Uniform Accelerated Motion and Kinematic Equations

Conditions of Speeding Up and Speeding Down in a Straight Line

  • Speeding Up (Increase in Speed):

    • This occurs when the velocity vector v\mathbf{v} and acceleration vector a\mathbf{a} are parallel to each other.
    • The angle between velocity and acceleration is θ=0\theta = 0^{\circ}.
    • Speeding up happens in two sign-based cases:
    • Both velocity and acceleration are positive ((+v)(+v) and (+a)(+a)).
    • Both velocity and acceleration are negative ((v)(-v) and (a)(-a)).
  • Speeding Down (Decrease in Speed) / Retardation:

    • This occurs when the velocity vector v\mathbf{v} and acceleration vector a\mathbf{a} are antiparallel to each other.
    • The angle between velocity and acceleration is θ=180\theta = 180^{\circ}.
    • Speeding down happens when the variables have opposite signs:
    • Velocity is positive and acceleration is negative ((+v)(+v) and (a)(-a)).
    • Velocity is negative and acceleration is positive ((v)(-v) and (+a)(+a)).

Uniform Accelerated Motion

  • Core Characteristics:
    • The acceleration a\mathbf{a} is constant throughout the entire duration of the motion.
    • The change in velocity in equal time intervals is always the same.
    • Constant acceleration can be expressed by the equality of velocity changes over time: a=v2v1t1=v4v3t2a = \frac{v_2 - v_1}{t_1} = \frac{v_4 - v_3}{t_2}.

Equations of Motion

These equations are exclusively valid for uniform accelerated motion:

  1. Velocity-Time Relation:

    • v=u+at\mathbf{v} = \mathbf{u} + \mathbf{a}t
  2. Displacement-Time Relation (Initial Velocity):

    • s=ut+12at2\mathbf{s} = \mathbf{u}t + \frac{1}{2}\mathbf{a}t^2
  3. Displacement-Time Relation (Final Velocity):

    • s=vt12at2\mathbf{s} = \mathbf{v}t - \frac{1}{2}\mathbf{a}t^2
  4. Velocity-Displacement Relation:

    • v2=u2+2asv^2 = u^2 + 2as
  5. Displacement-Average Velocity Relation:

    • s=(u+v2)t\mathbf{s} = (\frac{\mathbf{u} + \mathbf{v}}{2})t

Variable Key:

  • vv: Final velocity
  • uu: Initial velocity
  • aa: Acceleration
  • tt: Time interval
  • ss: Displacement, calculated as the change in position s=rfri\mathbf{s} = \mathbf{r}_f - \mathbf{r}_i

Procedural Guidelines for Motion Problems

  • Step 1: Select the origin. Generally, the starting point of the motion is considered the origin.
  • Step 2: Select one direction as positive (++) and the opposite direction as negative (-).
  • Step 3: Always input all variables into equations with their proper sign according to the chosen convention.

Special Observations and Ratios

  • Galileo's Law of Odd Numbers: If the initial conditions are set such that v=0v = 0 (starting from rest) and the acceleration aa is constant, the ratio of displacements in successive equal time intervals (s1:s2:s3s_1 : s_2 : s_3) is represented by the ratio of odd numbers:
    • s1:s2:s3=1:3:5s_1 : s_2 : s_3 = 1 : 3 : 5
  • Chronological Data:
    • Session: Day-07
    • Date: 24/07/24