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🎯⭐ INTERACTIVE LESSON

Particle Motion

Learn step-by-step with interactive practice!

Particle Motion - Complete Interactive Lesson

Part 1: Position, Velocity, Acceleration

Particle Motion

Part 1 of 7 — Position, Velocity, and Acceleration

Topic Overview

PartTopic
1Position, velocity, acceleration
2Speed & direction of motion
3Displacement vs. total distance
4Position from velocity (integration)
5Acceleration & velocity from integrals
6AP-style workshop
7Comprehensive assessment

The Motion Hierarchy

s(t)→derivativev(t)→derivativea(t)\boxed{s(t) \xrightarrow{\text{derivative}} v(t) \xrightarrow{\text{derivative}} a(t)} a(t)→integralv(t)→integrals(t)\boxed{a(t) \xrightarrow{\text{integral}} v(t) \xrightarrow{\text{integral}} s(t)}

FunctionSymbolRelationship
Positions(t)s(t) or x(t)x(t)Given or found by integrating vv
Velocityv(t)=s′(t)v(t) = s'(t)Derivative of position
Accelerationa(t)=v′(t)=s′′(t)a(t) = v'(t) = s''(t)Derivative of velocity

Worked Example

s(t)=t3−6t2+9t+2s(t) = t^3 - 6t^2 + 9t + 2. Find v(t)v(t) and a(t)a(t).

v(t)=s′(t)=3t2−12t+9=3(t−1)(t−3)v(t) = s'(t) = 3t^2 - 12t + 9 = 3(t-1)(t-3) a(t)=v′(t)=6t−12=6(t−2)a(t) = v'(t) = 6t - 12 = 6(t-2)

Key Fact: Velocity is signed (direction matters). Speed is ∣v(t)∣|v(t)| (always non-negative).

Practice — Finding v and a 🎯

Connect the concepts. 🔍

Calculate. ✍️

Key Takeaways — Part 1

  • v(t)=s′(t)v(t) = s'(t): velocity is the derivative of position
  • a(t)=v′(t)=s′′(t)a(t) = v'(t) = s''(t): acceleration is the derivative of velocity
  • At rest: v(t)=0v(t) = 0
  • Velocity has sign (direction); speed is ∣v(t)∣|v(t)|

Part 2: Displacement vs Total Distance

Particle Motion

Part 2 of 7 — Speed & Direction of Motion

Speed vs. Velocity

Speed=∣v(t)∣\boxed{\text{Speed} = |v(t)|}

ConceptFormulaAlways positive?
Velocityv(t)=s′(t)v(t) = s'(t)No (has sign)
Speed$v(t)

Direction of Motion

v(t)v(t)DirectionMeaning
v(t)>0v(t) > 0Moving right (or up)Position increasing
v(t)<0v(t) < 0Moving left (or down)Position decreasing
v(t)=0v(t) = 0At restPossibly changing direction

Speeding Up vs. Slowing Down

Speeding up: v and a have the SAME sign\boxed{\text{Speeding up: } v \text{ and } a \text{ have the SAME sign}} Slowing down: v and a have OPPOSITE signs\boxed{\text{Slowing down: } v \text{ and } a \text{ have OPPOSITE signs}}

v(t)v(t)a(t)a(t)Speed is...
++++Increasing
−-−-Increasing
++−-Decreasing
−-++Decreasing

Worked Example

s(t)=t3−6t2+9ts(t) = t^3 - 6t^2 + 9t. When is the particle speeding up on [0,4][0, 4]?

v(t)=3(t−1)(t−3)v(t) = 3(t-1)(t-3), a(t)=6(t−2)a(t) = 6(t-2)

  • v>0v > 0 on (0,1)(0,1) and (3,4)(3,4); v<0v < 0 on (1,3)(1,3)
  • a>0a > 0 on (2,4)(2,4); a<0a < 0 on (0,2)(0,2)

Same sign: (1,2)(1,2) (both negative) and (3,4)(3,4) (both positive).

Speeding up on (1,2)∪(3,4)(1, 2) \cup (3, 4).

Practice — Speed & Direction 🎯

Classify the motion. 🔍

Find the speed. ✍️

Key Takeaways — Part 2

  • Speed =∣v(t)∣= |v(t)|, always non-negative
  • v>0v > 0: right/up; v<0v < 0: left/down
  • Speeding up: vv and aa same sign
  • Slowing down: vv and aa opposite signs
  • Direction change: v(t)v(t) changes sign

Part 3: Speed and Speeding Up/Slowing Down

Particle Motion

Part 3 of 7 — Displacement vs. Total Distance

Two Different Quantities

Displacement=∫abv(t) dt=s(b)−s(a)\boxed{\text{Displacement} = \int_a^b v(t)\,dt = s(b) - s(a)}

Total Distance=∫ab∣v(t)∣ dt\boxed{\text{Total Distance} = \int_a^b |v(t)|\,dt}

QuantityFormulaSignMeaning
Displacement∫abv(t) dt\int_a^b v(t)\,dtCan be negativeNet change in position
Total distance$\int_a^bv(t),dt$

Worked Example

v(t)=t2−4v(t) = t^2 - 4 on [0,3][0, 3]. Find displacement and total distance.

Displacement: ∫03(t2−4) dt=[t33−4t]03=(9−12)−0=−3\int_0^3 (t^2-4)\,dt = \left[\frac{t^3}{3}-4t\right]_0^3 = (9-12) - 0 = -3

Total distance: v(t)=0v(t) = 0 at t=2t = 2. Split at t=2t = 2: ∫02∣t2−4∣ dt+∫23∣t2−4∣ dt=∫02(4−t2) dt+∫23(t2−4) dt\int_0^2 |t^2-4|\,dt + \int_2^3 |t^2-4|\,dt = \int_0^2 (4-t^2)\,dt + \int_2^3 (t^2-4)\,dt =[4t−t33]02+[t33−4t]23=163+73=233= \left[4t - \frac{t^3}{3}\right]_0^2 + \left[\frac{t^3}{3} - 4t\right]_2^3 = \frac{16}{3} + \frac{7}{3} = \frac{23}{3}

AP Tip: Displacement can be negative (particle ends left of start). Total distance is always positive. AP loves asking for both in the same problem.

Practice — Displacement & Distance 🎯

Distinguish displacement and distance. 🔍

Calculate total distance. ✍️

Key Takeaways — Part 3

  • Displacement =∫abv(t) dt= \int_a^b v(t)\,dt (net change, can be negative)
  • Total distance =∫ab∣v(t)∣ dt= \int_a^b |v(t)|\,dt (always positive)
  • Split the integral at points where v(t)=0v(t) = 0
  • Displacement =0= 0 means the particle returned to start

Part 4: Position from Velocity

Particle Motion

Part 4 of 7 — Position from Velocity (Integration)

Finding Position from Velocity

s(t)=s(t0)+∫t0tv(τ) dτ\boxed{s(t) = s(t_0) + \int_{t_0}^{t} v(\tau)\,d\tau}

This combines the initial condition s(t0)s(t_0) with the displacement ∫v dt\int v\,dt.

Worked Example

v(t)=3t2−2v(t) = 3t^2 - 2 and s(0)=5s(0) = 5. Find s(t)s(t).

s(t)=s(0)+∫0t(3τ2−2) dτ=5+[τ3−2τ]0t=5+t3−2ts(t) = s(0) + \int_0^t (3\tau^2 - 2)\,d\tau = 5 + [\tau^3 - 2\tau]_0^t = 5 + t^3 - 2t

s(t)=t3−2t+5\boxed{s(t) = t^3 - 2t + 5}

Position at a Specific Time

v(t)=6t−4v(t) = 6t - 4, s(1)=3s(1) = 3. Find s(4)s(4).

s(4)=s(1)+∫14(6t−4) dt=3+[3t2−4t]14s(4) = s(1) + \int_1^4 (6t-4)\,dt = 3 + [3t^2 - 4t]_1^4 =3+(48−16)−(3−4)=3+32+1=36= 3 + (48-16) - (3-4) = 3 + 32 + 1 = 36

Key Fact: You don't need to find s(t)s(t) as a formula — just compute the definite integral and add the initial position.

Practice — Position from Velocity 🎯

Build the position function. 🔍

Find position. ✍️

Key Takeaways — Part 4

  • s(t)=s(t0)+∫t0tv(τ) dτs(t) = s(t_0) + \int_{t_0}^t v(\tau)\,d\tau
  • Initial condition + displacement gives position
  • You can find ss at a specific time without finding s(t)s(t) as a formula
  • AP FRQs often give v(t)v(t) and initial position, ask for ss at another time

Part 5: Velocity from Acceleration

Particle Motion

Part 5 of 7 — Acceleration & Velocity from Integrals

Finding Velocity from Acceleration

v(t)=v(t0)+∫t0ta(τ) dτ\boxed{v(t) = v(t_0) + \int_{t_0}^{t} a(\tau)\,d\tau}

Full Chain: a→v→sa \to v \to s

GivenTo FindFormula
a(t)a(t) and v(t0)v(t_0)v(t)v(t)v(t0)+∫t0ta dτv(t_0) + \int_{t_0}^t a\,d\tau
v(t)v(t) and s(t0)s(t_0)s(t)s(t)s(t0)+∫t0tv dτs(t_0) + \int_{t_0}^t v\,d\tau
a(t)a(t), v(t0)v(t_0), s(t0)s(t_0)s(t)s(t)Integrate twice

Worked Example

a(t)=6ta(t) = 6t, v(0)=−4v(0) = -4, s(0)=1s(0) = 1. Find s(t)s(t).

Step 1: v(t)=−4+∫0t6τ dτ=−4+3t2v(t) = -4 + \int_0^t 6\tau\,d\tau = -4 + 3t^2

Step 2: s(t)=1+∫0t(−4+3τ2) dτ=1−4t+t3s(t) = 1 + \int_0^t (-4 + 3\tau^2)\,d\tau = 1 - 4t + t^3

s(t)=t3−4t+1\boxed{s(t) = t^3 - 4t + 1}

When Does the Particle Change Direction?

v(t)=3t2−4=0v(t) = 3t^2 - 4 = 0 at t=2/3t = 2/\sqrt{3}. Check sign change: v(0)=−4<0v(0) = -4 < 0, v(2)=8>0v(2) = 8 > 0. Direction changes at t=2/3t = 2/\sqrt{3}.

Practice — Integration 🎯

Build from acceleration. 🔍

Find velocity. ✍️

Key Takeaways — Part 5

  • v(t)=v(t0)+∫t0ta dτv(t) = v(t_0) + \int_{t_0}^t a\,d\tau
  • Integrate twice to go from aa to ss
  • Each integration adds a constant (initial condition)
  • Direction changes when v(t)v(t) changes sign

Part 6: AP-Style Workshop

Particle Motion

Part 6 of 7 — AP-Style Free-Response Workshop

AP FRQ Patterns for Particle Motion

PartTypical PromptKey Setup
(a)"When is the particle at rest?"Solve v(t)=0v(t) = 0
(b)"Find total distance on [a,b][a,b]"$\int_a^b
(c)"Is speed increasing or decreasing at t=kt = k?"Compare signs of v(k)v(k) and a(k)a(k)
(d)"Find position at time t=Tt = T"s(T)=s(t0)+∫t0Tv dts(T) = s(t_0) + \int_{t_0}^T v\,dt

AP Tip: In table-based problems, use the given values with Riemann sums or trapezoidal approximations.


Complete Worked FRQ

A particle moves along the xx-axis with velocity v(t)=t2−5t+4v(t) = t^2 - 5t + 4 for t≥0t \ge 0 and position s(0)=2s(0) = 2.

(a) When is the particle at rest?

v(t)=t2−5t+4=(t−1)(t−4)=0v(t) = t^2 - 5t + 4 = (t-1)(t-4) = 0 at t=1t = 1 and t=4t = 4.

(b) Total distance traveled on [0,6][0,6]

Sign analysis: v>0v > 0 on [0,1)[0,1), v<0v < 0 on (1,4)(1,4), v>0v > 0 on (4,6](4,6].

∫01(t2−5t+4) dt=[t33−5t22+4t]01=13−52+4=116\int_0^1 (t^2-5t+4)\,dt = \left[\frac{t^3}{3} - \frac{5t^2}{2} + 4t\right]_0^1 = \frac{1}{3} - \frac{5}{2} + 4 = \frac{11}{6}

∫14(t2−5t+4) dt=[t33−5t22+4t]14=(643−40+16)−(13−52+4)\int_1^4 (t^2-5t+4)\,dt = \left[\frac{t^3}{3} - \frac{5t^2}{2} + 4t\right]_1^4 = \left(\frac{64}{3} - 40 + 16\right) - \left(\frac{1}{3} - \frac{5}{2} + 4\right)

=643−24−116=1286−1446−116=−276=−92= \frac{64}{3} - 24 - \frac{11}{6} = \frac{128}{6} - \frac{144}{6} - \frac{11}{6} = -\frac{27}{6} = -\frac{9}{2}

∫46(t2−5t+4) dt=[t33−5t22+4t]46=(72−90+24)−(643−40+16)\int_4^6 (t^2-5t+4)\,dt = \left[\frac{t^3}{3} - \frac{5t^2}{2} + 4t\right]_4^6 = \left(72 - 90 + 24\right) - \left(\frac{64}{3} - 40 + 16\right)

=6−643+24=30−643=263= 6 - \frac{64}{3} + 24 = 30 - \frac{64}{3} = \frac{26}{3}

Total distance=116+92+263=116+276+526=906=15\text{Total distance} = \frac{11}{6} + \frac{9}{2} + \frac{26}{3} = \frac{11}{6} + \frac{27}{6} + \frac{52}{6} = \frac{90}{6} = 15

(c) Is speed increasing or decreasing at t=3t = 3?

v(3)=9−15+4=−2<0v(3) = 9 - 15 + 4 = -2 < 0 and a(3)=2(3)−5=1>0a(3) = 2(3) - 5 = 1 > 0

Opposite signs ⇒\Rightarrow speed is decreasing at t=3t = 3.

(d) Find s(6)s(6).

s(6)=2+∫06(t2−5t+4) dt=2+[t33−5t22+4t]06=2+72−90+24=8s(6) = 2 + \int_0^6 (t^2-5t+4)\,dt = 2 + \left[\frac{t^3}{3} - \frac{5t^2}{2} + 4t\right]_0^6 = 2 + 72 - 90 + 24 = 8

AP-style questions. 🎯

Analyze motion. 🔍

AP FRQ practice. ✍️

Key Takeaways — Part 6

  • AP FRQs test all aspects: rest, direction, distance, position
  • Always split integrals at v(t)=0v(t) = 0 for total distance
  • Speed increasing   ⟺  \iff vv and aa same sign
  • Show every step and justify sign changes for full credit

Part 7: Final Assessment

Particle Motion

Part 7 of 7 — Comprehensive Assessment

Formula Reference

RelationshipFormulaNotes
Velocity from positionv(t)=s′(t)v(t) = s'(t)Derivative
Acceleration from velocitya(t)=v′(t)=s′′(t)a(t) = v'(t) = s''(t)Second derivative
Position from velocitys(t)=s(t0)+∫t0tv dτs(t) = s(t_0) + \int_{t_0}^t v\,d\tauRequires initial condition
Velocity from accelerationv(t)=v(t0)+∫t0ta dτv(t) = v(t_0) + \int_{t_0}^t a\,d\tauRequires initial condition
Displacement∫abv(t) dt\int_a^b v(t)\,dtSigned (can be negative)
Total distance$\int_a^bv(t)
Speed$v(t)

Common AP Mistakes

MistakeCorrection
Confusing displacement with total distanceDisplacement is signed; total distance splits at v=0v = 0
Forgetting to check sign of vv for directionAlways state direction (left/right or positive/negative)
Using a>0a > 0 means "speeding up"Speed increases only when vv and aa have the same sign
Missing initial conditionsEvery antiderivative needs +C+C or initial value
Not justifying sign changesAP requires explicit sign analysis for direction change

Assessment — Set 1 🎯

Assessment — Set 2 🎯

Complete the analysis. 🔍

Final challenge. ✍️

Particle Motion — Complete! 🎓

PartTopicStatus
1Position, Velocity & Acceleration✅
2Speed & Direction of Motion✅
3Displacement vs. Total Distance✅
4Position from Velocity✅
5Acceleration & Velocity from Integrals✅
6AP-Style Free-Response Workshop✅
7Comprehensive Assessment✅

You have completed the full Particle Motion unit. You should now be confident with all AP Calculus AB particle motion problems!