Chapter 2 Notes: Motion Along a Straight Line

2-1 Position, Displacement, and Average Velocity

  • Physics focus: motion of objects moving along a single axis; treat such objects as point-like particles if all parts move in the same direction and rate.

  • Position along an axis: the location x read on a scaled axis (e.g., x-axis).

  • Sign convention on an axis:

    • Positive direction: increasing coordinates (to the right in the figure).

    • Negative direction: decreasing coordinates (to the left).

  • Displacement Δx:

    • Definition: change in position when moving from x1 to x2 in time interval Δt = t2 − t1.

    • Vector quantity with sign; Δx > 0 if motion is in the positive direction, Δx < 0 if in the negative direction.

    • Formula: Δx=x<em>2x</em>1\Delta x = x<em>2 - x</em>1

    • Example: moving from x1 = 5 m to x2 = 12 m → Δx=12m5m=+7m\Delta x = 12\,\text{m} - 5\,\text{m} = +7\,\text{m}; from x1 = 5 m to x2 = 1 m → Δx=1m5m=4m\Delta x = 1\,\text{m} - 5\,\text{m} = -4\,\text{m}

    • The final displacement may be zero even if the path covers distance (e.g., 5 m → 200 m → 5 m gives Δx = 0).

    • Displacement is a vector quantity with magnitude and direction; magnitude is the straight-line distance between initial and final positions.

  • Average velocity v_avg over interval Δt:

    • Definition: ratio of displacement to time interval.

    • Formula: v<em>avg=ΔxΔt=x</em>2x<em>1t</em>2t1v<em>{\text{avg}} = \frac{\Delta x}{\Delta t} = \frac{x</em>2 - x<em>1}{t</em>2 - t_1}

    • Sign of v_avg matches the direction of motion (positive if moving in +x, negative if in -x).

    • On a graph of x versus t, v_avg is the slope of the straight line joining the points (x1, t1) and (x2, t2).

  • Average speed s_avg over Δt:

    • Definition: total distance traveled divided by the time interval.

    • Formula: savg=distance traveled in the intervalΔt\text{s}_{\text{avg}} = \frac{\text{distance traveled in the interval}}{\Delta t}

    • Unlike v_avg, savg has no sign (it is a nonnegative quantity).

  • Relationship to everyday physics: study of how fast and how far objects move; real-world relevance spans NASCAR, geology, medicine, and transportation safety.

  • One-dimensional motion: motion along a straight line (vertical, horizontal, or slanted).

  • Checkpoint 1 (quick reasoning): Given three initial/final positions, determine which yield a negative displacement.

    • Pairs: (a) −3 m → +5 m; (b) −3 m → −7 m; (c) 7 m → −3 m

    • Answers: (b) Δx = (−7) − (−3) = −4 m; (c) Δx = (−3) − 7 = −10 m; thus (b) and (c) have negative displacement.

2-2 Instantaneous Velocity and Speed

  • Instantaneous velocity v at time t: rate at which position x changes at that exact time.

  • Definition via calculus: v(t) = \frac{dx}{dt} (the slope of the x(t) curve at time t).

  • Speed: the magnitude of velocity; speed=v\text{speed} = |v|; speed has no direction.

  • Instantaneous velocity vs average velocity:

    • Average velocity is over a finite interval; instantaneous velocity is limit as the interval shrinks to zero.

    • Graphically, on an x vs t plot, the slope at a single time t gives v(t).

  • Key relation: velocity is a vector quantity and has both magnitude and direction.

  • Example intuition: a stationary object has v = 0 → slope of x(t) is zero at that time.

  • Elevator-cab illustration (conceptual): x(t) curve for motion along an axis; slope of x(t) yields v(t); slope of v(t) yields a(t) (see Fig. 2-6 in the module).

2-3 Acceleration

  • Average acceleration a_avg over a time interval Δt:

    • Definition: change in velocity divided by the time over which the change occurs.

    • Formula: a<em>avg=ΔvΔt=v</em>2v<em>1t</em>2t1a<em>{\text{avg}} = \frac{\Delta v}{\Delta t} = \frac{v</em>2 - v<em>1}{t</em>2 - t_1}

    • Sign indicates the acceleration's direction along the axis.

  • Instantaneous acceleration a(t):

    • Definition: derivative of velocity with respect to time, or second derivative of position.

    • Formulas: a(t)=dvdt=d2xdt2a(t) = \frac{dv}{dt} = \frac{d^2 x}{dt^2}

  • On a graph of velocity versus time (v vs t), the acceleration at time t is the slope of the v(t) curve at that time.

  • Units: [acceleration]=m s2\text{[acceleration]} = \text{m s}^{-2} (often written as m/s^2).

  • Vector nature of acceleration: has magnitude and direction; positive a means acceleration in +x, negative a in −x.

  • Elevator example (qualitative):

    • When v is constant, a = 0.

    • During acceleration, v increases in the positive direction (a > 0) if moving in +x.

    • When decelerating, magnitude of a may be larger even if time to stop is shorter (steeper slope on v(t) during braking).

  • Practical interpretation: signs indicate direction; if velocity and acceleration have the same sign, speed increases; if opposite signs, speed decreases.

  • Common cues: large accelerations (e.g., up to 3g on roller coasters) can be described in g-units, where g ≈ 9.8 m/s^2.

Quick checkpoints and concepts

  • Checkpoint 2: Given four position-time equations, identify where velocity is constant and where velocity is negative.

    • Equations (examples):

    • (1) x=3t2x = 3t - 2 → v(t) = 3 (constant, positive)

    • (2) x=4t22x = -4t^2 - 2 → v(t) = -8t (not constant)

    • (3) x=2t2x = \frac{2}{t^2} → v(t) = -\frac{4}{t^3} (not constant)

    • (4) x=2x = -2 → v(t) = 0 (constant, zero velocity)

    • Negative velocity occurs for (2) at t > 0 and for (3) at t > 0.

  • Checkpoint 3: Interpreting velocity and acceleration signs: if velocity and acceleration have the same sign, speed increases; if opposite signs, speed decreases.

Sample Problems

  • Sample Problem 2.01: Average velocity, beat-up pickup truck

    • The journey: 8.4 km at 70 km/h, then 2.0 km walking to a gas station.

    • (a) Displacement from start to station:

    • Treat first position x1 = 0 and final x2 = 8.4 km + 2.0 km = 10.4 km.

    • Δx=x<em>2x</em>1=10.4 km\Delta x = x<em>2 - x</em>1 = 10.4\ \text{km}

    • Answer: Δx=10.4 km\Delta x = 10.4\ \text{km} (positive direction).

    • (b) Time interval for driving to the station:

    • Driving displacement Δxdr = 8.4 km; vavg,dr = 70 km/h.

    • a)Δt<em>dr=Δx</em>drvavg,dr=8.4 km70 km/h=0.12 ha) \Delta t<em>{dr} = \frac{\Delta x</em>{dr}}{v_{avg,dr}} = \frac{8.4\ \text{km}}{70\ \text{km/h}} = 0.12\ \text{h}

    • (c) Average velocity v_avg for the entire trip (start to station):

    • Total displacement Δxtotal = 10.4 km; total time Δttotal = 0.12 h + 0.50 h = 0.62 h.

    • v<em>avg=Δx</em>totalΔttotal=10.4 km0.62 h16.8 km/hv<em>{avg} = \frac{\Delta x</em>{total}}{\Delta t_{total}} = \frac{10.4\ \text{km}}{0.62\ \text{h}} \approx 16.8\ \text{km/h}

    • Graphical check: slope from origin to the Station on the x(t) plot gives the same value, vavg=16.8 km/hv_{avg} = 16.8\ \text{km/h}.

    • (d) If you spend 45 minutes pumping gas and walking back to the truck, find the average speed for the entire trip (start to return):

    • Total distance: 8.4 + 2.0 + 2.0 = 12.4 km.

    • Total time: 0.12 h + 0.50 h + 0.75 h = 1.37 h.

    • savg=distancetime=12.4 km1.37 h9.0 km/h\text{s}_{avg} = \frac{\text{distance}}{\text{time}} = \frac{12.4\ \text{km}}{1.37\ \text{h}} \approx 9.0\ \text{km/h}

  • Sample Problem 2.02: Velocity and slope of x versus t, elevator cab

    • Given x(t) for an elevator cab, plot v(t) as the slope of x(t).

    • Key takeaway: velocity is the slope of the x(t) curve; a(t) is the slope of the v(t) curve (i.e., the derivative of velocity).

  • Sample Problem 2.03: Acceleration and dv/dt

    • Provided an x(t) on the x-axis; (a) find v(t) = dx/dt and a(t) = dv/dt.

    • (b) Determine if/when v = 0.

    • (c) Describe the motion for t ≥ 0 using x(t), v(t), a(t).

    • General method: differentiate x(t) to get v(t); differentiate v(t) to get a(t); analyze signs and zeros to understand motion.

How to connect the concepts

  • From position to velocity:

    • v(t) is the slope of x(t) at time t: v(t)=dxdtv(t) = \frac{dx}{dt}.

  • From velocity to acceleration:

    • a(t) is the slope of v(t) at time t, or the second derivative of position: a(t)=dvdt=d2xdt2a(t) = \frac{dv}{dt} = \frac{d^2 x}{dt^2}.

  • From velocity to displacement:

    • Displacement over a time interval is the integral of velocity: approximately the area under the v(t) curve between t1 and t2; for constant v, Δx = v × Δt; for variable v, Δx = ∫_{t1}^{t2} v(t) dt.

Foundational notes and signs

  • Sign conventions:

    • Positive velocity or acceleration indicates motion or change in the positive x direction.

    • If velocity and acceleration share the same sign, speed increases; if signs are opposite, speed decreases.

  • Units recap:

    • Position: meters (m)

    • Velocity: meters per second (m/s)

    • Acceleration: meters per second squared (m/s^2)

  • Practical context: a few examples show why these concepts matter in real life, from race cars to earthquakes to medical diagnostics and everyday driving.

Summary of key formulas (LaTeX)

  • Displacement: Δx=x<em>2x</em>1\Delta x = x<em>2 - x</em>1

  • Average velocity: v<em>avg=ΔxΔt=x</em>2x<em>1t</em>2t1v<em>{\text{avg}} = \frac{\Delta x}{\Delta t} = \frac{x</em>2 - x<em>1}{t</em>2 - t_1}

  • Average speed: savg=distance traveledΔt\text{s}_{\text{avg}} = \frac{\text{distance traveled}}{\Delta t}

  • Instantaneous velocity: v(t)=dxdtv(t) = \frac{dx}{dt}

  • Acceleration (average): a<em>avg=ΔvΔt=v</em>2v<em>1t</em>2t1a<em>{\text{avg}} = \frac{\Delta v}{\Delta t} = \frac{v</em>2 - v<em>1}{t</em>2 - t_1}

  • Acceleration (instantaneous) and position relations: a(t)=dvdt=d2xdt2a(t) = \frac{dv}{dt} = \frac{d^2 x}{dt^2}

  • Sign interpretation rule: if sgn(v) = sgn(a) then speed is increasing; if sgn(v) ≠ sgn(a) then speed is decreasing.