AP Calculus BC 4.2 Straight-Line Motion Study Notes - New Syllabus
AP Calculus BC 4.2 Straight-Line Motion Study Notes- New syllabus
AP Calculus BC 4.2 Straight-Line Motion Study Notes – AP Calculus BC- per latest AP Calculus BC Syllabus.
LEARNING OBJECTIVE
- The derivative can be used to solve rectilinear motion problems involving position, speed, velocity, and acceleration.
Key Concepts:
- Straight-Line Motion:Connecting Position, Velocity, and Acceleration
Straight-Line Motion:Connecting Position, Velocity, and Acceleration
Straight-Line Motion:Connecting Position, Velocity, and Acceleration
In straight-line (one-dimensional) motion, the position of a moving object changes over time along a linear path.
The behavior of such motion can be modeled using three core functions in calculus:
Position function:
\( s(t) \) : describes the exact location (displacement) of an object along a straight line at time \( t \), typically measured in meters (m).
Velocity function:
\( v(t) = \dfrac{ds}{dt} \) : represents the rate of change of the position with respect to time. It tells both the speed and the direction of motion. Positive velocity indicates forward motion; negative velocity indicates backward motion.
Acceleration function:
\( a(t) = \dfrac{dv}{dt} = \dfrac{d^2s}{dt^2} \) : represents the rate of change of velocity with respect to time. It shows how the speed and/or direction of motion is changing.
Relationship Summary:
\( v(t) = \dfrac{ds}{dt} \quad \text{and} \quad a(t) = \dfrac{dv}{dt} = \dfrac{d^2s}{dt^2} \)
Concepts and Interpretation
- When \( v(t) > 0 \): The object is moving in the positive direction (right/forward).
- When \( v(t) < 0 \): The object is moving in the negative direction (left/backward).
- When \( v(t) = 0 \): The object is momentarily at rest.
- When \( a(t) > 0 \): The velocity is increasing; the object is speeding up (if already moving forward) or slowing down (if moving backward).
- When \( a(t) < 0 \): The velocity is decreasing; the object is slowing down (if moving forward) or speeding up (if moving backward).
Speeding Up vs. Slowing Down:
- The object is speeding up when velocity and acceleration have the same sign.
- The object is slowing down when velocity and acceleration have opposite signs.
Units and Real-World Meaning
- Position, \( s(t) \): measured in distance units like meters (m).
- Velocity, \( v(t) \): measured in meters per second (m/s); unit for position divided by time.
- Acceleration, \( a(t) \): measured in meters per second squared (m/s²); unit for velocity divided by time.
Example Interpretation: If \( v(3) = -5 \) and \( a(3) = -2 \), then the object is moving left at 5 m/s and speeding up (since velocity and acceleration are both negative).
Graphical Interpretation
- The graph of \( s(t) \) (position vs. time) gives insight into the motion of the object.
- The slope of the tangent to the graph of \( s(t) \) at a point gives the velocity \( v(t) \).
- The slope of the graph of \( v(t) \) gives the acceleration \( a(t) \).
- Points where \( v(t) = 0 \) correspond to turning points or rest points in the motion.
Example:
Suppose the position of a particle moving along a straight line is given by:
\( s(t) = 4t^3 – 3t^2 + 2t \), where \( s \) is in meters and \( t \) is in seconds.
Find:
- Velocity function \( v(t) \)
- Acceleration function \( a(t) \)
- Velocity and acceleration at \( t = 2 \)
▶️ Answer/Explanation
Differentiate \( s(t) \) to get velocity:
\( v(t) = \dfrac{ds}{dt} = 12t^2 – 6t + 2 \)
Differentiate \( v(t) \) to get acceleration:
\( a(t) = \dfrac{dv}{dt} = 24t – 6 \)
Evaluate at \( t = 2 \):
- \( v(2) = 12(2)^2 – 6(2) + 2 = 48 – 12 + 2 = 38 \) m/s
- \( a(2) = 24(2) – 6 = 48 – 6 = 42 \) m/s²
Example:
A car’s position along a straight road is modeled by the function:
\( s(t) = 100 – 20t + 3t^2 \), where \( s \) is in meters and \( t \) is in seconds.
Find:
- The velocity function \( v(t) \)
- The acceleration function \( a(t) \)
- Interpret the motion of the car at \( t = 4 \) seconds
▶️ Answer/Explanation
\( v(t) = \dfrac{ds}{dt} = -20 + 6t \)
\( a(t) = \dfrac{dv}{dt} = 6 \)
(Constant acceleration of 6 m/s²)
Evaluate at \( t = 4 \):
- \( v(4) = -20 + 6(4) = -20 + 24 = 4 \) m/s
- \( a(4) = 6 \) m/s²
Interpretation:
At 4 seconds, the car is moving forward at 4 m/s, and its velocity is increasing (accelerating) at a constant rate of 6 m/s².
Example:
A particle moves along a straight line such that its position at time \( t \) (in seconds) is given by the function:
\( s(t) = t^3 – 6t^2 + 9t + 5 \), where \( s(t) \) is measured in meters.
(a) Find the velocity and acceleration functions.
(b) At what time(s) is the particle at rest?
(c) Determine when the particle is moving to the right (positive velocity) and when it is moving to the left (negative velocity).
(d) Is the particle speeding up or slowing down at \( t = 1 \)? Justify your answer.
▶️ Answer/Explanation
(a) Velocity is the derivative of position:
\( v(t) = \dfrac{ds}{dt} = 3t^2 – 12t + 9 \)
Acceleration is the derivative of velocity:
\( a(t) = \dfrac{dv}{dt} = 6t – 12 \)
(b) The particle is at rest when \( v(t) = 0 \):
\( 3t^2 – 12t + 9 = 0 \Rightarrow t^2 – 4t + 3 = 0 \Rightarrow (t – 1)(t – 3) = 0 \)
So, the particle is at rest at \( t = 1 \) and \( t = 3 \) seconds.
(c) Use a sign chart for \( v(t) = 3t^2 – 12t + 9 \):
Critical points at \( t = 1 \) and \( t = 3 \)
- For \( t < 1 \), try \( t = 0 \): \( v(0) = 9 \) → positive
- For \( 1 < t < 3 \), try \( t = 2 \): \( v(2) = 3(4) – 12(2) + 9 = 12 – 24 + 9 = -3 \) → negative
- For \( t > 3 \), try \( t = 4 \): \( v(4) = 48 – 48 + 9 = 9 \) → positive
So, the particle is:
- Moving right when \( t \in ( -\infty, 1 ) \cup (3, \infty) \)
- Moving left when \( t \in (1, 3) \)
(d) At \( t = 1 \):
- \( v(1) = 3(1)^2 – 12(1) + 9 = 0 \) → particle is at rest
- \( a(1) = 6(1) – 12 = -6 \)
Since velocity is 0 and acceleration is negative, the particle is starting to move left. It’s speeding up in the negative direction → slowing down (relative to previous motion).