In-depth Notes on Rotation

Rigid Body Rotation

  • Rigid Body: A body that can rotate with all parts locked together without changing shape.

  • Fixed Axis: Rotation occurs about a stationary axis.

Rotational Variables

1. Angular Position
  • Defined by the arc from the x-axis (zero angular position) to the reference line.

  • Measured in radians (rad).

2. Angular Displacement
  • Change in angular position from ( \theta1 ) to ( \theta2 ):
    Δθ=θ2−θ1

  • Positive for counterclockwise rotation, negative for clockwise.

3. Angular Velocity
  • Average angular velocity between two time points ( t1 ) and ( t2 ):
    ωavg=ΔθΔt\omega_{avg} = \frac{\Delta \theta}{\Delta t}

  • Instantaneous angular velocity:
    ω=limΔt0ΔθΔt\omega = \lim_{\Delta t \to 0} \frac{\Delta \theta}{\Delta t}

4. Angular Acceleration
  • If angular velocity changes, there is angular acceleration.

  • Average angular acceleration:
    αavg=ΔωΔt\alpha_{avg} = \frac{\Delta \omega}{\Delta t}

  • Instantaneous angular acceleration:
    α=limΔt0ΔωΔt\alpha = \lim_{\Delta t \to 0} \frac{\Delta \omega}{\Delta t}

Unit: ( \text{rad/s}^2 ).

Relationship Between Linear and Angular Variables

  • For a point at a position ( r ) from the rotation axis:
    s=rΔθs = r \Delta \theta

  • Differentiating with respect to time gives linear velocity ( v ):
    v=rωv = r \omega

  • The period of revolution ( T ) relates to angular velocity:
    T=2πωT = \frac{2\pi}{\omega}

Kinetic Energy of Rotation

  • Total kinetic energy of a rotating body:
    K=21​mivi2
    where ( v_i = r\omega ), leading to:
    K=12Iω2K = \frac{1}{2} I \omega^2
    where ( I ) is the moment of inertia.

Rotational Inertia (Moment of Inertia)

  • Defines resistance to rotation.

  • Dependent on mass and axis of rotation:

    I=∑miri2
    I=miri2

  • Varies based on distribution of mass regarding the rotation axis.

  • Moment of inertia examples:

    • Rod around longitudinal axis:
      I=112mL2I = \frac{1}{12} m L^2

  • Solid sphere:
    I=25mR2I = \frac{2}{5} m R^2

  • Hoop:
    I=mR2I = m R^2

Torque

  • Defined as a force's ability to cause rotation:
    τ=rFsin(θ)\tau = r F \sin(\theta)
    where ( \theta ) is the angle between the force vector and the lever arm.

  • Effects of torque:

    • Greater distance from pivot increases torque.

    • Torque also depends on the angle of application.

Newton's Law of Rotation

  • Relation between torque and angular acceleration:
    Tnet=IαT_{net} = I \alpha

  • Where ( T_{net} ) is net torque and ( \alpha ) is angular acceleration.

Work and Power in Rotation

  • Work done by torque:
    W=τΔθW = \tau \Delta \theta

  • Power related to torque:
    P=Wt=τωP = \frac{W}{t} = \tau \omega

Summary of Key Formulas

Quantity

Formula

Angular position

( \theta )

Angular velocity

( \omega = \frac{\Delta \theta}{\Delta t} )

Angular acceleration

( \alpha = \frac{\Delta \omega}{\Delta t} )

Moment of inertia

( I = \sum mi ri^2 )

Torque

( \tau = r F \sin(\theta) )

Work

( W = \tau \Delta \theta )

Power

( P = \tau \omega )