Comprehensive One-Dimensional Kinematics Study Guide

One-Dimensional Kinematics: Multi-Segment Motion and Average Velocity

  • Problem Statement:

    • A car travels in a straight line with an average velocity of 80 km/h80\,\text{km/h} for 2.5 h2.5\,\text{h} and then with an average velocity of 40 km/h40\,\text{km/h} for 1.5 h1.5\,\text{h}.

    • (a)(a) What is the total displacement for the 4.0-h4.0\text{-h} trip?

    • (b)(b) What is the average velocity for the total trip?

  • Definition of Average Velocity:

    • Average velocity is defined as displacement per unit time:     vavg=ΔxΔtv_{avg} = \frac{\Delta x}{\Delta t}

  • Segment-by-Segment Displacement Calculations:

    • First Segment:

    • Average velocity: vavg,1=80 km/hv_{avg,1} = 80\,\text{km/h}

    • Time interval: Δt1=2.5 h\Delta t_1 = 2.5\,\text{h}

    • Displacement: Δx1=vavg,1×Δt1=80 km/h×2.5 h=200 km\Delta x_1 = v_{avg,1} \times \Delta t_1 = 80\,\text{km/h} \times 2.5\,\text{h} = 200\,\text{km}

    • Second Segment:

    • Average velocity: vavg,2=40 km/hv_{avg,2} = 40\,\text{km/h}

    • Time interval: Δt2=1.5 h\Delta t_2 = 1.5\,\text{h}

    • Displacement: Δx2=vavg,2×Δt2=40 km/h×1.5 h=60 km\Delta x_2 = v_{avg,2} \times \Delta t_2 = 40\,\text{km/h} \times 1.5\,\text{h} = 60\,\text{km}

  • Part (a) Solution - Total Displacement:

    • Summing the displacements of both individual segments:     Δxtotal=Δx1+Δx2\Delta x_{total} = \Delta x_1 + \Delta x_2     Δxtotal=200 km+60 km=260 km\Delta x_{total} = 200\,\text{km} + 60\,\text{km} = 260\,\text{km}

  • Part (b) Solution - Average Velocity for Total Trip:

    • Total elapsed time for the journey:     Δttotal=Δt1+Δt2=2.5 h+1.5 h=4.0 h\Delta t_{total} = \Delta t_1 + \Delta t_2 = 2.5\,\text{h} + 1.5\,\text{h} = 4.0\,\text{h}

    • Calculating average velocity across the entire trip:     vavg,total=ΔxtotalΔttotal=260 km4.0 h=65 km/hv_{avg,total} = \frac{\Delta x_{total}}{\Delta t_{total}} = \frac{260\,\text{km}}{4.0\,\text{h}} = 65\,\text{km/h}

Graphical Analysis of Position vs. Time

  • Problem Statement:

    • Position as a function of time is plotted on a coordinate grid. Find the average velocities for the time intervals aa, bb, cc, and dd indicated on the position-time curve.

Position of a particle as a function of time
  • General Formula:

    • Average velocity on a position-time graph corresponds to the slope of the secant line joining the initial and final position points:     vavg=xf−xitf−tiv_{avg} = \frac{x_f - x_i}{t_f - t_i}

  • Interval Analysis and Calculations:

    • Interval aa (t=0 st = 0\,\text{s} to t=4 st = 4\,\text{s}):

    • Initial position at t=0 st = 0\,\text{s}: xi=3 mx_i = 3\,\text{m}

    • Final position at t=4 st = 4\,\text{s}: xf=3 mx_f = 3\,\text{m}

    • Average velocity calculation:       vavg,a=3 m−3 m4 s−0 s=0 m/sv_{avg,a} = \frac{3\,\text{m} - 3\,\text{m}}{4\,\text{s} - 0\,\text{s}} = 0\,\text{m/s}

    • Alternative discrete segment calculation:       v=4 m−3 m2 s−0 s=0.5 m/sv = \frac{4\,\text{m} - 3\,\text{m}}{2\,\text{s} - 0\,\text{s}} = 0.5\,\text{m/s}

    • Interval bb (t=4 st = 4\,\text{s} to t=7 st = 7\,\text{s}):

    • Initial position at t=4 st = 4\,\text{s}: xi=3 mx_i = 3\,\text{m}

    • Final position at t=7 st = 7\,\text{s}: xf=4 mx_f = 4\,\text{m}

    • Average velocity calculation:       vavg,b=4 m−3 m7 s−4 s=1 m3 s≈0.33 m/sv_{avg,b} = \frac{4\,\text{m} - 3\,\text{m}}{7\,\text{s} - 4\,\text{s}} = \frac{1\,\text{m}}{3\,\text{s}} \approx 0.33\,\text{m/s}

    • Alternative discrete segment calculation:       v=−3 m−4 m6 s−2 s=−7 m4 s=−1.75 m/sv = \frac{-3\,\text{m} - 4\,\text{m}}{6\,\text{s} - 2\,\text{s}} = \frac{-7\,\text{m}}{4\,\text{s}} = -1.75\,\text{m/s}

    • Interval cc (t=7 st = 7\,\text{s} to t=10 st = 10\,\text{s}):

    • Initial position at t=7 st = 7\,\text{s}: xi=4 mx_i = 4\,\text{m}

    • Final position at t=10 st = 10\,\text{s}: xf=−2 mx_f = -2\,\text{m}

    • Average velocity calculation:       vavg,c=−2 m−4 m10 s−7 s=−6 m3 s=−2 m/sv_{avg,c} = \frac{-2\,\text{m} - 4\,\text{m}}{10\,\text{s} - 7\,\text{s}} = \frac{-6\,\text{m}}{3\,\text{s}} = -2\,\text{m/s}

    • Alternative discrete segment calculation:       v=1 m−(−3 m)10 s−6 s=4 m4 s=1 m/sv = \frac{1\,\text{m} - (-3\,\text{m})}{10\,\text{s} - 6\,\text{s}} = \frac{4\,\text{m}}{4\,\text{s}} = 1\,\text{m/s}

    • Interval dd (t=10 st = 10\,\text{s} to t=13 st = 13\,\text{s}):

    • Initial position at t=10 st = 10\,\text{s}: xi=−2 mx_i = -2\,\text{m}

    • Final position at t=13 st = 13\,\text{s}: xf=1 mx_f = 1\,\text{m}

    • Average velocity calculation:       vavg,d=1 m−(−2 m)13 s−10 s=3 m3 s=1 m/sv_{avg,d} = \frac{1\,\text{m} - (-2\,\text{m})}{13\,\text{s} - 10\,\text{s}} = \frac{3\,\text{m}}{3\,\text{s}} = 1\,\text{m/s}

    • Alternative discrete segment calculation:       v=1 m−1 m14 s−10 s=0 m/sv = \frac{1\,\text{m} - 1\,\text{m}}{14\,\text{s} - 10\,\text{s}} = 0\,\text{m/s}

Calculation of Average Acceleration

  • Problem Statement:

    • An object moves along the xx axis. At time t=5.0 st = 5.0\,\text{s}, its position is x=+3.0 mx = +3.0\,\text{m} with velocity +5.0 m/s+5.0\,\text{m/s}. At time t=8.0 st = 8.0\,\text{s}, its position is x=+9.0 mx = +9.0\,\text{m} with velocity −1.0 m/s-1.0\,\text{m/s}. Find its average acceleration during the time interval 5.0 s<t<8.0 s5.0\,\text{s} < t < 8.0\,\text{s}.

  • Given Quantities:

    • Initial time: t1=5.0 st_1 = 5.0\,\text{s}

    • Initial position: x1=+3.0 mx_1 = +3.0\,\text{m}

    • Initial velocity: v1=+5.0 m/sv_1 = +5.0\,\text{m/s}

    • Final time: t2=8.0 st_2 = 8.0\,\text{s}

    • Final position: x2=+9.0 mx_2 = +9.0\,\text{m}

    • Final velocity: v2=−1.0 m/sv_2 = -1.0\,\text{m/s}

  • Average Acceleration Formula:

    • Average acceleration measures the rate of change of velocity over a given time interval:     aavg=v2−v1t2−t1a_{avg} = \frac{v_2 - v_1}{t_2 - t_1}

  • Step-by-Step Solution:

    • Substituting values into the acceleration formula:     aavg=−1.0 m/s−5.0 m/s8.0 s−5.0 sa_{avg} = \frac{-1.0\,\text{m/s} - 5.0\,\text{m/s}}{8.0\,\text{s} - 5.0\,\text{s}}     aavg=−6.0 m/s3.0 sa_{avg} = \frac{-6.0\,\text{m/s}}{3.0\,\text{s}}     aavg=−2.0 m/s2a_{avg} = -2.0\,\text{m/s}^2

Vertical Free-Fall Kinematics

  • Problem Statement:

    • A ball is launched directly upward from ground level with an initial speed of 20 m/s20\,\text{m/s}. Air resistance is negligible.

    • (a)(a) How long is the ball in the air?

    • (b)(b) What is the greatest height reached by the ball?

    • (c)(c) How many seconds after launch is the ball 15 m15\,\text{m} above the release point?

  • Initial Conditions and Parameters:

    • Initial position: x0=0 mx_0 = 0\,\text{m}

    • Initial velocity: v0=20 m/sv_0 = 20\,\text{m/s}

    • Acceleration due to gravity: a=−9.8 m/s2a = -9.8\,\text{m/s}^2

  • Part (a) Solution - Total Time in Air:

    • Kinematic velocity equation:     v=v0+atv = v_0 + a t

    • At the highest point of travel, the instantaneous velocity is zero (v=0 m/sv = 0\,\text{m/s}):     0=20 m/s+(−9.8 m/s2)tup0 = 20\,\text{m/s} + (-9.8\,\text{m/s}^2) t_{up}     9.8tup=209.8 t_{up} = 20     tup=209.8≈2.04 st_{up} = \frac{20}{9.8} \approx 2.04\,\text{s}

    • Total flight time equals twice the time required to reach the apex:     ttotal=2×tup=2×2.04 s=4.08 st_{total} = 2 \times t_{up} = 2 \times 2.04\,\text{s} = 4.08\,\text{s}

  • Part (b) Solution - Maximum Height Reached:

    • Kinematic relation between velocity, acceleration, and displacement:     v2=v02+2a(x−x0)v^2 = v_0^2 + 2 a (x - x_0)

    • Setting final velocity v=0 m/sv = 0\,\text{m/s} at peak height:     02=(20 m/s)2+2(−9.8 m/s2)xmax0^2 = (20\,\text{m/s})^2 + 2 (-9.8\,\text{m/s}^2) x_{max}     0=400+2(−9.8)xmax0 = 400 + 2(-9.8) x_{max}     19.6xmax=40019.6 x_{max} = 400     xmax=40019.6≈20.4 mx_{max} = \frac{400}{19.6} \approx 20.4\,\text{m}

  • Part (c) Solution - Elapsed Time at Height 15 m15\,\text{m}:

    • Kinematic position-time equation:     x=x0+v0t+12at2x = x_0 + v_0 t + \frac{1}{2} a t^2

    • Substituting x=15 mx = 15\,\text{m}, v0=20 m/sv_0 = 20\,\text{m/s}, and a=−9.8 m/s2a = -9.8\,\text{m/s}^2:     15=20t−4.9t215 = 20 t - 4.9 t^2     4.9t2−20t+15=04.9 t^2 - 20 t + 15 = 0

    • Solving the quadratic equation at2+bt+c=0a t^2 + b t + c = 0 with a=4.9a = 4.9, b=−20b = -20, c=15c = 15:     t=−b±b2−4ac2at = \frac{-b \pm \sqrt{b^2 - 4 a c}}{2 a}     t=20±(−20)2−4(4.9)(15)2(4.9)t = \frac{20 \pm \sqrt{(-20)^2 - 4(4.9)(15)}}{2(4.9)}     t=20±400−2949.8t = \frac{20 \pm \sqrt{400 - 294}}{9.8}     t=20±1069.8t = \frac{20 \pm \sqrt{106}}{9.8}

    • Evaluating both real roots:

    • First root (ascending path): t1=20−1069.8≈1.02 st_1 = \frac{20 - \sqrt{106}}{9.8} \approx 1.02\,\text{s}

    • Second root (descending path): t2=20+1069.8≈3.00 st_2 = \frac{20 + \sqrt{106}}{9.8} \approx 3.00\,\text{s}

Reaction Time and Hard Braking Kinematics

  • Problem Statement:

    • An automobile under hard braking loses speed at a rate of 7.0 m/s27.0\,\text{m/s}^2. Reaction time to engage brakes is 0.50 s0.50\,\text{s}. A school zone speed limit requires all cars to be able to stop in 4.0 m4.0\,\text{m}.

    • (a)(a) What maximum initial speed does this imply for an automobile in this zone?

    • (b)(b) What fraction of the 4.0 m4.0\,\text{m} distance is due to reaction time?

  • Given Parameters:

    • Deceleration rate during braking: a=−7.0 m/s2a = -7.0\,\text{m/s}^2

    • Reaction time before applying brakes: tr=0.50 st_r = 0.50\,\text{s}

    • Maximum stopping distance: dtotal=4.0 md_{total} = 4.0\,\text{m}

  • Part (a) Solution - Maximum Allowed Initial Speed v0v_0:

    • Reaction Distance (drd_r):

    • Distance traveled at constant velocity v0v_0 prior to brake application:       dr=v0×tr=0.50v0d_r = v_0 \times t_r = 0.50 v_0

    • Braking Distance (dbd_b):

    • Using kinematic equation v2=v02+2adbv^2 = v_0^2 + 2 a d_b with final velocity v=0 m/sv = 0\,\text{m/s}:       0=v02+2(−7.0)db0 = v_0^2 + 2(-7.0) d_b       14db=v0214 d_b = v_0^2       db=v0214d_b = \frac{v_0^2}{14}

    • Combined Stopping Distance Quadratic Equation:     dtotal=dr+dbd_{total} = d_r + d_b     0.50v0+v0214=4.00.50 v_0 + \frac{v_0^2}{14} = 4.0

    • Multiplying through by 1414 to convert to standard quadratic form:     v02+7v0−56=0v_0^2 + 7 v_0 - 56 = 0

    • Applying quadratic formula:     v0=−7+72−4(1)(−56)2(1)v_0 = \frac{-7 + \sqrt{7^2 - 4(1)(-56)}}{2(1)}     v0=−7+49+2242v_0 = \frac{-7 + \sqrt{49 + 224}}{2}     v0=−7+2732v_0 = \frac{-7 + \sqrt{273}}{2}     v0≈4.76 m/sv_0 \approx 4.76\,\text{m/s}

  • Part (b) Solution - Fraction of Distance Due to Reaction Time:

    • Calculating distance traveled during reaction period:     dr=v0×tr=4.76 m/s×0.50 s=2.38 md_r = v_0 \times t_r = 4.76\,\text{m/s} \times 0.50\,\text{s} = 2.38\,\text{m}

    • Computing fraction relative to total stopping distance of 4.0 m4.0\,\text{m}:     Fraction=drdtotal=2.38 m4.0 m=0.595\text{Fraction} = \frac{d_r}{d_{total}} = \frac{2.38\,\text{m}}{4.0\,\text{m}} = 0.595

    • Expressed as a percentage:     Percentage=59.5%\text{Percentage} = 59.5\%