction or at a different .

Useful standard forms include a line through (x0,y0)(x_0,y_0) with direction vector ⟨a,b⟩\langle a,b\rangle:

x=x0+at,y=y0+bt.x=x_0+at,\qquad y=y_0+bt.

A circle centered at (h,k)(h,k) with radius rr can be written as

x=h+rcos⁡t,y=k+rsin⁡t,0≤t≤2π.x=h+r\cos t,\qquad y=k+r\sin t, \qquad 0\le t\le 2\pi.

For the unit circle, x=cos⁡tx=\cos t and y=sin⁡ty=\sin t; increasing tt from 00 to 2π2\pi traces the circle counterclockwise.

Takeaway: Always identify both the geometric path and how the parameter moves along it.

Slopes and tangent lines

The slope of a parametrically defined curve is found by differentiating both coordinate functions. The chain rule gives

dydt=dydxdxdt.\frac{dy}{dt}=\frac{dy}{dx}\frac{dx}{dt}.

Therefore, when x′(t)≠0x'(t)\ne 0,

dydx=dy/dtdx/dt=y′(t)x′(t).\frac{dy}{dx}=\frac{dy/dt}{dx/dt}=\frac{y'(t)}{x'(t)}.

To find a at t=t0t=t_0, first find the point (x(t0),y(t0))(x(t_0),y(t_0)), then evaluate the slope, and finally use point-slope form:

y−y(t0)=dydx∣t=t0(x−x(t0)).y-y(t_0)=\left.\frac{dy}{dx}\right|_{t=t_0}\bigl(x-x(t_0)\bigr).

For the circle

x=3cos⁡t,y=3sin⁡t,x=3\cos t,\qquad y=3\sin t,

we have

x′(t)=−3sin⁡t,y′(t)=3cos⁡t,x'(t)=-3\sin t,\qquad y'(t)=3\cos t,

so

dydx=−cot⁡t.\frac{dy}{dx}=-\cot t.

At t=π4t=\frac{\pi}{4}, the point is (322,322)\left(\frac{3\sqrt{2}}{2},\frac{3\sqrt{2}}{2}\right), and the slope is −1-1. Thus the is

y−322=−(x−322),y-\frac{3\sqrt{2}}{2}=-\left(x-\frac{3\sqrt{2}}{2}\right),

which simplifies to

x+y=32.x+y=3\sqrt{2}.

Special tangent behavior follows directly from the coordinate derivatives:

  • A horizontal tangent occurs when y′(t)=0y'(t)=0 and x′(t)≠0x'(t)\ne 0.

  • A vertical tangent occurs when x′(t)=0x'(t)=0 and y′(t)≠0y'(t)\ne 0.

  • If both derivatives are zero, the usual slope formula is inconclusive. The point may be a cusp, a corner, or another singular point and requires additional analysis.

Takeaway: Find the point and both coordinate derivatives before deciding whether the tangent is ordinary, horizontal, vertical, or singular.

Second derivatives and concavity

To study concavity, differentiate the first-derivative formula with respect to the parameter and then divide by dx/dtdx/dt:

d2ydx2=ddx(dydx)=ddt(dydx)dx/dt.\frac{d^2y}{dx^2} =\frac{d}{dx}\left(\frac{dy}{dx}\right) =\frac{\dfrac{d}{dt}\left(\dfrac{dy}{dx}\right)}{dx/dt}.

An equivalent formula is

d2ydx2=x′(t)y′′(t)−y′(t)x′′(t)[x′(t)]3,\frac{d^2y}{dx^2} =\frac{x'(t)y''(t)-y'(t)x''(t)}{[x'(t)]^3},

provided x′(t)≠0x'(t)\ne 0. A positive value indicates concavity up, while a negative value indicates concavity down.

For

x=t2,y=t3,x=t^2,\qquad y=t^3,

we obtain, for t≠0t\ne 0,

dydx=3t22t=3t2.\frac{dy}{dx}=\frac{3t^2}{2t}=\frac{3t}{2}.

Differentiating with respect to tt gives

ddt(dydx)=32,\frac{d}{dt}\left(\frac{dy}{dx}\right)=\frac{3}{2},

and therefore

d2ydx2=3/22t=34t.\frac{d^2y}{dx^2}=\frac{3/2}{2t}=\frac{3}{4t}.

Thus the curve is concave down for t<0t<0 and concave up for t>0t>0, wherever the derivative is defined.

Takeaway: Concavity depends on how the tangent slope changes with respect to xx, so the final division by dx/dtdx/dt is essential.

Distance and area

For a smooth curve defined by x=x(t)x=x(t) and y=y(t)y=y(t) on a≤t≤ba\le t\le b, is

L=∫ab(dxdt)2+(dydt)2 dt.L=\int_a^b\sqrt{\left(\frac{dx}{dt}\right)^2+\left(\frac{dy}{dt}\right)^2}\,dt.

The expression under the integral is the rate at which distance accumulates. For a circle of radius rr, use

x=rcos⁡t,y=rsin⁡t,0≤t≤2π.x=r\cos t,\qquad y=r\sin t, \qquad 0\le t\le 2\pi.

Then

dxdt=−rsin⁡t,dydt=rcos⁡t,\frac{dx}{dt}=-r\sin t, \qquad \frac{dy}{dt}=r\cos t,

so

L=∫02πr2sin⁡2t+r2cos⁡2t dt=∫02πr dt=2πr.L=\int_0^{2\pi}\sqrt{r^2\sin^2t+r^2\cos^2t}\,dt =\int_0^{2\pi}r\,dt =2\pi r.

The area under a is based on A=∫y dxA=\int y\,dx. Since dx=x′(t) dtdx=x'(t)\,dt, the corresponding formula is

A=∫aby(t)x′(t) dt.A=\int_a^b y(t)x'(t)\,dt.

This produces . Check whether the curve lies below the horizontal axis or whether x(t)x(t) decreases. If either occurs, the integral may be negative, so split the interval and use absolute values or add geometric areas separately when ordinary area is required.

For

x=t2,y=t,0≤t≤2,x=t^2,\qquad y=t, \qquad 0\le t\le 2,

we have x′(t)=2tx'(t)=2t, and therefore

A=∫02t(2t) dt=2∫02t2 dt=2[t33]02=163.A=\int_0^2t(2t)\,dt =2\int_0^2t^2\,dt =2\left[\frac{t^3}{3}\right]_0^2 =\frac{16}{3}.

Here x(t)x(t) increases and y(t)y(t) is nonnegative, so the signed integral equals the ordinary geometric area.

Takeaway: Differentiate the coordinate functions first, then use the appropriate integral and inspect its sign.

Parametric motion

Parametric equations also describe motion. If the position is

r(t)=⟨x(t),y(t)⟩,\mathbf r(t)=\langle x(t),y(t)\rangle,

then the is

v(t)=r′(t)=⟨x′(t),y′(t)⟩.\mathbf v(t)=\mathbf r'(t)=\langle x'(t),y'(t)\rangle.

Its magnitude is the :

∥v(t)∥=[x′(t)]2+[y′(t)]2.\lVert\mathbf v(t)\rVert =\sqrt{[x'(t)]^2+[y'(t)]^2}.

The is

a(t)=v′(t)=⟨x′′(t),y′′(t)⟩.\mathbf a(t)=\mathbf v'(t)=\langle x''(t),y''(t)\rangle.

Because is the rate at which accumulates, total distance traveled over an interval is

L=∫ab∥v(t)∥ dt.L=\int_a^b\lVert\mathbf v(t)\rVert\,dt.

For the projectile model

x(t)=20t,y(t)=30t−4.9t2,x(t)=20t,\qquad y(t)=30t-4.9t^2,

where position is measured in meters and time in seconds, the velocity is

v(t)=⟨20,30−9.8t⟩,\mathbf v(t)=\langle 20,30-9.8t\rangle,

and the is

∥v(t)∥=202+(30−9.8t)2.\lVert\mathbf v(t)\rVert=\sqrt{20^2+(30-9.8t)^2}.

The acceleration is constant:

a(t)=⟨0,−9.8⟩.\mathbf a(t)=\langle 0,-9.8\rangle.

The tangent slope is

dydx=30−9.8t20.\frac{dy}{dx}=\frac{30-9.8t}{20}.

When 30−9.8t=030-9.8t=0, the vertical component of velocity is zero, so the trajectory has a horizontal tangent and the object reaches its maximum height.

Takeaway: Coordinate derivatives have both geometric and physical meanings: their ratio gives tangent slope, their vector gives velocity, their magnitude gives , and their second derivatives give acceleration.

A unified problem-solving workflow

A reliable workflow keeps the parameter interval, geometry, derivatives, and signs connected:

  1. Identify the parameter interval and determine the direction of travel as tt increases.

  2. For a specified parameter value, calculate the point (x(t),y(t))(x(t),y(t)).

  3. Differentiate both coordinate functions to obtain x′(t)x'(t) and y′(t)y'(t).

  4. Compute the tangent slope with

    dydx=y′(t)x′(t),\frac{dy}{dx}=\frac{y'(t)}{x'(t)},

    provided x′(t)≠0x'(t)\ne 0.

  5. Check separately for horizontal tangents, vertical tangents, and values where both derivatives vanish.

  6. For concavity, use

    d2ydx2=d(dy/dx)/dtdx/dt.\frac{d^2y}{dx^2}=\frac{d(dy/dx)/dt}{dx/dt}.
  7. For distance, integrate the :

    L=∫ab[x′(t)]2+[y′(t)]2 dt.L=\int_a^b\sqrt{[x'(t)]^2+[y'(t)]^2}\,dt.
  8. For area, use

    A=∫aby(t)x′(t) dt,A=\int_a^b y(t)x'(t)\,dt,

    then inspect whether the result is signed or geometric area.

  9. For motion, interpret ⟨x′(t),y′(t)⟩\langle x'(t),y'(t)\rangle as velocity, ⟨x′′(t),y′′(t)⟩\langle x''(t),y''(t)\rangle as acceleration, and the velocity magnitude as .

The central idea is that a parametrization describes both where a curve is and how it is traversed. Derivatives reveal local direction and changing slope, while integrals accumulate distance or .