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Rotational Motion Simplified Revision Notes

Revision notes with simplified explanations to understand Rotational Motion quickly and effectively.

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11.1.3 Rotational Motion

Key Terms and Definitions

  1. Angular Displacement (θθ): The angle an object turns through in any given direction, measured in radians (rad).
  2. Angular Speed (ωω): The rate at which an object rotates, defined as the angle it covers per unit of time. Units are rads⁻¹.
  3. Angular Velocity (ωω): The rate of change of angular displacement per unit of time, with a direction (can be clockwise or anti-clockwise). Units are rads⁻¹.
  4. Angular Acceleration (αα): The rate of change of angular velocity over time, measured in rads⁻²

Relationship between Linear and Rotational Quantities

Rotational quantities have analogous equations to those in linear motion, making it easier to understand and remember rotational motion equations.

Linear QuantityRotational Quantity
Linear Velocity v=displacementtimev = \frac{\text{displacement}}{\text{time}}Angular Velocity ω=ΔθΔt\omega = \frac{\Delta \theta}{\Delta t}
Linear Acceleration a=velocitytimea = \frac{\text{velocity}}{\text{time}}Angular Acceleration α=ΔωΔt\alpha = \frac{\Delta \omega}{\Delta t}
image

Uniform and Non-Uniform Angular Acceleration

  • Uniform Angular Acceleration: This occurs when angular acceleration remains constant over time.
    • In this case, a graph of angular velocity against time will be a straight line.
    • The gradient of the line on this graph gives the angular acceleration.
    • The area under this graph represents angular displacement.
  • Non-Uniform Angular Acceleration: When angular acceleration varies with time.
    • The angular velocity graph will not be a straight line, but curved.
    • To find acceleration at a specific point, draw a tangent and calculate its gradient.
image

Graphs Related to Uniform Angular Acceleration

  1. Angular Velocity vs. Time:
  • For uniform acceleration, this graph is a straight line.
  • Gradient of the line = Angular acceleration.
  • Area under the line = Angular displacement.
  1. Angular Displacement vs. Time:
  • For uniform acceleration, angular displacement increases quadratically with time, creating a parabolic curve.
image

Equations of Motion for Uniform Angular Acceleration

These equations are similar to the SUVAT equations for linear motion but applied to rotational variables:

Linear Motion EquationRotational Motion Equation
v=u+atv = u + atω2=ω1+αt\omega_2 = \omega_1 + \alpha t
s=12(u+v)ts = \frac{1}{2} (u + v)tθ=12(ω1+ω2)t\theta = \frac{1}{2} (\omega_1 + \omega_2)t
s=ut+12at2s = ut + \frac{1}{2}at^2θ=ω1t+12αt2\theta = \omega_1 t + \frac{1}{2} \alpha t^2
v2=u2+2asv^2 = u^2 + 2asω22=ω12+2αθ\omega_2^2 = \omega_1^2 + 2 \alpha \theta

Where:

  • θ\theta = Angular displacement
  • ω1\omega_1 = Initial angular velocity
  • ω2\omega_2 = Final angular velocity
  • α\alpha = Angular acceleration
  • tt = Time
infoNote

Example Problem

Example: A wheel starts from rest and accelerates with an angular acceleration of 2 rads⁻² for 5 seconds. Find the angular velocity and angular displacement at the end of 5 seconds.

Solution:

  1. Given:
  • Initial angular velocity, ω1=0\omega_1 = 0
  • Angular acceleration, α=2 rads2\alpha = 2 \text{ rads}^{-2}
  • Time, t=5 st = 5 \text{ s}
  1. Final Angular Velocity:
ω2=ω1+αt=0+(2)(5)=:success[10textrads1]\omega_2 = \omega_1 + \alpha t = 0 + (2)(5) = :success[10 text{ rads}^{-1}]
  1. Angular Displacement:
θ=ω1t+12αt2=05+12(2)(5)2=0+25=:success[25textrad]\theta = \omega_1 t + \frac{1}{2} \alpha t^2 = 0 \cdot 5 + \frac{1}{2} (2) (5)^2 = 0 + 25 = :success[25 text{ rad}]
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