In AP Calculus BC, the acceleration vector a(t) is the derivative of the velocity vector (the second derivative of position), found by differentiating each component of a vector-valued function r(t) = <x(t), y(t)> separately, so a(t) = <x''(t), y''(t)>.
The acceleration vector tells you how a particle's velocity is changing at any instant, in both magnitude and direction. If a particle moves in the plane with position r(t) = <x(t), y(t)>, you find velocity by differentiating each component once, and acceleration by differentiating each component again. So a(t) = v'(t) = r''(t) = <x''(t), y''(t)>.
Here's the mental shortcut. Everything you know about derivatives in 1D motion still works, you just do it twice, once per component. The CED says it directly in 9.4.A: methods for differentiating real-valued functions extend to vector-valued functions. There's no new differentiation rule to learn. The x-component of acceleration is the second derivative of the x-position, and the y-component is the second derivative of the y-position. That's the whole computation. The conceptual upgrade is that acceleration now has a direction, so a particle can be accelerating even while its speed stays constant (think of a car turning a corner at a steady 30 mph).
This term lives in Unit 9 (Parametric Equations, Polar Coordinates, and Vector-Valued Functions), which is BC-only. It directly supports two learning objectives. Under 9.4.A, you calculate derivatives of vector-valued functions, and a(t) is the second-derivative case. Under 9.6.A, you use those derivatives to solve planar motion problems, since essential knowledge FUN-8.B.1 states that derivatives determine velocity, speed, and acceleration for a particle moving along a curve in the plane. Planar motion is one of the most reliable BC FRQ setups, and the acceleration vector is one of the standard parts of that question. If you can't move cleanly between position, velocity, and acceleration in component form, you're leaving easy FRQ points on the table.
Keep studying AP Calculus Unit 9
Visual cheatsheet
view galleryVelocity Vector (Unit 9)
Velocity is the bridge between position and acceleration. You can't get a(t) without going through v(t), since a(t) = v'(t). Going the other way, integrating the acceleration vector component-by-component recovers velocity (plus initial conditions), which is exactly the kind of round trip FRQs love.
Straight-Line Motion in Units 4-6 (Units 4-6)
The position-velocity-acceleration chain from AB motion problems (s, v = s', a = v'') is the same chain here. Unit 9 just runs it in two components at once. If you mastered rectilinear motion, the acceleration vector is that idea copied into the x and y directions.
Distance Traveled (Unit 9)
Distance traveled is the integral of speed, where speed is the magnitude of the velocity vector, per FUN-8.B.2. This is where direction matters most. Speed is a single number, but acceleration is a vector, and a particle can have a nonzero acceleration vector while its speed isn't changing at all.
Displacement Vector (Unit 9)
Displacement is the definite integral of the velocity vector over a time interval. Acceleration and displacement sit on opposite ends of the same ladder. Differentiate twice from position to get acceleration, integrate twice from acceleration (with initial conditions) to get back to position.
The most common question is computational and fast. You're given r(t) and asked for a(t), which means differentiating each component twice. Practice versions look like this: given r(t) = <2t² + 3t, 4t² - 2t>, find a(t). (Answer: v(t) = <4t + 3, 8t - 2>, so a(t) = <4, 8>.) These show up as multiple-choice items and as part (a)-style FRQ openers. On free-response, the 2023 BC FRQ Q2 used exactly this planar motion setup, giving information about x'(t) and y(t) and asking you to work through the position-velocity-acceleration chain at specific times. Expect to also evaluate a(t) at a given t, find its magnitude, or use it alongside speed and total distance in a multi-part motion problem. Calculator-active versions may give you derivatives numerically, so know which derivative you're being handed.
Both are derivatives of a vector-valued position function, which is why they blur together under time pressure. The velocity vector v(t) = r'(t) is the first derivative and points in the direction of motion (tangent to the curve). The acceleration vector a(t) = r''(t) is the second derivative and points in the direction velocity is changing, which is often not the direction the particle is moving. Quick check: speed comes from the magnitude of velocity, never from acceleration.
The acceleration vector is the second derivative of the position vector and the first derivative of the velocity vector, so a(t) = v'(t) = r''(t).
To compute a(t) for r(t) = <x(t), y(t)>, differentiate each component twice and write a(t) = <x''(t), y''(t)>.
Acceleration has both magnitude and direction, so a particle moving at constant speed along a curve still has a nonzero acceleration vector.
This concept supports learning objectives 9.4.A and 9.6.A in BC-only Unit 9, and it's a standard piece of planar motion FRQs.
Integrating the acceleration vector component-by-component (with initial conditions) recovers the velocity vector, so you can move up and down the position-velocity-acceleration chain in both directions.
It's the derivative of the velocity vector, or equivalently the second derivative of the position vector. For r(t) = <x(t), y(t)>, the acceleration vector is a(t) = <x''(t), y''(t)>.
Differentiate each component of r(t) twice. For example, if r(t) = <2t² + 3t, 4t² - 2t>, then v(t) = <4t + 3, 8t - 2> and a(t) = <4, 8>.
No. A particle turning along a curve at constant speed has a nonzero acceleration vector because the direction of its velocity is changing. Acceleration is zero only when the velocity vector itself is constant in both magnitude and direction.
Velocity is r'(t) and points tangent to the path in the direction of motion; acceleration is r''(t) and points in the direction velocity is changing. Speed is the magnitude of velocity, not the magnitude of acceleration.
It's BC-only. Vector-valued functions live in Unit 9 (Topics 9.4 and 9.6), which isn't tested on the AB exam. AB tests acceleration only for straight-line motion, where it's a single function, not a vector.