Sign in to save

Bookmark this page so you can find it later.

Sign in to save

Bookmark this page so you can find it later.

This cheat sheet covers the AP Calculus BC tools for curves that are not written as simple functions of xx. Parametric equations describe position using a parameter, polar equations describe distance from the origin using angle, and vector functions describe motion in space. Students need these formulas to find slopes, areas, arc lengths, velocities, accelerations, and curve behavior on non-Cartesian paths.

The most important idea is to connect each representation back to calculus with derivatives and integrals. For parametric curves, use dydx=dy/dtdx/dt\frac{dy}{dx}=\frac{dy/dt}{dx/dt} and integrate with respect to tt. For polar curves, use x=rcosθx=r\cos\theta, y=rsinθy=r\sin\theta, and area A=12αβr2dθA=\frac{1}{2}\int_{\alpha}^{\beta}r^2\,d\theta.

For vector functions, velocity is r(t)\mathbf{r}'(t), acceleration is r(t)\mathbf{r}''(t), and speed is r(t)|\mathbf{r}'(t)|.

Key Facts

  • For a parametric curve x=x(t)x=x(t) and y=y(t)y=y(t), the slope is dydx=dydtdxdt\frac{dy}{dx}=\frac{\frac{dy}{dt}}{\frac{dx}{dt}} when dxdt0\frac{dx}{dt}\neq 0.
  • The second derivative of a parametric curve is d2ydx2=ddt(dydx)dxdt\frac{d^2y}{dx^2}=\frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{\frac{dx}{dt}} when dxdt0\frac{dx}{dt}\neq 0.
  • The arc length of a parametric curve from t=at=a to t=bt=b is L=ab(dxdt)2+(dydt)2dtL=\int_a^b\sqrt{\left(\frac{dx}{dt}\right)^2+\left(\frac{dy}{dt}\right)^2}\,dt.
  • Polar coordinates convert to rectangular coordinates using x=rcosθx=r\cos\theta and y=rsinθy=r\sin\theta.
  • The area enclosed by a polar curve from θ=α\theta=\alpha to θ=β\theta=\beta is A=12αβr2dθA=\frac{1}{2}\int_{\alpha}^{\beta}r^2\,d\theta.
  • The slope of a polar curve is dydx=drdθsinθ+rcosθdrdθcosθrsinθ\frac{dy}{dx}=\frac{\frac{dr}{d\theta}\sin\theta+r\cos\theta}{\frac{dr}{d\theta}\cos\theta-r\sin\theta} when the denominator is not 00.
  • For a vector function r(t)=x(t),y(t),z(t)\mathbf{r}(t)=\langle x(t),y(t),z(t)\rangle, velocity is v(t)=r(t)\mathbf{v}(t)=\mathbf{r}'(t) and acceleration is a(t)=r(t)\mathbf{a}(t)=\mathbf{r}''(t).
  • Speed is the magnitude of velocity, so speed=v(t)=(x(t))2+(y(t))2+(z(t))2\text{speed}=|\mathbf{v}(t)|=\sqrt{(x'(t))^2+(y'(t))^2+(z'(t))^2}.

Vocabulary

Parametric equation
A pair or set of equations, such as x=x(t)x=x(t) and y=y(t)y=y(t), that describe a curve using a parameter tt.
Parameter
A variable, often tt or θ\theta, that controls the position of a point on a curve.
Polar curve
A curve described by r=f(θ)r=f(\theta), where rr is distance from the origin and θ\theta is the angle from the positive xx-axis.
Vector function
A function such as r(t)=x(t),y(t)\mathbf{r}(t)=\langle x(t),y(t)\rangle or r(t)=x(t),y(t),z(t)\mathbf{r}(t)=\langle x(t),y(t),z(t)\rangle that gives position using component functions.
Velocity vector
The derivative of position, v(t)=r(t)\mathbf{v}(t)=\mathbf{r}'(t), which gives both speed and direction of motion.
Arc length
The total distance along a curve, found by integrating speed over the relevant parameter interval.

Common Mistakes to Avoid

  • Using dydt\frac{dy}{dt} as the slope of a parametric curve is wrong because slope means change in yy with respect to xx, so use dydx=dy/dtdx/dt\frac{dy}{dx}=\frac{dy/dt}{dx/dt}.
  • Forgetting the factor 12\frac{1}{2} in polar area is wrong because the sector-area formula is built into A=12αβr2dθA=\frac{1}{2}\int_{\alpha}^{\beta}r^2\,d\theta.
  • Using abydx\int_a^b y\,dx directly on a parametric curve without substituting is wrong because dx=x(t)dtdx=x'(t)\,dt, so area uses aby(t)x(t)dt\int_a^b y(t)x'(t)\,dt when appropriate.
  • Treating velocity and speed as the same thing is wrong because velocity is a vector v(t)\mathbf{v}(t), while speed is the scalar magnitude v(t)|\mathbf{v}(t)|.
  • Ignoring where dxdt=0\frac{dx}{dt}=0 or the polar slope denominator equals 00 is wrong because these points may create vertical tangents, cusps, or undefined slopes.

Practice Questions

  1. 1 For x=t2+1x=t^2+1 and y=t33ty=t^3-3t, find dydx\frac{dy}{dx} at t=2t=2.
  2. 2 Find the area enclosed by the polar curve r=2sinθr=2\sin\theta for 0θπ0\leq \theta\leq \pi.
  3. 3 For r(t)=t2,sint,et\mathbf{r}(t)=\langle t^2,\sin t, e^t\rangle, find v(t)\mathbf{v}(t), a(t)\mathbf{a}(t), and the speed at t=0t=0.
  4. 4 Explain why a parametric curve can pass the vertical line test multiple times but still have a well-defined tangent direction at each regular point.

Understanding Parametric, Polar, and Vector Functions

A parameter does more than label points on a curve. It records the order in which the curve is traced. The same location can occur at two different parameter values, yet the object may pass through in different directions.

This matters when a graph crosses itself or retraces part of its path. A parameter interval can describe only one portion of a larger curve, so always identify where tracing starts and ends. Tangent behavior needs extra care.

A vertical tangent can occur when the horizontal coordinate has zero rate of change while the vertical coordinate does not. If both coordinate rates are zero, the usual slope method fails. Students should inspect values just before and after that time to determine whether there is a cusp, a corner, or another special point.

Polar graphs can be confusing because one point has more than one polar description. A negative radius places the point in the direction opposite the given angle. This feature creates petals, loops, and repeated sections in many polar curves.

A quick table of angles and radii often reveals the shape before any detailed calculation. It is especially important for area problems. The correct angle bounds must trace a region exactly once.

If a loop is traced twice, an integral can produce double the intended area. When two polar curves form a shared region, find where their radii are equal and check which curve lies farther from the origin over each interval.

A sketch is not optional here. It protects against using the wrong boundaries.

Vector functions give a mathematical model of movement through three dimensional space. The velocity vector includes direction, while speed is only a nonnegative size. An object can have a large velocity change even when its speed stays constant, such as a car moving around a circular track.

Its direction changes continuously, so it has acceleration toward the center of the turn. Acceleration does not always mean an object is speeding up. When acceleration points generally along the motion, speed increases.

When it points against the motion, speed decreases. Curvature measures how sharply a path turns.

A straight path has no turning, while a tight bend has greater curvature. This helps describe roads, roller coasters, robot paths, and the flight of a thrown object.

Good work with these topics combines algebra, graphs, and calculus. Keep track of the independent variable, since a derivative with respect to time has a different meaning from a derivative with respect to angle. Check units whenever a problem describes motion.

Position might use meters, velocity meters per second, and acceleration meters per second squared. Use a calculator graph as evidence, not as a replacement for reasoning. Graph windows can hide small loops, intersections, or repeated tracing.

Before integrating for length or area, write the interval in words and state what part of the curve it represents. Before reporting a tangent or a maximum speed, verify that the required derivative exists at that point. These checks prevent many common errors.