AP Course

AP Calculus AB/BC

Study the complete College Board sequence for AP Calculus AB and BC, from limits through infinite series.

Choose an official unit and topic to open its lecture, concept check, or focused practice.

Lessons
1.1 Introducing Calculus: Can Change Occur at an Instant?1.2 Defining Limits and Using Limit Notation1.3 Estimating Limit Values from Graphs1.4 Estimating Limit Values from Tables1.5 Determining Limits Using Algebraic Properties of Limits1.6 Determining Limits Using Algebraic Manipulation1.7 Selecting Procedures for Determining Limits1.8 Determining Limits Using the Squeeze Theorem1.9 Connecting Multiple Representations of Limits1.10 Exploring Types of Discontinuities1.11 Defining Continuity at a Point1.12 Confirming Continuity over an Interval1.13 Removing Discontinuities1.14 Connecting Infinite Limits and Vertical Asymptotes1.15 Connecting Limits at Infinity and Horizontal Asymptotes1.16 Working with the Intermediate Value Theorem (IVT)2.1 Defining Average and Instantaneous Rates of Change at a Point2.2 Defining the Derivative of a Function and Using Derivative Notation2.3 Estimating Derivatives of a Function at a Point2.4 Connecting Differentiability and Continuity: Determining When Derivatives Do and Do Not Exist2.5 Applying the Power Rule2.6 Derivative Rules: Constant, Sum, Difference, and Constant Multiple2.7 Derivatives of cos x, sin x, e^x, and ln x2.8 The Product Rule2.9 The Quotient Rule2.10 Finding the Derivatives of Tangent, Cotangent, Secant, and/or Cosecant Functions3.1 The Chain Rule3.2 Implicit Differentiation3.3 Differentiating Inverse Functions3.4 Differentiating Inverse Trigonometric Functions3.5 Selecting Procedures for Calculating Derivatives3.6 Calculating Higher-Order Derivatives4.1 Interpreting the Meaning of the Derivative in Context4.2 Straight-Line Motion: Connecting Position, Velocity, and Acceleration4.3 Rates of Change in Applied Contexts Other Than Motion4.4 Introduction to Related Rates4.5 Solving Related Rates Problems4.6 Approximating Values of a Function Using Local Linearity and Linearization4.7 Using L’Hospital’s Rule for Determining Limits of Indeterminate Forms5.1 Using the Mean Value Theorem5.2 Extreme Value Theorem, Global Versus Local Extrema, and Critical Points5.3 Determining Intervals on Which a Function Is Increasing or Decreasing5.4 Using the First Derivative Test to Determine Relative (Local) Extrema5.5 Using the Candidates Test to Determine Absolute (Global) Extrema5.6 Determining Concavity of Functions over Their Domains5.7 Using the Second Derivative Test to Determine Extrema5.8 Sketching Graphs of Functions and Their Derivatives5.9 Connecting a Function, Its First Derivative, and Its Second Derivative5.10 Introduction to Optimization Problems5.11 Solving Optimization Problems5.12 Exploring Behaviors of Implicit Relations6.1 Exploring Accumulations of Change6.2 Approximating Areas with Riemann Sums6.3 Riemann Sums, Summation Notation, and Definite Integral Notation6.4 The Fundamental Theorem of Calculus and Accumulation Functions6.5 Interpreting the Behavior of Accumulation Functions Involving Area6.6 Applying Properties of Definite Integrals6.7 The Fundamental Theorem of Calculus and Definite Integrals6.8 Finding Antiderivatives and Indefinite Integrals: Basic Rules and Notation6.9 Integrating Using Substitution6.10 Integrating Functions Using Long Division and Completing the Square6.11 Integrating Using Integration by Parts6.12 Using Linear Partial Fractions6.13 Evaluating Improper Integrals6.14 Selecting Techniques for Antidifferentiation7.1 Modeling Situations with Differential Equations7.2 Verifying Solutions for Differential Equations7.3 Sketching Slope Fields7.4 Reasoning Using Slope Fields7.5 Approximating Solutions Using Euler’s Method7.6 Finding General Solutions Using Separation of Variables7.7 Finding Particular Solutions Using Initial Conditions and Separation of Variables7.8 Exponential Models with Differential Equations7.9 Logistic Models with Differential Equations8.1 Finding the Average Value of a Function on an Interval8.2 Connecting Position, Velocity, and Acceleration of Functions Using Integrals8.3 Using Accumulation Functions and Definite Integrals in Applied Contexts8.4 Finding the Area Between Curves Expressed as Functions of x8.5 Finding the Area Between Curves Expressed as Functions of y8.6 Finding the Area Between Curves That Intersect at More Than Two Points8.7 Volumes with Cross Sections: Squares and Rectangles8.8 Volumes with Cross Sections: Triangles and Semicircles8.9 Volume with Disc Method: Revolving Around the x- or y-Axis8.10 Volume with Disc Method: Revolving Around Other Axes8.11 Volume with Washer Method: Revolving Around the x- or y-Axis8.12 Volume with Washer Method: Revolving Around Other Axes8.13 The Arc Length of a Smooth, Planar Curve and Distance Traveled9.1 Defining and Differentiating Parametric Equations9.2 Second Derivatives of Parametric Equations9.3 Finding Arc Lengths of Curves Given by Parametric Equations9.4 Defining and Differentiating Vector-Valued Functions9.5 Integrating Vector-Valued Functions9.6 Solving Motion Problems Using Parametric and Vector-Valued Functions9.7 Defining Polar Coordinates and Differentiating in Polar Form9.8 Find the Area of a Polar Region or the Area Bounded by a Single Polar Curve9.9 Finding the Area of the Region Bounded by Two Polar Curves10.1 Defining Convergent and Divergent Infinite Series10.2 Working with Geometric Series10.3 The nth Term Test for Divergence10.4 Integral Test for Convergence10.5 Harmonic Series and p-Series10.6 Comparison Tests for Convergence10.7 Alternating Series Test for Convergence10.8 Ratio Test for Convergence10.9 Determining Absolute or Conditional Convergence10.10 Alternating Series Error Bound10.11 Finding Taylor Polynomial Approximations of Functions10.12 Lagrange Error Bound10.13 Radius and Interval of Convergence of Power Series10.14 Finding Taylor or Maclaurin Series for a Function10.15 Representing Functions as Power Series
Quizzes
Practice Problems AP formula notes, graph references, and practice sets will be added here.

AP Calculus AB/BC · Unit 4 · Topic 4.2

Straight-Line Motion: Connecting Position, Velocity, and Acceleration

Relate position, velocity, speed, and acceleration along a line.

1. Topic Focus

Interpret derivatives as rates in context, connect motion quantities, solve related-rate models, linearize, and evaluate indeterminate limits.

This topic: Relate position, velocity, speed, and acceleration along a line.

2. Key Relationship

\(v(t)=s'(t),\quad a(t)=v'(t)=s''(t)\)

Read every symbol with its domain, direction, units, and hypotheses before applying the relationship.

3. Visual Connection

position s(t)velocity v(t)acceleration a(t)turnv = 0
Successive motion derivativesThe slope of position is velocity, and the slope of velocity is acceleration; signs translate those graphs into direction and speed behavior.

4. Worked Example

A particle changes direction where velocity changes sign, not merely where acceleration is zero.

Write the governing relationship first, carry out the algebra cleanly, and finish with a sentence that answers the mathematical question.

5. Concept Development

1. Position Locates the Particle on an Oriented Line

The position function \(s(t)\) gives a signed coordinate at time \(t\). Before interpreting motion, identify which direction is positive. A negative position means the particle lies on the negative side of the origin; it does not mean the particle is moving in the negative direction.

Position, direction of motion, and distance from the origin are different ideas:

\(\text{position}=s(t),\qquad \text{distance from the origin}=|s(t)|.\)

2. Velocity Is the Rate of Change of Position

\(v(t)=s'(t).\)

Velocity is the slope of the position graph. Its sign determines direction, not location:

  • \(v(t)>0\): motion in the positive direction, such as right or up.
  • \(v(t)<0\): motion in the negative direction, such as left or down.
  • \(v(t)=0\): the particle is instantaneously at rest.

3. Speed Is the Magnitude of Velocity

\(\text{speed at time }t=|v(t)|.\)

Velocity includes direction and may be negative; speed is nonnegative. If \(v(4)=-7\) meters per second, the particle moves in the negative direction with speed 7 meters per second.

4. Acceleration Is the Rate of Change of Velocity

\(a(t)=v'(t)=s''(t).\)

Acceleration is the slope of the velocity graph and records how velocity changes. Positive acceleration means velocity is increasing numerically; negative acceleration means velocity is decreasing numerically. Acceleration does not directly state the direction of motion.

5. Keep the Quantities and Units Distinct

QuantityRelationshipIf position is meters and time is seconds
Position\(s(t)\)meters
Velocity\(v(t)=s'(t)\)meters per second
Speed\(|v(t)|\)meters per second
Acceleration\(a(t)=v'(t)=s''(t)\)meters per second squared

6. Rest Is Not Automatically a Direction Change

A particle is at rest wherever \(v(t)=0\). It changes direction at a rest time only if velocity changes sign across that time. A velocity graph may touch the time axis and remain on the same side, producing a momentary stop without a reversal.

\(\text{direction change at }t=c\quad\Longrightarrow\quad v(c)=0\text{ and }v\text{ changes sign at }c.\)

The reverse implication is false: \(v(c)=0\) alone is insufficient.

7. Speeding Up and Slowing Down

Speed increases when velocity and acceleration have the same sign because acceleration pushes velocity farther from zero. Speed decreases when their signs differ because acceleration pushes velocity toward zero.

VelocityAccelerationMotion directionSpeed behavior
positivepositivepositive directionspeeding up
positivenegativepositive directionslowing down
negativenegativenegative directionspeeding up
negativepositivenegative directionslowing down
\(v(t)a(t)>0\Rightarrow\text{speeding up},\qquad v(t)a(t)<0\Rightarrow\text{slowing down}.\)

8. Build a Motion Sign Chart

  1. Find \(v=s'\) and \(a=v'\).
  2. Solve \(v(t)=0\) for rest-time candidates.
  3. Solve \(a(t)=0\) for possible changes in speed behavior.
  4. Place all relevant times on one timeline within the physical domain.
  5. Test the signs of \(v\) and \(a\) on every interval.
  6. Translate each sign pair into direction and speed behavior.

Zeros of velocity divide direction intervals; zeros of velocity or acceleration can divide speeding-up and slowing-down intervals.

9. Connect the Three Graphs

  • The slope of the position graph is the value of velocity.
  • A local maximum or minimum of position can occur where velocity changes sign through zero.
  • The slope of the velocity graph is the value of acceleration.
  • A local maximum or minimum of velocity can occur where acceleration changes sign through zero.
  • Concavity of the position graph has the same sign as acceleration.

A horizontal position graph means the particle remains at one position over an interval. A single horizontal tangent means only instantaneous rest.

10. Average and Instantaneous Velocity

Average velocity over \([a,b]\) is displacement divided by elapsed time, while instantaneous velocity at \(a\) is the derivative:

\(v_{\mathrm{avg}}=\frac{s(b)-s(a)}{b-a},\qquad v(a)=s'(a).\)

A particle can return to its starting position, giving zero displacement and zero average velocity, even though it moved and had nonzero speed during the interval.

11. Interpret a Given Velocity or Acceleration Model

If velocity is given directly, it determines direction, rest times, and acceleration after differentiation, but it does not determine absolute position without one position value. Likewise, knowing acceleration alone does not reveal velocity or direction without additional velocity information.

12. Common AP Motion Errors

  • Using the sign of position to determine direction.
  • Reporting negative speed instead of taking \(|v|\).
  • Calling every zero of velocity a direction change without a sign test.
  • Using \(a>0\) to conclude that the particle moves right.
  • Claiming that \(a=0\) means the particle is at rest.
  • Testing only velocity when asked whether speed increases.
  • Ignoring the stated time domain, especially \(t\ge0\).

6. Detailed Worked Example and Error Check

Example 1: Complete motion analysis from position. Let

\(s(t)=t^3-6t^2+9t,\qquad t\ge0.\)

Differentiate and factor:

\(v(t)=3(t-1)(t-3),\qquad a(t)=6(t-2).\)

The critical times are 1 and 3 from velocity and 2 from acceleration.

IntervalSign of \(v\)Sign of \(a\)Conclusion
\((0,1)\)positivenegativemoves right and slows down
\((1,2)\)negativenegativemoves left and speeds up
\((2,3)\)negativepositivemoves left and slows down
\((3,\infty)\)positivepositivemoves right and speeds up

Velocity changes sign at both \(t=1\) and \(t=3\), so the particle changes direction at both times. It moves from \(s(0)=0\) to \(s(1)=4\), reverses and returns to \(s(3)=0\), then reverses again.

Example 2: Rest without reversal. Suppose \(s(t)=(t-2)^3\). Then

\(v(t)=3(t-2)^2.\)

The particle is at rest at \(t=2\), but \(v(t)>0\) on both sides. It pauses instantaneously and continues in the positive direction; it does not change direction.

Example 3: Start from velocity. Let \(v(t)=t^2-4t+3=(t-1)(t-3)\), \(t\ge0\). Then \(a(t)=2t-4\). The particle moves right on \([0,1)\) and \((3,\infty)\), moves left on \((1,3)\), and is at rest at 1 and 3. It speeds up on \((1,2)\) and \((3,\infty)\), where \(v\) and \(a\) have the same sign.

Without a value such as \(s(0)\), this velocity model cannot identify the particle's coordinate.

Example 4: Compare average and instantaneous velocity. A ball's height is \(s(t)=64-16t^2\) feet until it reaches the ground. Solving \(s(t)=0\) gives impact at \(t=2\). Since

\(v(t)=-32t,\qquad a(t)=-32,\)

its impact velocity is \(-64\) feet per second and impact speed is 64 feet per second. Its average velocity over the full fall is

\(\frac{s(2)-s(0)}{2-0}=\frac{0-64}{2}=-32\text{ ft/s}.\)

The average velocity and final instantaneous velocity differ because the velocity changes throughout the fall.

Example 5: Read motion from a position graph. Suppose a differentiable position graph rises on \((0,2)\), has a horizontal tangent at \(t=2\), falls on \((2,5)\), and is constant on \([5,7]\). Then velocity is positive on \((0,2)\), zero at 2, negative on \((2,5)\), and zero throughout \([5,7]\). The particle reverses at \(t=2\) and remains at one fixed position from time 5 through time 7.

7. AP Reasoning Routine

Name variables and units, write the relationship before differentiating, substitute values at the correct time, and interpret the sign in context.

  • Identify the representation and requested quantity.
  • State the rule or theorem and verify its conditions.
  • Keep exact values until the final requested approximation.
  • Interpret sign, units, interval, and context.
AP Checkpoint

Let \(s(t)=t^3-3t^2-9t\), for \(t\ge0\), unless a part states otherwise.
(a) Find velocity and acceleration, all rest times, and every interval of positive- and negative-direction motion.
(b) Find the particle's position, velocity, speed, and acceleration at \(t=2\), with appropriate distinctions among them.
(c) Determine every interval on which the particle is speeding up or slowing down.
(d) Does the particle change direction at each rest time? Justify using velocity signs.
(e) For a different particle with \(v(t)=(t-2)^2\), explain what happens at \(t=2\).
(f) A position graph is decreasing and concave up at \(t=5\). State the signs of velocity and acceleration and decide whether speed is increasing or decreasing.
(g) If position is measured in kilometers and time in hours, state the units of \(s\), \(v\), \(|v|\), and \(a\).
(h) Explain why \(a(4)=0\) does not establish that a particle is at rest or changes direction at \(t=4\).

Check the solution

In part (a), \(v(t)=3t^2-6t-9=3(t-3)(t+1)\) and \(a(t)=6t-6\). In the domain \(t\ge0\), the only rest time is \(t=3\). Velocity is negative on \([0,3)\) and positive on \((3,\infty)\), so the particle moves in the negative direction before 3 and the positive direction after 3. In part (b), \(s(2)=-22\) is the position, \(v(2)=-9\) is the velocity, \(|v(2)|=9\) is the speed, and \(a(2)=6\) is the acceleration. In part (c), acceleration is negative on \((0,1)\) and positive on \((1,\infty)\). Thus \(v\) and \(a\) have the same sign on \((0,1)\) and \((3,\infty)\), where the particle speeds up; their signs differ on \((1,3)\), where it slows down. In part (d), velocity changes from negative to positive at \(t=3\), so the particle does change direction there. In part (e), velocity is zero at 2 but positive on both sides, so the particle rests instantaneously without reversing direction. In part (f), decreasing position gives \(v(5)<0\), and concave up gives \(a(5)>0\). Opposite signs mean the particle is slowing down. In part (g), position is kilometers, velocity and speed are kilometers per hour, and acceleration is kilometers per hour squared. In part (h), \(a(4)=0\) says only that velocity has zero instantaneous rate of change at that time. Rest and direction change depend on the value and sign behavior of velocity.