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Chapter 2: 1-D Motion & Kinematics – Study Notes

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Chapter 2: 1-D Motion & Kinematics

Introduction to 1-D Motion

One-dimensional (1-D) motion describes the movement of objects along a single axis, typically the x-axis. This chapter introduces the foundational concepts and equations used to analyze such motion, including position, displacement, velocity, and acceleration.

Coordinate System and Position

  • Coordinate System: Defines the reference axis (or axes) and the origin (reference point) for measuring motion.

  • Position (x): The location of an object along the chosen axis, measured from the origin.

Displacement

  • Displacement (Δx): The change in position of an object. Formula: where is the final position and is the initial position.

  • Example: If a car moves from m to m, then m.

Velocity

  • Average Velocity (vav): The rate of change of displacement over time. Formula:

  • Instantaneous Velocity: The velocity at a specific instant, given by the slope of the position vs. time graph at a single point.

  • Graphical Interpretation:

    • On a position vs. time plot, the slope between two points gives the average velocity.

    • The slope at a single point gives the instantaneous velocity.

Acceleration

  • Average Acceleration (aav): The rate of change of velocity over time. Formula:

  • Instantaneous Acceleration: The acceleration at a specific instant, given by the slope of the velocity vs. time graph at a single point.

  • Graphical Interpretation:

    • On a velocity vs. time plot, the slope between two points gives the average acceleration.

    • The slope at a single point gives the instantaneous acceleration.

Kinematic Equations for Constant Acceleration

When acceleration is constant, the following kinematic equations describe 1-D motion:

Equation

Missing Variable

Variables: = position, = initial position, = final velocity, = initial velocity, = acceleration, = time.

Solving Kinematics Problems: Holt's Kinematic Algorithm (HoKA)

  • Choose a coordinate system.

  • Make a table of the variables: , , , , , and .

  • Identify all known quantities; typically, there are at least two unknowns (one needed, one not needed).

  • Use the equation that does not contain the unwanted variable to solve for the desired quantity.

Worked Examples

Example 1: Freefall

  • Problem: Noodle the cat fell off his cat tower and landed with a speed of 24 m/s.

    • (a) How far up was he when he fell?

    • (b) For how long was he falling?

  • Solution: Use kinematic equations with , m/s, m/s2 (downward).

    • Distance: m

    • Time: s

Example 2: Maximum Height

  • Problem: A small rock is thrown straight up. Neglect air resistance. When the rock is at its maximum height, its velocity is zero. What is its acceleration at this instant?

  • Solution: The acceleration is m/s2 (downward), even at the instant when velocity is zero.

Example 3: Uniform Deceleration

  • Problem: A truck covers 40.0 m in 8.50 s while uniformly slowing down to a final velocity of 2.80 m/s.

    • (a) Find the truck's original speed.

    • (b) Find its acceleration.

  • Solution:

    • Original speed: m/s

    • Acceleration: m/s2

Example 4: Two Cars on a Line

  • Problem: A red car and a green car move toward each other along an x-axis. At time , the red car is at and the green car is at m. If the red car has a constant velocity of 20 km/h, the cars pass each other at m. But if the red car has a constant velocity of 40 km/h, they pass each other at m. What are (a) the initial velocity and (b) the constant acceleration of the green car?

    • Initial velocity of green car: m/s

    • Constant acceleration of green car: m/s2

Summary Table: Kinematic Equations

Equation

Missing Variable

Additional info: The notes are based on lecture slides and include both conceptual explanations and worked examples, suitable for introductory college physics students studying kinematics in one dimension.

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