Unit 6: Rotational Motion

Unit 6: Rotational Motion

Introduction

  • Definition of Rotational Motion: Rotational motion is essential in everyday life. It includes the rotation of
      the Earth, wheels, and various technological applications, from Swiss watches to heavy machinery.

  • Key Concepts: To understand rotational motion, three key concepts are crucial:
      - Angular Velocity
      - Angular Acceleration
      - Centripetal Acceleration

  • Applications: These concepts help in understanding various motions:
      - A car on a circular racetrack
      - Clusters of galaxies orbiting a center

  • Integration with Newton's Laws:
      - Rotational motion, combined with Newton’s law of universal gravitation, helps explain space travel and satellite placement.
      - Energy conservation principles and gravitational potential energy relate to planetary escape speed.

6.1 Rotation About a Fixed Axis

  • Axis of Rotation: The axis about which an object rotates. Every rotating body has this axis.
      - Example: Earth has two axes of rotation.
Notes of Importance (N.B.):
  • All parameters such as angular displacement (q), work (w), angular acceleration (a), time (t), and angular momentum (L) are represented using the right-hand rule of rotation about the axis O.
Angular Displacement
  • Definition: The angular position of a rotating disc about a fixed axis.
  • Reference Line: For the disc, a fixed line is chosen. A point P is located at a distance r from axis O.
  • As the disc rotates, point P traces an arc length s on the circular path made by radius r.

Detailed Description of Angular Concepts

Angular Displacement Equation
  • The relationship between angular displacement (ϴ), arc length (s), and radius (r):
    θ=sr\theta = \frac{s}{r}
  • SI Unit: The radian (rad) is defined as the angle subtended by an arc length equal to the radius of the arc,
    1rad=360°2π=57.3°1 rad = \frac{360°}{2\pi} = 57.3°
Revolution to Radians Conversion
  • 1 revolution = 360° = 2π radians
Angular Velocity (ω)
  • Definition: The rate of change of angular displacement over time.
  • Formula:
    ω=Δθt\omega = \frac{\Delta\theta}{t}
  • Measurement: Measured in radians/second (rad/s), it is a vector quantity.
Linear Velocity (V)
  • Definition: The speed of a rotating object tangent to the curve along the circular path.
  • Formula:
    V=ω×rV = \omega \times r
  • Conversion: SI unit is meters/second (m/s) = rad/s × m.
Example Calculation:
  • Calculate Angular Velocity of a Flywheel
      - Given: Radius = 2m, Linear velocity (V) = 16m/s.
      - Calculation:
    ω=Vr=162=8rad/s\omega = \frac{V}{r} = \frac{16}{2} = 8 rad/s

Exercises

  1. Flywheel Spins: A flywheel spins 250 times per minute.
    What is its angular velocity?
       - Answer: 26.17 rad/s

  2. CD Rotating: A CD rotates at 4800 revolutions per minute.
    What is the linear speed of a point at the rim (radius 40mm)?
       - Answer: 20.1 m/s

Worked Example 6.2
  • Given: CD rotating at 4800 revolutions per minute.
  • Find: Linear velocity of a point 40 mm from the axis of rotation.
  1. Calculate Angular Velocity:
    Angle turned in 60 s=4800×2π\text{Angle turned in 60 s} = 4800 \times 2\pi
       - Use the equation:
    ω=anglet\omega = \frac{\text{angle}}{t}
  2. Substituting Values:
    ω=4800×2π60=502.7rad/s\omega = \frac{4800 \times 2\pi}{60} = 502.7 rad/s
  3. Final Velocity Calculation:
    v=rω=0.04m×502.7rad/s=20.1m/sv = r\omega = 0.04 m \times 502.7 rad/s = 20.1 m/s

Review Questions

  1. Car Engine: A car engine rotates at 3000 revolutions per minute.
    What is its angular velocity in rad/s?

  2. Linear Velocity on a CD: The linear velocity of a point on a CD is a constant 1.2 m/s.
       - At the start (23 mm from center),
       - At the end (58 mm from center).
    What is the angular velocity?

  3. Car Wheel: A car traveling at 16 m/s has a wheel with a diameter of 0.7 m.
    Find the wheel's angular velocity in rad/s.

  4. Turbine: A turbine rotates at 3000 revolutions per minute.
       - a) What is its angular velocity in rad/s?
       - b) Calculate the linear velocity of a turbine blade at the end and halfway down the blade.

Angular Acceleration (α)

  • Definition: Angular acceleration is the rate of change of angular velocity over time.
  • Formula:
    α=Δωt\alpha = \frac{\Delta\omega}{t}
  • SI Unit: rad/s²
  • Other unit examples include rev/min².
Example of Angular Acceleration Calculation
  • A flywheel accelerates from 15.1 rad/s to 23.1 rad/s over 4 seconds.
  1. Angular Displacement (θ):
    θ=(ωi+ωf)×t2=(15.1+23.1)42=76.4rad\theta = \left(\omega_{i} + \omega_{f}\right) \times \frac{t}{2} = \left(15.1 + 23.1\right) \frac{4}{2} = 76.4 rad
  2. Find α:
    α=Δωt=23.115.14=2rad/s2\alpha = \frac{\Delta\omega}{t} = \frac{23.1 - 15.1}{4} = 2 rad/s²
Exercises
  1. Calculate Angular Acceleration:
       - If angular velocity increases from 3 rad/s to 23 rad/s in 4 seconds, find α.
  2. Final Angular Velocity: A flywheel starts from rest and rotates at 3 rad/s² for 5 seconds. Find the final angular velocity.

Rotational Kinematics

Constant Angular Acceleration
  • The simplest motion to analyze is rotational motion under constant angular acceleration.
Exercises
  1. Exercise Bike: Angular velocity at the rear wheel is 4 rad/s at t=0 with an acceleration of 2 rad/s².
       - a. Angle with x-axis at t=3 s?
       - b. Angular velocity at this time?

  2. Disk Comparison: A disk rotates; Point B is three times farther from the axis than Point A. If the speed of B is V, what is the speed of A?

  3. Disk with Increasing Angular Velocity: A disk's Point B is twice as far from the axis as Point A. Analyze the angular and radial acceleration of A and B.

  4. Discus Thrower: An angular acceleration of 50 rad/s² moves a discus in a circle of radius 0.8 m. Find radial and tangential components of acceleration.

  5. Fairground Wheel: A wheel makes 1 rev every 8 s and decelerates at -0.1 rad/s². What is the initial angular velocity of someone located at 4 m from the axis?

6.2 Torque and Angular Acceleration

  • Torque (τ): The rotational effect of force. Defined and measured as:
    τ=rimesFsin(θ)\tau = r imes F \sin(\theta)
      where
    θ\theta is the angle between force and position vector.
  • Units: Torque uses the unit N.m, which differs from Joules (work and energy).
Definition of Torque
  • Torque can also be defined as:
    τ=rxF\tau = r x F
Vector Product of Two Vectors
  • The vector product from unit lessons states that:
    τ=rxF=rFsin(θ)\tau = r x F = |r||F| \sin(\theta)
  • Remember in vector products, the orientation of forces plays a crucial role in determining the resultant torque.
Exercises
  1. Force Torque: If a force of (3i + 4j) N acts at (120i + 50j) cm from a pivot, determine the torque produced. (Find the angle between r and F.)
  2. Mechanic Torque: A mechanic applies a 270 N force at 50 cm from a nut pivot. What is the torque produced, and how much work is done when rotating it through a half turn?
  3. Force at Position Calculation: Calculate torque exerted by (2N, -5N) at (3m, 1m) from the pivot.

6.3 Rotational Kinetic Energy and Moment of Inertia (MOI)

  • Definition of Rotational Inertia: The rotating body's resistance to change in motion, equivalent to mass in linear motion.
      - The moment of inertia (I) influences how hard it is to change the rotation of a body.
      - Torque relationship:
    τ=Iα\tau = I\alpha
Moment of Inertia for Point Mass and Rigid Bodies
  • For a point mass:
    I=mr2I = mr^2
      - Where m is mass and r is the distance from the axis of rotation.
  • For a rigid body:
      - Sum of moment of inertia for point masses:
    I=miri2I = \sum m_{i}r_{i}^2
Specific Shapes and their Moment of Inertia
  • Examples:
      - Thin disk:
    I=12MR2I = \frac{1}{2} MR^2
      - Slender rod: Calculations vary based on where the axis passes through (center or end).
Rotational Kinetic Energy
  • Rotational Equivalent of Kinetic Energy: In linear motion, the kinetic energy is given by the equation
    EK=12mv2E_K = \frac{1}{2} mv^2
      - For rotation, we rephrase as:
    Erot=12Iω2E_{rot} = \frac{1}{2} I\omega^2
      - This energy also depends on the position of the axis of rotation.
Exercises
  1. Point Mass Energy: Calculate the rotational kinetic energy of a 2kg point mass moving at 5 rad/s, 0.5m from the axis.
  2. Drum Rotation: Find the rotational kinetic energy of a drum with an I of 16000 kg.m² and an angular speed of 3 rad/s.
  3. Torque and Work Done Calculation: A person pulls on a cord on a drum with a diameter of 32cm. Find torque, work done, and the angle the drum rotates.
  4. Cylinder Acceleration: Analyze the acceleration of a cylinder when a string is pulled with a force of 16N.
  5. Rolling Ball's Total Kinetic Energy: Determine the total kinetic energy of a 5-kg ball rolling at 4m/s with a radius of 10cm.
  6. Inclined Plane Roll: Analyze the motion of a ring, solid cylinder, and sphere rolling down a slope from a height of 1m without slipping. Determine the order and time taken to reach the bottom.

6.4 Work and Power

  • Work Done by Torque: Work done can be calculated by:
    W=τ×qW = \tau \times q
      - Torque has a directional component, with cos(0°) highlighting the effects of linear force components.
      - SI Units: Work (Joules) can be formulated through torque and angular displacement.
Power in Rotational Motion
  • Rotational Power: The rate of work done in a rotational context is denoted as:
    P=Wt=τ×ωP = \frac{W}{t} = \tau \times \omega
  • Compare to the linear power format:
    P=Wt=F×S/t=F×VP = \frac{W}{t} = F \times S/t = F \times V
Exercises
  1. Mechanic's Power Development: If a mechanic applies a torque of 160 N.m over three-quarters of a turn in 2 seconds, find the power developed.

6.5 Parallel Axis Theorem

  • Parallel Axis Theorem: The moment of inertia about a parallel axis is calculated by:
    IP=ICM+Md2I_P = I_{CM} + M d^2
      - Where M is mass of the rigi body, and d is the distance between the two axes.
Exercises
  1. Moment of Inertia Calculation: For an 8 kg rigid body with a MOI of 60 kg.m², rotated about a parallel axis 0.6m from the CM, calculate the MOI about the new axis.
  2. Uniform Solid Sphere: Verify moment of inertia about its surface parallel axis from the center calculation results: Show as (7/5)mR².
  3. Moment of Inertia Comparisons: Compute MOI for solid cylinder, hollow cylinder, and solid sphere when their axes are at the edge compared to the center.

6.6 Angular Momentum and Angular Impulse

  • Angular Momentum (L): Similar to linear momentum, but expressed as:
    L=IωextorL=mvrL = I\omega ext{ or }L = mvr
      - For point mass:
    L=mr2ω=r×m×vL = mr^2 \omega = r \times m \times v
Angular Impulse Defined
  • Definition of Linear Impulse:
    J=Fnetimesextchangeintime=ΔpJ = F_{net} imes ext{change in time} = \Delta p
  • Angular Impulse:
    J=τnet×Δt=ΔLJ = \tau_{net} \times \Delta t = \Delta L
  • Units of Angular Impulse are represented as Newton-meter-second [J] = N.m.s.
Exercises
  1. Flywheel Angular Momentum Calculation: Given a flywheel rotating at 1000 rev/min with an MOI of 50 kg.m², determine the angular momentum.
  2. Rotating Flywheel: Analyze the influence of a 2 kg mass on a flywheel’s angular speed after a duration of 2.5 s.

6.7 Conservation of Angular Momentum

  • Law of Conservation of Angular Momentum: When the net torque acting on a rotating body is zero, its angular momentum remains constant:
    τnet=0    L=constant\tau_{net} = 0 \implies L = \text{constant}
  • Applications: Skating and diving scenarios help to demonstrate this principle.
Exercises
  1. Skater's Angular Momentum Change: A skater spins with an initial moment of inertia of 1.2 kg.m² at 5 rad/s. If she extends her arms, and spins at 1.8 rad/s, find her new MOI.

6.8 Center of Mass of a Rigid Body

  • Center of Mass (C.M.): A rigid body balances freely when supported at its center of mass.
  • Geometric Center: For uniform rigid bodies such as discs, the C.M. is at geometric center.
  • Non-uniform Bodies: C.M. shifts closer to denser mass ends, such as in irregular shapes or significant mass distributions (e.g., Sun-Earth).
Exercises
  1. Determine C.M.: Given various point masses, find the overall center of mass for the system.

Additional Solved Problems

  1. Helicopter Rotor: A rotor turns at 3.20 × 10^2 revolutions per minute. Find its angular velocity in radians per second, arc lengths traced, and average angular velocity during increased throttle.
  2. Angular Acceleration Calculation: If angular velocity reduces from 15 rad/s to 9 rad/s in 3 seconds, calculate average angular acceleration.
  3. Acceleration Summary: Evaluate a wheel's rotation with a constant angular acceleration of 3.50 rad/s² from an initial velocity of 2 rad/s over 2 seconds, understanding total distance traveled in radians and revolutions.
  4. Compact Disc Player: Analyze speed changes within compact disc technology, gauging speed variations depending on read head positions.
  5. Race Car Dynamics: Analyze the uniform acceleration of a race car, gauge centripetal dynamics over a circular race track, while maintaining equations for kinematic continuity.

Conclusion

These notes provide a comprehensive framework for understanding rotational motion principles along with practical exercises, reinforcing critical concepts related to angular dynamics.