AP-CALCBC-9-FRQ

U9 FRQ Practice

Master AP Calculus BC Unit 9 free-response questions on parametric, vector, and polar functions with step-by-step strategies, formulas, and worked FRQ practice.

What you'll do in this lesson

A voice-first session with the Crimsora tutor on U9 FRQ Practice, then targeted practice and FRQs — with the tutor adapting to where you get stuck.

What this lesson covers

Unit 9 free-response questions are among the most predictable on the AP Calculus BC exam — and the most rewarding once you know the drill. Each year the exam pairs a parametric/vector-motion problem or a polar-area problem with a fixed menu of tasks: find velocity, speed, acceleration, position, slope, arc length, or enclosed area. This lesson is not about re-learning the formulas but about deploying them under time pressure with clean notation and calculator efficiency.

We will walk through how graders read these problems, which formulas earn which points, and the small notational habits that separate a 9 from a 6. By the end you will have a repeatable attack plan for any Unit 9 FRQ.

Recognize the Two FRQ Archetypes

Nearly every Unit 9 FRQ falls into one of two families, and identifying which one you face in the first ten seconds tells you exactly which formulas to have ready.

The parametric/vector motion archetype gives you x(t)x(t) and y(t)y(t) (or a velocity vector) and asks for position, velocity, speed, acceleration, total distance, or times when the particle is at rest or changes direction. The polar area archetype gives you one or more curves r=f(θ)r=f(\theta) and asks for enclosed area, points of intersection, or rates of change with respect to θ\theta or tt.
ArchetypeGivenTypical asks
Parametric/vector motionx(t),y(t)x(t),y(t) or x(t),y(t)\langle x'(t),y'(t)\ranglespeed, acceleration, position via integral, total distance, slope
Polar arear=f(θ)r=f(\theta)area of region, area between curves, drdθ\frac{dr}{d\theta}, tangent slope
A common misconception is that these problems require heavy algebra. They do not. Most points come from setting up the correct definite integral or derivative expression and evaluating it — often with a calculator on the calculator-active section. Reading which section you are in (calculator allowed or not) changes your approach entirely.

The Motion FRQ Toolkit

For a particle with position (x(t),y(t))(x(t),y(t)), memorize these four moves. Velocity is the vector x(t),y(t)\langle x'(t), y'(t)\rangle. Speed is its magnitude, (x(t))2+(y(t))2\sqrt{(x'(t))^2+(y'(t))^2}. Acceleration is x(t),y(t)\langle x''(t), y''(t)\rangle.

To recover position from velocity you integrate and add the initial condition: x(b)=x(a)+abx(t)dtx(b)=x(a)+\int_a^b x'(t)\,dt. This accumulation-function idea is tested every year, so write the initial value explicitly.

Total distance traveled over [a,b][a,b] is the arc length integral ab(x(t))2+(y(t))2dt\int_a^b \sqrt{(x'(t))^2+(y'(t))^2}\,dt. Do not confuse total distance (uses speed, always positive) with displacement (integrates the signed velocity component).

The slope of the path is dydx=dy/dtdx/dt\frac{dy}{dx}=\dfrac{dy/dt}{dx/dt}, valid where dxdt0\frac{dx}{dt}\neq 0. A particle is momentarily at rest when both x(t)=0x'(t)=0 and y(t)=0y'(t)=0 simultaneously.
QuantityFormula
Velocityx(t),y(t)\langle x'(t), y'(t)\rangle
Speed(x(t))2+(y(t))2\sqrt{(x'(t))^2+(y'(t))^2}
Accelerationx(t),y(t)\langle x''(t), y''(t)\rangle
Positionx(a)+atx(u)dux(a)+\int_a^t x'(u)\,du
Total distanceab(x(t))2+(y(t))2dt\int_a^b \sqrt{(x'(t))^2+(y'(t))^2}\,dt
On calculator-active problems, store the integral directly in your calculator and round only the final answer to three decimals.

The Polar Area Toolkit

Polar FRQs live on one formula: the area swept from θ=α\theta=\alpha to θ=β\theta=\beta is A=12αβr2dθA=\frac{1}{2}\int_\alpha^\beta r^2\,d\theta. The most frequent error is forgetting the factor 12\frac{1}{2} or squaring incorrectly, so write 12(f(θ))2dθ\frac{1}{2}\int (f(\theta))^2\,d\theta before plugging in numbers.

When a problem asks for the area between two polar curves, subtract inside the integral: A=12αβ((router)2(rinner)2)dθA=\frac{1}{2}\int_\alpha^\beta \big((r_{\text{outer}})^2-(r_{\text{inner}})^2\big)\,d\theta. You must first find the intersection angles by solving f(θ)=g(θ)f(\theta)=g(\theta), often on the calculator.

Polar problems sometimes attach a time parameter: rr or θ\theta may depend on tt, and the exam asks for drdt\frac{dr}{dt} or the rate at which area accumulates. Use the chain rule carefully and state which variable you are differentiating with respect to.

A subtle grading point: bounds must match the region described. Sketching the curve quickly, even roughly, prevents integrating over the wrong interval. Graders award setup points for a correct integral with correct limits even if arithmetic slips, so always show the full expression before evaluating.

Scoring Habits That Earn Every Point

AP readers grade against a rubric of specific point-earning statements, so presentation matters as much as calculus. First, define your integral or derivative in exact form before you evaluate — the unevaluated expression usually earns its own point. Second, keep at least three decimal places throughout calculator work and round only at the end.

Units and justification are frequent point-carriers. If a question asks whether speed is increasing, you must reference the sign of ddt\frac{d}{dt} of speed or compare acceleration and velocity directions, not just assert. When asked to interpret a value, write a sentence with units, such as 'the particle is 4.213 units to the right of its start.'
HabitWhy it earns points
Write the setup integral firstSetup point is separate from answer point
Include initial condition in positionRequired for accumulation answer
State dx/dt0dx/dt\neq0 for slopeJustifies the quotient
Give three decimalsRounding rule on calculator sections
Answer with a sentence + unitsInterpretation points
Finally, never erase the setup even if your number looks wrong — a correct setup with a computational error still scores partial credit, while a lone wrong number scores nothing.

Key terms

Speed.
The magnitude of the velocity vector, (x(t))2+(y(t))2\sqrt{(x'(t))^2+(y'(t))^2}; always nonnegative and equals the integrand for total distance.
Total distance traveled.
The arc length of the path, ab(x(t))2+(y(t))2dt\int_a^b \sqrt{(x'(t))^2+(y'(t))^2}\,dt, distinct from net displacement.
Velocity vector.
The vector x(t),y(t)\langle x'(t), y'(t)\rangle giving instantaneous direction and rate of motion of a parametrically defined particle.
Acceleration vector.
The component-wise second derivative x(t),y(t)\langle x''(t), y''(t)\rangle of the position functions.
Polar area formula.
A=12αβr2dθA=\frac{1}{2}\int_\alpha^\beta r^2\,d\theta, the area swept by a radius vector over an angular interval.
Parametric slope.
dydx=dy/dtdx/dt\frac{dy}{dx}=\dfrac{dy/dt}{dx/dt}, the slope of the tangent to a parametric curve where dx/dt0dx/dt\neq0.
Displacement.
The signed change in a coordinate, abx(t)dt\int_a^b x'(t)\,dt, which may be less than total distance when direction reverses.
Accumulation function.
Position recovered from a rate via x(t)=x(a)+atx(u)dux(t)=x(a)+\int_a^t x'(u)\,du, combining an initial value with a definite integral.

Worked example

A particle moves in the plane so that at time t0t\ge 0 its velocity is 2t,cost\langle 2t, \cos t\rangle. At t=0t=0 the particle is at the point (1,3)(1,3). (a) Find the speed at t=πt=\pi. (b) Find the position of the particle at t=πt=\pi. (c) Find the total distance traveled from t=0t=0 to t=πt=\pi.
Part (a): Speed is the magnitude of velocity, (x(t))2+(y(t))2=(2t)2+(cost)2\sqrt{(x'(t))^2+(y'(t))^2}=\sqrt{(2t)^2+(\cos t)^2}. At t=πt=\pi, x(π)=2πx'(\pi)=2\pi and y(π)=cosπ=1y'(\pi)=\cos\pi=-1, so speed =(2π)2+(1)2=4π2+16.362=\sqrt{(2\pi)^2+(-1)^2}=\sqrt{4\pi^2+1}\approx 6.362.

Part (b): Recover each coordinate using the accumulation formula with the given initial condition. For xx: x(π)=1+0π2tdt=1+[t2]0π=1+π210.870x(\pi)=1+\int_0^\pi 2t\,dt = 1+[t^2]_0^\pi = 1+\pi^2\approx 10.870. For yy: y(π)=3+0πcostdt=3+[sint]0π=3+(00)=3y(\pi)=3+\int_0^\pi \cos t\,dt = 3+[\sin t]_0^\pi = 3+(0-0)=3. So the position is (1+π2, 3)(10.870, 3)(1+\pi^2,\ 3)\approx(10.870,\ 3). Notice we wrote the initial value plus the integral — that setup earns a rubric point on its own.

Part (c): Total distance is the arc length integral 0π(2t)2+(cost)2dt\int_0^\pi \sqrt{(2t)^2+(\cos t)^2}\,dt. Write this exact integral first, then evaluate on the calculator to get approximately 9.9479.947. Report three decimals and remember this is distance, not displacement.

Practice questions

For a particle with position (x(t),y(t))(x(t),y(t)), which expression gives the total distance traveled on [0,4][0,4]?
  1. 04(x(t)+y(t))dt\int_0^4 (x'(t)+y'(t))\,dt
  2. 04(x(t))2+(y(t))2dt\int_0^4 \sqrt{(x'(t))^2+(y'(t))^2}\,dt
  3. 04(x(t))2dt+04(y(t))2dt\sqrt{\int_0^4 (x'(t))^2\,dt + \int_0^4 (y'(t))^2\,dt}
  4. 1204(x(t))2+(y(t))2dt\frac{1}{2}\int_0^4 (x'(t))^2+(y'(t))^2\,dt

Answer: 04(x(t))2+(y(t))2dt\int_0^4 \sqrt{(x'(t))^2+(y'(t))^2}\,dt

Total distance is the arc length of the path, which integrates speed. Speed is the magnitude (x(t))2+(y(t))2\sqrt{(x'(t))^2+(y'(t))^2}, so the correct integral keeps the square root inside. The first choice mistakenly adds components (giving displacement-like signed motion), and the others misplace the root or add an incorrect factor.
The polar curve r=1+2cosθr=1+2\cos\theta has an inner loop. Set up, but do not evaluate, the integral for the area enclosed by the inner loop. Describe how you would find the limits of integration.

Answer: A=122π/34π/3(1+2cosθ)2dθA=\frac{1}{2}\int_{2\pi/3}^{4\pi/3} (1+2\cos\theta)^2\,d\theta

The inner loop occurs where r=0r=0, since the curve passes through the pole to form the loop. Solving 1+2cosθ=01+2\cos\theta=0 gives cosθ=12\cos\theta=-\frac12, so θ=2π3\theta=\frac{2\pi}{3} and θ=4π3\theta=\frac{4\pi}{3}. Between these angles rr is negative, tracing the inner loop, and applying A=12r2dθA=\frac{1}{2}\int r^2\,d\theta over that interval captures exactly the enclosed region. Squaring handles the sign automatically.
A particle has velocity x(t),y(t)=t2, t24\langle x'(t),y'(t)\rangle = \langle t-2,\ t^2-4\rangle. At what time(s) on [0,5][0,5] is the particle at rest, and justify your answer.

Answer: t=2t=2

The particle is at rest only when both velocity components equal zero simultaneously. Setting x(t)=t2=0x'(t)=t-2=0 gives t=2t=2. Setting y(t)=t24=0y'(t)=t^2-4=0 gives t=2t=2 or t=2t=-2; only t=2t=2 lies in [0,5][0,5]. Since both conditions hold at t=2t=2, that is the sole time the particle is at rest. Checking both components is essential — a zero in only one component means the particle is still moving.

FAQ

How do I know whether a Unit 9 FRQ wants displacement or total distance?
Read the verb. 'How far has the particle moved' or 'total distance traveled' means arc length with the speed integrand (x)2+(y)2\sqrt{(x')^2+(y')^2}. 'What is the net change in position' or 'displacement' means integrating the signed component x(t)dt\int x'(t)\,dt. When in doubt, distance is always the one with the square root and is never negative.
Do I always need the factor of one-half in polar area problems?
Yes. The polar area formula is A=12αβr2dθA=\frac{1}{2}\int_\alpha^\beta r^2\,d\theta, and the 12\frac12 comes from the area of a circular sector. Dropping it is one of the most common point-losing errors. Write the 12\frac12 into your setup immediately, before you substitute the function for rr.
Can I use my calculator to find the answers, and how should I show work?
On the calculator-active section you may evaluate integrals and solve equations numerically. But you must still write the exact setup — the integral or equation — on your paper, because the setup earns a separate rubric point. Then report the numerical answer to three decimal places. Do not show calculator syntax; show mathematical expressions.
What is the fastest way to find where two polar curves intersect?
Set the two expressions equal, f(θ)=g(θ)f(\theta)=g(\theta), and solve for θ\theta within the given interval, using your calculator's solver if the section allows it. Also check whether both curves pass through the pole, since intersections at the origin can occur at different θ\theta values and are easy to miss. A quick sketch confirms which angles bound your region.

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The Crimsora tutor teaches U9 FRQ Practice live — explaining on a whiteboard, asking you questions, and adapting to where you get stuck.