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Physics · Ch 2 — Motion in a Straight Line

Summary

Summary

  • Frame of reference: Motion is described relative to a chosen origin and axes. Position is a vector x⃗\vec{x}; in one dimension, it is simply xx with sign.
  • Path length & displacement: Distance is the total length of the path traveled (scalar). Displacement Δx=xf−xi\Delta x = x_f - x_i is the straight-line change in position (vector). Displacement can be zero even if distance is not.
  • Average velocity & speed: Average velocity vˉ=ΔxΔt\bar{v} = \frac{\Delta x}{\Delta t} (vector). Average speed =total distancetotal time= \frac{\text{total distance}}{\text{total time}} (scalar). For a round trip, average velocity is zero but average speed is not.
  • Instantaneous velocity: v=lim⁡Δt→0ΔxΔt=dxdtv = \lim_{\Delta t \to 0} \frac{\Delta x}{\Delta t} = \frac{dx}{dt}. It is the slope of the xx–tt graph at that instant.
  • Acceleration: Average acceleration aˉ=ΔvΔt\bar{a} = \frac{\Delta v}{\Delta t}; instantaneous acceleration a=dvdt=d2xdt2a = \frac{dv}{dt} = \frac{d^2x}{dt^2}. Acceleration is the slope of the vv–tt graph.
  • Equations of motion (constant acceleration aa): For motion along a straight line with uniform aa:

v=u+atv = u + at

s=ut+12at2s = ut + \frac12 at^2

v2=u2+2asv^2 = u^2 + 2as

where uu = initial velocity, vv = final velocity, ss = displacement, tt = time.

  • Graphical interpretation: Slope of xx–tt gives vv; slope of vv–tt gives aa; area under vv–tt graph gives displacement.
  • Free fall: A special case of constant acceleration (a=g≈9.8 m/s2a = g \approx 9.8\ \text{m/s}^2 downward). All equations of motion apply with a=−ga = -g (if upward is positive).

Table of Physical Quantities

Physical quantitySymbolDimensionsUnitRemarks
Path length--[L]m
DisplacementΔx\Delta x[L]m=x2−x1= x_2 - x_1. In one dimension, its sign indicates the direction.
Velocity (a) Averagevˉ\bar{v}[LT−1^{-1}]m s−1^{-1}=ΔxΔt= \dfrac{\Delta x}{\Delta t}
Velocity (b) Instantaneousvv[LT−1^{-1}]m s−1^{-1}=lim⁡Δt→0ΔxΔt=dxdt= \displaystyle\lim_{\Delta t \to 0} \dfrac{\Delta x}{\Delta t} = \dfrac{dx}{dt}. In one dimension, its sign indicates the direction.