๐ŸŽฏโญ INTERACTIVE LESSON

Conservation of Momentum

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Conservation of Momentum - Complete Interactive Lesson

Part 1: System Momentum

๐Ÿ”’ Conservation of Momentum โ€” Isolated Systems

Part 1 of 7 โ€” Conservation of Momentum

One of the most powerful principles in all of physics: the total momentum of an isolated system is conserved. This means the total momentum before an interaction equals the total momentum after โ€” no matter how complex the forces between objects are.

pโƒ—i=pโƒ—f\vec{p}_i = \vec{p}_f

This single equation lets us solve problems that would be nearly impossible using Newton's laws alone.

What Is an Isolated System?

An isolated system is one where no net external force acts on the system.

External vs. Internal Forces

Force TypeDefinitionEffect on Total Momentum
InternalForces between objects within the systemNo effect (they cancel by Newton's 3rd Law)
ExternalForces from outside the systemChanges total momentum

Examples

SystemInternal ForcesExternal ForcesIsolated?
Two colliding billiard ballsContact force between themFriction from table (small)Approximately yes
Rifle + bulletExplosion forceGravity, normal forceHorizontally yes
Earth + falling ballGravity between themNone (both included!)Yes!

Key Insight

By carefully choosing what to include in your "system," you can often make external forces cancel or be negligible.

The Law of Conservation of Momentum

If the net external force on a system is zero, the total momentum of the system remains constant.

pโƒ—total,ย initial=pโƒ—total,ย final\vec{p}_{\text{total, initial}} = \vec{p}_{\text{total, final}}

For two objects:

m1vโƒ—1i+m2vโƒ—2i=m1vโƒ—1f+m2vโƒ—2fm_1 \vec{v}_{1i} + m_2 \vec{v}_{2i} = m_1 \vec{v}_{1f} + m_2 \vec{v}_{2f}

Why It Works โ€” Newton's Third Law

When object A pushes on object B, B pushes back on A with an equal and opposite force:

Fโƒ—Aย onย B=โˆ’Fโƒ—Bย onย A\vec{F}_{A \text{ on } B} = -\vec{F}_{B \text{ on } A}

Since both forces act for the same time ฮ”t\Delta t:

Jโƒ—onย B=โˆ’Jโƒ—onย A\vec{J}_{\text{on } B} = -\vec{J}_{\text{on } A}

ฮ”pโƒ—B=โˆ’ฮ”pโƒ—A\Delta \vec{p}_B = -\Delta \vec{p}_A

ฮ”pโƒ—A+ฮ”pโƒ—B=0\Delta \vec{p}_A + \Delta \vec{p}_B = 0

The total momentum change is zero โ€” momentum is transferred, not created or destroyed.

Simple Example

Two Skaters Push Apart

Two ice skaters face each other and push off. Skater A (mA=60m_A = 60 kg) and Skater B (mB=80m_B = 80 kg) are initially at rest.

Before: pi=0+0=0p_i = 0 + 0 = 0

After: pf=mAvA+mBvB=0p_f = m_A v_A + m_B v_B = 0

60vA+80vB=060 v_A + 80 v_B = 0

vA=โˆ’8060vB=โˆ’43vBv_A = -\frac{80}{60} v_B = -\frac{4}{3} v_B

If Skater B moves at +1.5+1.5 m/s:

vA=โˆ’43(1.5)=โˆ’2.0ย m/sv_A = -\frac{4}{3}(1.5) = -2.0 \text{ m/s}

The lighter skater moves faster in the opposite direction โ€” but the total momentum remains zero.

Concept Check โ€” Conservation of Momentum ๐ŸŽฏ

Conservation of Momentum Calculations ๐Ÿงฎ

  1. A 10 kg ball moving at +6 m/s collides with a 5 kg ball at rest. After the collision, the 10 kg ball moves at +2 m/s. What is the velocity of the 5 kg ball? (in m/s)

  2. Two objects (m1=4m_1 = 4 kg at +3+3 m/s, m2=2m_2 = 2 kg at โˆ’6-6 m/s) collide and stick together. What is their final velocity? (in m/s)

  3. A 3 kg object at rest breaks into two pieces. Piece A (1 kg) moves at +12 m/s. What is the velocity of piece B (2 kg)? (in m/s, include sign)

Conservation of Momentum Concepts ๐Ÿ”

Exit Quiz โ€” Isolated Systems โœ…

Part 2: Internal & External Forces

๐ŸŽฑ Two-Object 1D Momentum Problems

Part 2 of 7 โ€” Conservation of Momentum

The most common AP Physics 1 momentum problems involve two objects interacting in one dimension. In this lesson, we'll master the systematic approach to solving these problems using conservation of momentum.

The General 1D Setup

For two objects in one dimension:

m1v1i+m2v2i=m1v1f+m2v2fm_1 v_{1i} + m_2 v_{2i} = m_1 v_{1f} + m_2 v_{2f}

Problem-Solving Steps

  1. Draw a before/after diagram โ€” show velocities with arrows
  2. Choose positive direction โ€” typically the direction of the initially moving object
  3. Assign signed velocities โ€” positive or negative based on direction
  4. Write the momentum equation โ€” substitute known values
  5. Solve for the unknown
  6. Interpret the sign โ€” positive = positive direction, negative = opposite

Three Scenarios

TypeDescriptionUnknowns
Collision (separate after)Objects bounce apartUsually v1fv_{1f} or v2fv_{2f}
Perfectly inelasticObjects stick togethervfv_f (one velocity)
Explosion / recoilObjects push apart from restTwo velocities (need extra info)

Example 1: Head-On Collision

A 6 kg ball moving at +5+5 m/s collides head-on with a 4 kg ball moving at โˆ’3-3 m/s. After the collision, the 6 kg ball moves at +1+1 m/s. Find the velocity of the 4 kg ball.

Before: pi=(6)(+5)+(4)(โˆ’3)=30โˆ’12=+18p_i = (6)(+5) + (4)(-3) = 30 - 12 = +18 kgยทm/s

After: pf=(6)(+1)+(4)(v2f)=6+4v2fp_f = (6)(+1) + (4)(v_{2f}) = 6 + 4v_{2f}

Conservation: 18=6+4v2f18 = 6 + 4v_{2f}

v2f=18โˆ’64=+3ย m/sv_{2f} = \frac{18 - 6}{4} = +3 \text{ m/s}

The 4 kg ball reverses and moves at +3+3 m/s (in the positive direction).

Example 2: Perfectly Inelastic Collision

A 2 kg block moving at +8+8 m/s collides with a 6 kg block at rest. They stick together. Find the final velocity.

m1v1i+m2v2i=(m1+m2)vfm_1 v_{1i} + m_2 v_{2i} = (m_1 + m_2) v_f

(2)(8)+(6)(0)=(2+6)vf(2)(8) + (6)(0) = (2 + 6)v_f

16=8vf16 = 8v_f

vf=+2ย m/sv_f = +2 \text{ m/s}

Energy Check

  • KEi=12(2)(8)2=64KE_i = \frac{1}{2}(2)(8)^2 = 64 J
  • KEf=12(8)(2)2=16KE_f = \frac{1}{2}(8)(2)^2 = 16 J
  • Lost: 64โˆ’16=4864 - 16 = 48 J (converted to heat, sound, deformation)

In a perfectly inelastic collision, kinetic energy is always lost (converted to other forms). This is the maximum KE loss for a given set of initial conditions.

Concept Check โ€” 1D Momentum Problems ๐ŸŽฏ

Two-Object Problem Practice ๐Ÿงฎ

  1. A 4 kg cart at +5 m/s collides with a 6 kg cart at โˆ’2 m/s. They stick together. What is the final velocity? (in m/s, to 1 decimal)

  2. A 0.010 kg bullet at +400 m/s embeds in a 2.0 kg block at rest. What is the final speed of the block+bullet? (in m/s, to 3 significant figures)

  3. A 8 kg ball at +3 m/s hits a 2 kg ball at +1 m/s. The 8 kg ball slows to +2 m/s. What is the final velocity of the 2 kg ball? (in m/s)

Collision Types ๐Ÿ”

Exit Quiz โ€” 1D Problems โœ…

Part 3: Conservation Law

๐Ÿ’ฃ Recoil Problems (Explosion Type)

Part 3 of 7 โ€” Conservation of Momentum

In recoil (or "explosion") problems, objects that start together push apart. Internal forces propel them in opposite directions, but the total momentum of the system is conserved.

Examples: a gun firing a bullet, fireworks exploding, skaters pushing off each other, a nucleus undergoing radioactive decay.

The Recoil Principle

When the system starts at rest, the total initial momentum is zero:

pi=0p_i = 0

By conservation of momentum:

pf=m1v1+m2v2=0p_f = m_1 v_1 + m_2 v_2 = 0

m1v1=โˆ’m2v2m_1 v_1 = -m_2 v_2

What This Means

  • The two objects always move in opposite directions
  • The lighter object moves faster
  • The ratio of speeds is inverse to the ratio of masses:

โˆฃv1โˆฃโˆฃv2โˆฃ=m2m1\frac{|v_1|}{|v_2|} = \frac{m_2}{m_1}

Energy Source

In explosions/recoil, where does the kinetic energy come from?

  • Chemical energy (gunpowder, fuel)
  • Elastic potential energy (spring, muscle contraction)
  • Nuclear energy (radioactive decay)

Internal energy is converted to kinetic energy, but momentum remains zero.

Classic Examples

Gun Recoil

A 5 kg rifle fires a 0.010 kg bullet at 800 m/s. Find the recoil velocity of the rifle.

0=(5)(vr)+(0.010)(800)0 = (5)(v_r) + (0.010)(800) 0=5vr+80 = 5v_r + 8 vr=โˆ’1.6ย m/sv_r = -1.6 \text{ m/s}

The rifle recoils at 1.6 m/s โ€” much slower than the bullet because it is much heavier.

Two Skaters

Skater A (50 kg) and Skater B (75 kg) push off from rest.

0=(50)(vA)+(75)(vB)0 = (50)(v_A) + (75)(v_B) vA=โˆ’7550vB=โˆ’1.5vBv_A = -\frac{75}{50} v_B = -1.5 v_B

If Skater B moves at +2+2 m/s: vA=โˆ’3v_A = -3 m/s.

Energy Analysis

KEtotal=12(50)(3)2+12(75)(2)2=225+150=375ย JKE_{\text{total}} = \frac{1}{2}(50)(3)^2 + \frac{1}{2}(75)(2)^2 = 225 + 150 = 375 \text{ J}

This 375 J came from the chemical energy in the skaters' muscles.

Multi-Piece Explosions

When an object breaks into more than two pieces, we apply conservation of momentum in each direction.

Example: Three-Piece Explosion

A 6 kg object at rest explodes into three pieces:

  • Piece 1 (2 kg): vx=+3v_x = +3 m/s, vy=0v_y = 0
  • Piece 2 (1 kg): vx=0v_x = 0, vy=+6v_y = +6 m/s
  • Piece 3 (3 kg): Find vxv_x and vyv_y

x-direction: 0=(2)(3)+(1)(0)+(3)(v3x)0 = (2)(3) + (1)(0) + (3)(v_{3x}) v3x=โˆ’2ย m/sv_{3x} = -2 \text{ m/s}

y-direction: 0=(2)(0)+(1)(6)+(3)(v3y)0 = (2)(0) + (1)(6) + (3)(v_{3y}) v3y=โˆ’2ย m/sv_{3y} = -2 \text{ m/s}

Piece 3 moves at (โˆ’2,โˆ’2)(-2, -2) m/s, with speed โˆฃv3โˆฃ=4+4=22โ‰ˆ2.83|v_3| = \sqrt{4 + 4} = 2\sqrt{2} \approx 2.83 m/s.

Concept Check โ€” Recoil Problems ๐ŸŽฏ

Recoil Calculations ๐Ÿงฎ

  1. A 3.0 kg rifle fires a 0.020 kg bullet at 600 m/s. What is the recoil speed of the rifle? (in m/s)

  2. An 80 kg astronaut in space throws a 2 kg tool at 10 m/s. What is the astronaut's recoil speed? (in m/s)

  3. A 10 kg object at rest explodes into two pieces. Piece A (4 kg) moves at +15 m/s. What is the speed of piece B? (in m/s)

Round all answers to 3 significant figures.

Recoil Concepts ๐Ÿ”

Exit Quiz โ€” Recoil โœ…

Part 4: Explosions & Recoil

๐Ÿงญ 2D Momentum Conservation

Part 4 of 7 โ€” Conservation of Momentum

Momentum is a vector, and conservation applies to each component independently. When objects collide or interact in two dimensions, we apply conservation of momentum separately in the xx and yy directions.

2D Conservation Equations

In two dimensions, the single vector equation:

pโƒ—i=pโƒ—f\vec{p}_i = \vec{p}_f

becomes two scalar equations:

x-direction:ย m1v1ix+m2v2ix=m1v1fx+m2v2fx\textbf{x-direction: } m_1 v_{1ix} + m_2 v_{2ix} = m_1 v_{1fx} + m_2 v_{2fx}

y-direction:ย m1v1iy+m2v2iy=m1v1fy+m2v2fy\textbf{y-direction: } m_1 v_{1iy} + m_2 v_{2iy} = m_1 v_{1fy} + m_2 v_{2fy}

Velocity Components

If an object moves at speed vv at angle ฮธ\theta from the xx-axis:

vx=vcosโกฮธ,vy=vsinโกฮธv_x = v\cos\theta, \quad v_y = v\sin\theta

Problem-Solving Strategy

  1. Set up a coordinate system (xx and yy axes)
  2. Break all velocities into components
  3. Apply conservation of momentum in xx and yy separately
  4. Solve the two equations (may need both simultaneously)
  5. Find magnitude and direction of the final velocity if needed

Example: 2D Collision

A 2 kg ball moving at 5 m/s in the +x+x direction collides with a 3 kg ball at rest. After the collision, the 2 kg ball moves at 3 m/s at 30ยฐ above the xx-axis. Find the velocity of the 3 kg ball.

x-components: pix=(2)(5)+(3)(0)=10ย kg\cdotpm/sp_{ix} = (2)(5) + (3)(0) = 10 \text{ kgยทm/s} pfx=(2)(3cosโก30ยฐ)+(3)(v2x)p_{fx} = (2)(3\cos 30ยฐ) + (3)(v_{2x}) 10=(2)(2.598)+3v2x10 = (2)(2.598) + 3v_{2x} 10=5.196+3v2x10 = 5.196 + 3v_{2x} v2x=1.60ย m/sv_{2x} = 1.60 \text{ m/s}

y-components: piy=0p_{iy} = 0 pfy=(2)(3sinโก30ยฐ)+(3)(v2y)p_{fy} = (2)(3\sin 30ยฐ) + (3)(v_{2y}) 0=(2)(1.5)+3v2y0 = (2)(1.5) + 3v_{2y} v2y=โˆ’1.0ย m/sv_{2y} = -1.0 \text{ m/s}

Speed: v2=1.602+1.02=3.56=1.89v_2 = \sqrt{1.60^2 + 1.0^2} = \sqrt{3.56} = 1.89 m/s

Direction: ฮธ=arctanโก(โˆ’1.0/1.60)=โˆ’32ยฐ\theta = \arctan(-1.0/1.60) = -32ยฐ (below xx-axis)

2D Perfectly Inelastic Collision

When objects stick together in 2D:

m1vโƒ—1+m2vโƒ—2=(m1+m2)vโƒ—fm_1 \vec{v}_1 + m_2 \vec{v}_2 = (m_1 + m_2)\vec{v}_f

Example

Ball A (2 kg) moves at 4 m/s in the +x+x direction. Ball B (3 kg) moves at 3 m/s in the +y+y direction. They collide and stick.

x: (2)(4)+(3)(0)=5vfx(2)(4) + (3)(0) = 5v_{fx} โ†’ vfx=1.6v_{fx} = 1.6 m/s

y: (2)(0)+(3)(3)=5vfy(2)(0) + (3)(3) = 5v_{fy} โ†’ vfy=1.8v_{fy} = 1.8 m/s

Speed: vf=1.62+1.82=5.80=2.41v_f = \sqrt{1.6^2 + 1.8^2} = \sqrt{5.80} = 2.41 m/s

Direction: ฮธ=arctanโก(1.8/1.6)=48.4ยฐ\theta = \arctan(1.8/1.6) = 48.4ยฐ above the xx-axis

Concept Check โ€” 2D Momentum ๐ŸŽฏ

2D Momentum Calculations ๐Ÿงฎ

  1. A 5 kg ball at 6 m/s (+x+x) collides with a 5 kg ball at rest. They stick together. What is the xx-component of the final velocity? (in m/s)

  2. For the same collision, what is the final speed? (in m/s)

  3. A 3 kg object at 4 m/s (+x+x) and a 1 kg object at 8 m/s (+y+y) collide and stick. What is the final speed? (in m/s, to 3 significant figures)

2D Momentum Concepts ๐Ÿ”

Exit Quiz โ€” 2D Conservation โœ…

Part 5: 2D Momentum Conservation

โš ๏ธ When Is Momentum NOT Conserved?

Part 5 of 7 โ€” Conservation of Momentum

Momentum conservation is powerful, but it doesn't apply to every situation. Understanding when and why momentum is not conserved is just as important as knowing how to use it.

The answer comes down to one thing: external forces.

The Role of External Forces

The complete version of Newton's Second Law for a system:

Fโƒ—net,ย external=dpโƒ—totaldt\vec{F}_{\text{net, external}} = \frac{d\vec{p}_{\text{total}}}{dt}

  • If Fโƒ—net,ย ext=0\vec{F}_{\text{net, ext}} = 0: momentum is conserved โœ…
  • If Fโƒ—net,ย extโ‰ 0\vec{F}_{\text{net, ext}} \neq 0: momentum is NOT conserved โŒ

Common External Forces

External ForceEffectExample
FrictionRemoves momentum from systemSliding collision on rough surface
GravityAdds downward momentum over timeProjectile-style collisions
Normal forceCan add/remove vertical momentumObject hitting a floor
Applied forceChanges system momentumPushing a cart during collision

When Can We Still Use Conservation?

Even with external forces, momentum conservation can be useful in these situations:

1. During Very Short Collisions

If the collision time ฮ”t\Delta t is very small (milliseconds), even large external forces produce negligible impulse:

Jext=Fextฮ”tโ‰ˆ0J_{\text{ext}} = F_{\text{ext}} \Delta t \approx 0

So momentum is approximately conserved during the instant of collision.

2. In One Direction Only

If an external force acts only vertically (like gravity), horizontal momentum is still conserved:

pxย isย conserved(evenย ifย pyย isย not)p_x \text{ is conserved} \quad \text{(even if } p_y \text{ is not)}

3. By Choosing a Larger System

If friction from the floor acts on sliding blocks, include the Earth in your system โ€” then gravity and normal forces become internal! (Impractical, but theoretically valid.)

Example

A ball on a table collides with another ball. Friction acts on both, but during the brief collision instant (ฮ”tโ‰ˆ0.001\Delta t \approx 0.001 s), the friction impulse is negligible. Momentum is conserved during the collision, but not after (friction gradually reduces momentum).

Example: Gravity as External Force

A 2 kg ball is thrown horizontally at 10 m/s off a cliff. After 3 seconds:

Horizontal momentum: px=(2)(10)=20p_x = (2)(10) = 20 kgยทm/s โ€” CONSERVED (no horizontal external force, ignoring air resistance)

Vertical momentum: py=(2)(0+10ร—3)=60p_y = (2)(0 + 10 \times 3) = 60 kgยทm/s downward โ€” NOT conserved (gravity is an external force adding downward impulse)

The impulse from gravity: Jy=mgฮ”t=(2)(10)(3)=60J_y = mg\Delta t = (2)(10)(3) = 60 kgยทm/s โ€” exactly the change in vertical momentum!

Key Takeaway

Always check: Is there a net external force? If yes, momentum is NOT conserved in that direction. But it may still be conserved in the perpendicular direction.

Concept Check โ€” External Forces ๐ŸŽฏ

External Force Analysis ๐Ÿงฎ

  1. A 5 kg ball falls for 4 seconds. How much momentum does gravity add? (in kgยทm/s, use g=10g = 10 m/sยฒ)

  2. Two 3 kg blocks collide on a surface with friction ฮผk=0.2\mu_k = 0.2. If the collision lasts 0.005 s, what is the impulse from friction on the system during the collision? (in Nยทs, use g=10g = 10 m/sยฒ)

  3. For the same system in problem 2, if the blocks slide together for 2 s after colliding, what impulse does friction deliver during this time? (in Nยทs)

Round all answers to 3 significant figures.

Conservation Conditions ๐Ÿ”

Exit Quiz โ€” External Forces โœ…

Part 6: Problem-Solving Workshop

๐Ÿ”ง Problem-Solving Workshop

Part 6 of 7 โ€” Conservation of Momentum

Let's practice solving a variety of momentum conservation problems โ€” from basic 1D collisions to recoil, 2D, and problems with external forces. This workshop focuses on building your problem-solving confidence for the AP exam.

Problem-Solving Checklist

Before writing any equation, always ask:

  1. โœ… Is the system isolated? (No net external force โ†’ momentum conserved)
  2. โœ… What is the system? (Choose objects wisely to eliminate external forces)
  3. โœ… Is this 1D or 2D? (How many equations do I need?)
  4. โœ… Do objects stick together? (Perfectly inelastic โ†’ one final velocity)
  5. โœ… Is energy also needed? (Elastic collision โ†’ both pp and KEKE conserved)
  6. โœ… What are my knowns and unknowns? (List them before solving)

The Master Equation (1D)

m1v1i+m2v2i=m1v1f+m2v2fm_1 v_{1i} + m_2 v_{2i} = m_1 v_{1f} + m_2 v_{2f}

For perfectly inelastic: replace right side with (m1+m2)vf(m_1 + m_2)v_f

Problem 1: Ballistic Pendulum ๐ŸŽฏ

A 0.010 kg bullet embeds in a 2.0 kg wooden block hanging from a string. The block+bullet swings upward to a height of 0.20 m. What was the bullet's speed? (Use g=10g = 10 m/sยฒ)

Hint: Use two steps โ€” conservation of momentum during collision, then conservation of energy during swing.

Problem 2: Head-On Collision ๐Ÿš—

Car A (1500 kg) travels east at 20 m/s. Car B (2000 kg) travels west at 15 m/s. They collide and lock bumpers.

  1. What is the total initial momentum of the system? (in kgยทm/s, take east as positive)

  2. What is the final velocity of the wreckage? (in m/s, to 3 significant figures, include sign)

  3. In which direction does the wreckage move? (type "east" or "west")

Problem 3: Recoil in Space ๐Ÿš€

An astronaut (80 kg) floating at rest in space fires a thruster that ejects 0.50 kg of gas at 2000 m/s relative to the astronaut.

Problem 4: Mixed Practice ๐Ÿ“

  1. A 6 kg block at +4 m/s collides with a 2 kg block at โˆ’8 m/s. They stick together. What is the final velocity? (in m/s)

  2. A 0.15 kg ball at +20 m/s collides with a 0.15 kg ball at โˆ’10 m/s. After collision, the first ball moves at +5 m/s. What is the velocity of the second ball? (in m/s, include sign)

  3. A 50 kg cannon at rest fires a 5 kg ball at 100 m/s. What is the cannon's recoil speed? (in m/s)

Problem Type Identification ๐Ÿ”

Exit Quiz โ€” Problem Solving โœ…

Part 7: Synthesis & AP Review

๐ŸŽ“ Synthesis & AP Review

Part 7 of 7 โ€” Conservation of Momentum

Let's synthesize everything about conservation of momentum: isolated systems, 1D and 2D problems, recoil, and external forces. This review prepares you for AP-level questions on this critical topic.

Key Concepts Summary

ConceptKey EquationWhen to Use
Conservation of momentumpโƒ—i=pโƒ—f\vec{p}_i = \vec{p}_fIsolated system (no net external force)
1D collisionm1v1i+m2v2i=m1v1f+m2v2fm_1 v_{1i} + m_2 v_{2i} = m_1 v_{1f} + m_2 v_{2f}Two objects in a line
Perfectly inelasticm1v1i+m2v2i=(m1+m2)vfm_1 v_{1i} + m_2 v_{2i} = (m_1 + m_2)v_fObjects stick together
Recoil from rest0=m1v1+m2v20 = m_1 v_1 + m_2 v_2Objects push apart from rest
2D conservationApply in xx and yy separatelyObjects move in different directions

When Momentum Is / Isn't Conserved

โœ… ConservedโŒ Not Conserved
No net external forceNet external force acts
During brief collisions (even with friction)Over long times with friction/gravity
In direction perpendicular to external forceIn direction of external force
When system includes all interacting objectsWhen part of the system is excluded

AP Review โ€” Conceptual ๐ŸŽฏ

AP Review โ€” Quantitative ๐Ÿ“

AP Calculation Practice ๐Ÿงฎ

  1. A 0.050 kg bullet at 400 m/s embeds in a 4.95 kg block at rest. What is the block+bullet velocity? (in m/s)

  2. The block+bullet slides along a surface with ฮผk=0.40\mu_k = 0.40. How far does it slide before stopping? (in m, use g=10g = 10 m/sยฒ)

  3. A 60 kg person standing on a 15 kg skateboard at rest throws a 5 kg ball at 12 m/s horizontally. What is the recoil speed of the person+skateboard? (in m/s)

Round all answers to 3 significant figures.

Comprehensive Review ๐Ÿ”

Final Exit Quiz โ€” Conservation of Momentum โœ