๐ŸŽฏโญ INTERACTIVE LESSON

Particle Motion

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Particle Motion - Complete Interactive Lesson

Part 1: Position & Velocity

Particle Motion

Part 1 of 7 โ€” Position, Velocity, Acceleration

The Relationships

FunctionSymbolRelationship
Positions(t)s(t)Given or found by integrating vv
Velocityv(t)v(t)v(t)=sโ€ฒ(t)v(t) = s'(t)
Accelerationa(t)a(t)a(t)=vโ€ฒ(t)=sโ€ฒโ€ฒ(t)a(t) = v'(t) = s''(t)

Key Interpretations

  • Speed =โˆฃv(t)โˆฃ= |v(t)| (always positive)
  • Particle moves right when v(t)>0v(t) > 0
  • Particle moves left when v(t)<0v(t) < 0
  • Particle speeds up when vv and aa have the same sign
  • Particle slows down when vv and aa have opposite signs

Position, Velocity, Acceleration ๐ŸŽฏ

A particle moves along a line with s(t)=t3โˆ’6t2+9t+1s(t) = t^3 - 6t^2 + 9t + 1.

Key Takeaways โ€” Part 1

  1. Differentiate position to get velocity, differentiate again for acceleration
  2. "At rest" means v(t)=0v(t) = 0
  3. Direction of motion determined by sign of v(t)v(t)

Part 2: Velocity & Acceleration

Particle Motion

Part 2 of 7 โ€” Displacement vs Total Distance

Displacement (Net Change)

Displacement=โˆซabv(t)โ€‰dt=s(b)โˆ’s(a)\text{Displacement} = \int_a^b v(t)\,dt = s(b) - s(a)

Total Distance Traveled

Totalย Distance=โˆซabโˆฃv(t)โˆฃโ€‰dt\text{Total Distance} = \int_a^b |v(t)|\,dt

Split the integral where v(t)=0v(t) = 0 (direction changes).

Worked Example

v(t)=t2โˆ’4v(t) = t^2 - 4 on [0,3][0, 3].

v=0v = 0 at t=2t = 2.

Displacement: โˆซ03(t2โˆ’4)โ€‰dt=[t33โˆ’4t]03=9โˆ’12=โˆ’3\int_0^3 (t^2-4)\,dt = [\frac{t^3}{3} - 4t]_0^3 = 9-12 = -3

Total distance: โˆซ02โˆฃt2โˆ’4โˆฃโ€‰dt+โˆซ23โˆฃt2โˆ’4โˆฃโ€‰dt\int_0^2 |t^2-4|\,dt + \int_2^3 |t^2-4|\,dt =โˆซ02(4โˆ’t2)โ€‰dt+โˆซ23(t2โˆ’4)โ€‰dt=163+73=233= \int_0^2 (4-t^2)\,dt + \int_2^3 (t^2-4)\,dt = \frac{16}{3} + \frac{7}{3} = \frac{23}{3}

Displacement vs Distance ๐ŸŽฏ

Key Takeaways โ€” Part 2

  1. Displacement can be negative (net change in position)
  2. Total distance is always positive (use โˆฃv(t)โˆฃ|v(t)|)
  3. Split at points where v(t)=0v(t) = 0 (direction changes)

Part 3: Speed vs Velocity

Particle Motion

Part 3 of 7 โ€” Speed and Speeding Up/Slowing Down

Speed vs Velocity

  • Velocity has direction (can be negative)
  • Speed =โˆฃv(t)โˆฃ= |v(t)| (always non-negative)
  • Maximum speed occurs at an endpoint or where ddtโˆฃv(t)โˆฃ=0\frac{d}{dt}|v(t)| = 0

Speeding Up vs Slowing Down

v(t)v(t)a(t)a(t)Particle is...
++++Speeding up (moving right, accelerating right)
โˆ’-โˆ’-Speeding up (moving left, accelerating left)
++โˆ’-Slowing down
โˆ’-++Slowing down

Key: Same sign = speeding up. Opposite signs = slowing down.

Speed Analysis ๐ŸŽฏ

v(t)=t2โˆ’5t+4=(tโˆ’1)(tโˆ’4)v(t) = t^2 - 5t + 4 = (t-1)(t-4), a(t)=2tโˆ’5a(t) = 2t - 5

Key Takeaways โ€” Part 3

  1. Speed = โˆฃv(t)โˆฃ|v(t)|
  2. Same sign of vv and aa = speeding up
  3. Opposite signs = slowing down

Part 4: Displacement vs Distance

Particle Motion

Part 4 of 7 โ€” Position from Velocity

Given v(t)v(t), Find s(t)s(t)

s(t)=s(0)+โˆซ0tv(ฯ„)โ€‰dฯ„s(t) = s(0) + \int_0^t v(\tau)\,d\tau

Worked Example

v(t)=3t2โˆ’2v(t) = 3t^2 - 2, s(0)=5s(0) = 5. Find s(2)s(2).

s(2)=5+โˆซ02(3t2โˆ’2)โ€‰dt=5+[t3โˆ’2t]02=5+(8โˆ’4)=9s(2) = 5 + \int_0^2 (3t^2 - 2)\,dt = 5 + [t^3 - 2t]_0^2 = 5 + (8-4) = 9

Finding Position ๐ŸŽฏ

Key Takeaways โ€” Part 4

  1. Position = initial position + displacement
  2. Maximum/minimum position occurs when v=0v = 0 (direction change)

Part 5: Motion Analysis

Particle Motion

Part 5 of 7 โ€” Velocity from Acceleration

Given a(t)a(t), Find v(t)v(t)

v(t)=v(0)+โˆซ0ta(ฯ„)โ€‰dฯ„v(t) = v(0) + \int_0^t a(\tau)\,d\tau

Free Fall Model

Near Earth's surface: a(t)=โˆ’g=โˆ’9.8a(t) = -g = -9.8 m/s2^2 (or โˆ’32-32 ft/s2^2)

v(t)=v0โˆ’gtv(t) = v_0 - gt

s(t)=s0+v0tโˆ’12gt2s(t) = s_0 + v_0 t - \frac{1}{2}gt^2

Acceleration to Velocity ๐ŸŽฏ

Key Takeaways โ€” Part 5

  1. Integrate acceleration to find velocity
  2. Free fall: a=โˆ’ga = -g (constant), giving quadratic position

Part 6: Problem-Solving Workshop

Particle Motion

Part 6 of 7 โ€” AP-Style Workshop

AP-Style Motion Problems ๐ŸŽฏ

A particle moves with v(t)=2sinโก(t)v(t) = 2\sin(t) for tโ‰ฅ0t \geq 0.

Workshop Complete!

Part 7: Review & Applications

Particle Motion โ€” Review

Part 7 of 7 โ€” Final Assessment

Final Assessment ๐ŸŽฏ

Particle Motion โ€” Complete! โœ…

You have mastered:

  • โœ… Position, velocity, acceleration relationships
  • โœ… Displacement vs total distance
  • โœ… Speed analysis (speeding up/slowing down)
  • โœ… Finding position from velocity and acceleration