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Lesson 68 — Kinematics: Position, Velocity, and Acceleration

Successive derivatives of position yield velocity, acceleration, and jerk. Uniform motion, uniformly accelerated motion, simple harmonic motion, and air resistance with calculus rigor.

Used in: Math III — Japan (applications of derivatives: rate of change) · Leistungskurs Mathematik — Germany Grade 12 (Differentialrechnung: Weg, Geschwindigkeit, Beschleunigung) · H2 Mathematics — Singapore (applications of differentiation: rates of change) · AP Calculus AB/BC — USA (FUN-4: using derivatives to analyze motion)

v(t)=s(t),a(t)=v(t)=s(t),j(t)=a(t)=s(t)v(t) = s'(t), \quad a(t) = v'(t) = s''(t), \quad j(t) = a'(t) = s'''(t)
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Rigorous notation, full derivation, hypotheses

Kinematics via Differential Calculus

Fundamental Definitions

"The instantaneous velocity of an object is the limit of the average velocities of the object over shorter and shorter time intervals." — Active Calculus §1.1

"The position function s(t)s(t) gives the position of an object along a number line at time tt. The velocity function v(t)=s(t)v(t) = s'(t) gives the velocity of the object at time tt." — OpenStax Calculus Vol.1 §3.4

Standard Motion Cases

Motions(t)s(t)v(t)v(t)a(t)a(t)Observation
Rests0s_00000fixed point
Uniform (MRU)s0+v0ts_0 + v_0 tv0v_000straight line on s×ts \times t graph
Uniformly Accelerated (MUV)s0+v0t+12a0t2s_0 + v_0 t + \tfrac{1}{2}a_0 t^2v0+a0tv_0 + a_0 ta0a_0parabola
Simple Harmonic (MHS)Acos(ωt+ϕ)A\cos(\omega t + \phi)Aωsin(ωt+ϕ)-A\omega\sin(\omega t + \phi)Aω2cos(ωt+ϕ)-A\omega^2\cos(\omega t + \phi)a=ω2sa = -\omega^2 s
With Air ResistanceODE solutionv(1ekt/m)v_\infty(1-e^{-kt/m})decays to 0terminal velocity

Torricelli's Theorem (derivation via calculus)

Simple Harmonic Motion (SHM)

x(t)=Acos(ωt+ϕ)x(t) = A\cos(\omega t + \phi) satisfies the ODE x¨+ω2x=0\ddot x + \omega^2 x = 0.

  • Period: T=2π/ωT = 2\pi/\omega.
  • Frequency: f=1/Tf = 1/T.
  • For a spring: ω=k/m\omega = \sqrt{k/m}; for a pendulum (small oscillations): ω=g/L\omega = \sqrt{g/L}.

Figure: Graphs of ss, vv, aa for SHM

ts(t)A cos(ωt)tv(t)-Aω sin(ωt)ta(t)-Aω² cos(ωt)Phase shift: s and v separated by 90°; s and a separated by 180° (opposite)

Kinematics in Rn\mathbb{R}^n

For r(t)=(x(t),y(t),z(t))R3\vec{r}(t) = (x(t), y(t), z(t)) \in \mathbb{R}^3:

v(t)=r˙(t),a(t)=r¨(t),v=speed.\vec{v}(t) = \dot{\vec{r}}(t), \qquad \vec{a}(t) = \ddot{\vec{r}}(t), \qquad |\vec{v}| = \text{speed}.

Each component is differentiated independently. Centripetal acceleration in curved trajectory: ac=v2/ρa_c = v^2/\rho (where ρ\rho is the radius of curvature).

Solved Examples

Exercise list

40 exercises · 10 with worked solution (25%)

12 21 3 2 2
  1. Ex. 68.1

    s(t)=2t26ts(t) = 2t^2 - 6t. Calculate v(t)v(t) and a(t)a(t).

  2. Ex. 68.2

    s(t)=t36t2+9ts(t) = t^3 - 6t^2 + 9t. When is v=0v = 0? At each instant, is the object accelerating or braking?

  3. Ex. 68.3

    s(t)=1005t2s(t) = 100 - 5t^2 (free fall, g=10g = 10 m/s²). When does it hit the ground? Velocity at that instant.

  4. Ex. 68.4Answer key

    s(t)=5t+32t2+12t3s(t) = 5t + \frac{3}{2}t^2 + \frac{1}{2}t^3. Velocity and acceleration at t=2t = 2.

  5. Ex. 68.5

    s(t)=etsints(t) = e^{-t}\sin t. Calculate v(t)v(t) and a(t)a(t). What does the decaying amplitude reveal?

  6. Ex. 68.6

    s(t)=10sin(2t)s(t) = 10\sin(2t). Identify AA, ω\omega, and the period TT. Write v(t)v(t).

  7. Ex. 68.7

    s(t)=t44t3+6t2s(t) = t^4 - 4t^3 + 6t^2. Maximum velocity on [0,3][0, 3].

  8. Ex. 68.8

    s(t)=ln(1+t2)s(t) = \ln(1 + t^2). Calculate v(t)v(t) and evaluate at t=1t = 1.

  9. Ex. 68.9Answer key

    s(t)=t24ts(t) = t^2 - 4t. Distance traveled between t=0t = 0 and t=4t = 4 (note: vv changes sign).

  10. Ex. 68.10

    s(t)=Acos(ωt)s(t) = A\cos(\omega t). Calculate the jerk j(t)=s(t)j(t) = s'''(t).

  11. Ex. 68.11

    s(t)=2t36t+1s(t) = 2t^3 - 6t + 1. When is velocity zero? Is there a change in direction?

  12. Ex. 68.12

    s(t)=sin(t2)s(t) = \sin(t^2). Calculate v(t)v(t) (chain rule) and evaluate at t=πt = \sqrt{\pi}.

  13. Ex. 68.13

    A ball is thrown upward from the ground with v0=20v_0 = 20 m/s. Maximum height (g=10g = 10 m/s²).

  14. Ex. 68.14

    A car at v0=30v_0 = 30 m/s brakes uniformly with a=5a = -5 m/s². Stopping distance (Torricelli's Theorem).

  15. Ex. 68.15Answer key

    An airplane starts from rest and takes off at vf=80v_f = 80 m/s after a runway of 10001000 m. Average acceleration and takeoff time.

  16. Ex. 68.16

    A stone falls from h=80h = 80 m. Time to fall and speed at impact (g=10g = 10 m/s²).

  17. Ex. 68.17Answer key

    A car accelerates from 0-100 km/h in 10.510.5 s. Average acceleration and distance traveled during acceleration.

  18. Ex. 68.18

    Projectile motion: v0=50v_0 = 50 m/s at 30°30° to the horizontal. Horizontal range (g=10g = 10 m/s²).

  19. Ex. 68.19

    Rocket: a(t)=300.5ta(t) = 30 - 0.5t m/s² until t=60t = 60 s (engine cutoff). Velocity and position at engine cutoff.

  20. Ex. 68.20

    A train brakes uniformly, traveling 200200 m in 2020 s and stopping. What was its initial v0v_0?

  21. Ex. 68.21

    A ball is thrown from the top of a 5050 m tower with v0=20v_0 = 20 m/s upwards. Time until it hits the ground.

  22. Ex. 68.22

    An object of m=1m = 1 kg falls with drag b=0.2b = 0.2 kg/s. Terminal velocity (g=10g = 10 m/s²).

  23. Ex. 68.23

    Mass-spring system: m=1m = 1 kg, k=100k = 100 N/m. Angular frequency ω\omega, period TT, and frequency ff.

  24. Ex. 68.24

    x(t)=0.1cos(2πt)x(t) = 0.1\cos(2\pi t). Amplitude, period, v(t)v(t), and maximum velocity.

  25. Ex. 68.25

    Pendulum of length L=1L = 1 m. Angular frequency ω=g/L\omega = \sqrt{g/L} and period (g=10g = 10 m/s²).

  26. Ex. 68.26

    Verify that x(t)=Acos(ωt+ϕ)x(t) = A\cos(\omega t + \phi) satisfies the ODE x¨+ω2x=0\ddot{x} + \omega^2 x = 0.

  27. Ex. 68.27

    SHM: E=12mx˙2+12kx2E = \frac{1}{2}m\dot{x}^2 + \frac{1}{2}kx^2. Show that EE is constant by differentiating with respect to time.

  28. Ex. 68.28Answer key

    x(t)=etcos(5t)x(t) = e^{-t}\cos(5t) (damped oscillator). Apparent frequency and behavior of the amplitude.

  29. Ex. 68.29

    Phase relationship between x(t)=Acos(ωt+ϕ)x(t) = A\cos(\omega t + \phi) and v(t)v(t). Confirm 90°90°.

  30. Ex. 68.30Answer key

    Show that a(t)a(t) and x(t)x(t) are 180°180° out of phase in SHM — i.e., a=ω2xa = -\omega^2 x.

  31. Ex. 68.31

    A ball is thrown upward. At its highest point, the acceleration is:

  32. Ex. 68.32Answer key

    Explain why average velocity (Δs/Δt\Delta s/\Delta t) \neq average of velocities in general. Give a numerical example.

  33. Ex. 68.33

    Explain the difference between velocity (1D vector quantity with sign) and speed (scalar). Why is v<0v < 0 possible?

  34. Ex. 68.34

    Circular motion: r=R(cosωt,sinωt)\vec{r} = R(\cos\omega t, \sin\omega t). Show that a=ω2r\vec{a} = -\omega^2\vec{r} and a=Rω2|\vec{a}| = R\omega^2.

  35. Ex. 68.35

    Projectile motion launched with v0v_0 and angle θ\theta. Derive the range formula R=v02sin(2θ)/gR = v_0^2\sin(2\theta)/g and the optimal angle.

  36. Ex. 68.36Answer key

    Car travels at 60 km/h for 1 hour, then at 120 km/h for 1 hour. Average velocity by time? Average velocity over equal distances traveled?

  37. Ex. 68.37Answer key

    Quadratic drag: mv˙=mgbv2m\dot{v} = -mg - bv^2. Terminal velocity and analytical solution for v(t)v(t) (via separation of variables).

  38. Ex. 68.38Answer key

    Helix: r(t)=(Rcosωt,Rsinωt,vt)\vec{r}(t) = (R\cos\omega t, R\sin\omega t, vt). Calculate v\vec{v}, v|\vec{v}|, and a\vec{a}.

  39. Ex. 68.39

    Derive Torricelli's equation vf2=v02+2aΔsv_f^2 = v_0^2 + 2a\,\Delta s from the UAM equations by eliminating time tt.

  40. Ex. 68.40

    Show that in SHM, the time-averaged kinetic and potential energies are each E/2E/2 — using sin2=cos2=1/2\langle\sin^2\rangle = \langle\cos^2\rangle = 1/2.

Sources

  • Active Calculus — Matt Boelkins et al. · 2024 · §1.1–§1.5 Measuring Velocity and Interpreting Derivatives · CC-BY-NC-SA. Primary source.
  • Calculus Volume 1 — OpenStax · 2016 · §3.4 Derivatives as Rates of Change · CC-BY-NC-SA.
  • APEX Calculus — Hartman, Heinold, Siemers, Chalishajar · 2023 · §2.4 Velocity and Position · CC-BY-NC.
  • Nobel Prize in Physics 1921 (Einstein) — Relativity and the formulation of spacetime as the backdrop for modern kinematics.

Updated on 2024-05-15 · Author(s): Clube da Matemática

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