Circular Motion Study Guide

Introduction to Circular Motion

  • Overview of topic 2.9: Circular Motion in AP Physics.

  • Instructor: Kristen Gonzalez Vega, Centennial High School, Frisco, Texas.

Forces Affecting Motion

  • Discussion on forces acting perpendicular or parallel to an object's displacement.

  • Key Principles:

    • Forces acting parallel to motion affect speed (acceleration).

    • Forces acting perpendicular to motion affect direction.

Application of Forces in Vehicle Motion

  • Scenario: Driving a car forward.

    • Possible actions to change motion:

    • Speeding up: Pressing the gas leads to static friction force accelerating the car.

    • Slowing down: Pressing the brakes leads to kinetic friction slowing down the car.

    • Turning left or right: Static friction facilitates the turn to avoid skidding.

  • Conclusion: Forces are responsible for changes in motion; net force causes this change.

Understanding Motion Changes

  • Examining the combined action of parallel and perpendicular forces in motion:

    • Forward Acceleration: Forces parallel to motion (e.g., driving forward).

    • Direction Change: Forces perpendicular to motion (e.g., turning).

    • Result: The car can speed up and turn simultaneously.

Accelerations in Circular Motion

  • Tangential Acceleration (a_t):

    • Defined as the rate of change of speed along a path;

    • Affects speeding up or slowing down an object.

  • Centripetal Acceleration (a_c):

    • Always directed toward the center of the circular path;

    • Defined as acceleration required for circular motion.

    • Equation: {a_c = rac{v^2}{r}} where:

    • v = velocity of the object,

    • r = radius of the circular path.

  • Net Acceleration:

    • Resultant of tangential and centripetal accelerations.

    • Can occur in various combinations:

    • Only tangential acceleration when moving in a straight line and accelerating.

    • Only centripetal acceleration when moving at a constant speed while turning.

    • Both when simultaneously turning and speeding up/slowing down.

Practical Example: Block on a String

  • Setup: Block attached to a string and pushed to move in a circle.

  • Observation Points: Two key points at approximate positions 2 o'clock (upper right) and 8 o'clock (lower left).

    • 2 o'clock Position:

    • Velocity: Tangent to the path, directed up to the left.

    • Tangential Acceleration: Kinetic friction acting backwards (slowing down).

    • Centripetal Acceleration: Tension force pointing towards the center.

    • Net Acceleration: Intermediate vector between backward (tangential) and inward (centripetal).

    • 8 o'clock Position:

    • Velocity: Tangent to the path, directed down to the right.

    • Tangential Acceleration: Kinetic friction opposing motion, directed backward.

    • Centripetal Acceleration: Tension directed towards the center.

    • Net Acceleration: Similar to the 2 o'clock position.

Applying Newton's Laws

  • Perpendicular Direction:

    • Net force (tension) directed towards aligning with centripetal acceleration:

    • T = m a_c (where T = tension, {m} = mass of the block).

  • Parallel Direction:

    • Net force (kinetic friction) affects tangential acceleration:

    • f{k} = m at (where f{k} = kinetic friction and {at} is tangential acceleration).

Example: Marble on a Roller Coaster

  • Marble follows a path that dips and rises.

  • Analysis at Key Points:

    • Bottom of the Hill:

    • Follows circular motion; normal force upwards exceeds gravitational force downwards:

      • Net Force Equation: FN - mg = mac

      • Results in normal force: F_N = rac{mv^2}{r} + mg

    • Top of the Hill:

    • Gravitational force downwards exceeds normal force upwards:

      • Net Force Equation: mg - FN = mac

      • Results in normal force: F_N = mg - rac{mv^2}{r}

  • Comparison: Normal force is greater at the bottom of the hill compared to the top.

Summary of Key Concepts

  • Forces parallel to velocity lead to tangential acceleration.

  • Forces perpendicular to velocity induce centripetal acceleration.

  • Expressions:

    • ext{Net Force Parallel} = m a_t

    • ext{Net Force Perpendicular} = m a_c

  • Clarification: There is no distinct force called centripetal force; it is the net force creating centripetal acceleration, which can consist of multiple forces acting together.