Forces, Rotation & Equilibrium — Chapter Practice, Grade 12

Use force diagrams, friction, circular motion, springs, and torque to explain motion and balance.

Problem 1

A net force of 36 N acts on a 4 kg block on a frictionless surface. Find its acceleration.
Answer and explanation

9 m/s²

a = ΣF ÷ m = 36 ÷ 4 = 9 m/s².

Problem 2

A club strikes a 0.045 kg golf ball, giving it an acceleration of 2,000 m/s². What net force did the club apply?
Answer and explanation

90 N

ΣF = ma = 0.045 × 2,000 = 90 N.

Problem 3

A book rests on a table. Earth pulls the book down with the force of gravity. According to Newton's third law, what is the reaction force to this pull?
  1. The book pulling up on the Earth
  2. The book's inertia
  3. The table pushing up on the book
  4. The book pushing down on the table
Answer and explanation

The book pulling up on the Earth

A third-law pair acts on two different objects. If Earth pulls the book down, the reaction is the book pulling Earth up. (The table's push is a separate force, not the reaction to gravity.)

Problem 4

A 1,000 kg elevator rises at a constant velocity. What is the net force on it?
  1. Greater than its weight
  2. Zero
  3. 9,800 N upward
  4. 1,000 N upward
Answer and explanation

Zero

Constant velocity means zero acceleration, so by ΣF = ma the net force must be zero — the cable tension exactly balances the weight.

Problem 5

Explain, using Newton's first law, why a passenger's head snaps backward when a car is rear-ended and lurches forward.
Answer and explanation

Before the impact the passenger's head is at rest. When the car and seat are suddenly pushed forward, the head tends to stay where it was because of inertia (Newton's first law), so it lags behind the moving body and appears to snap backward. A headrest supplies the force needed to accelerate the head along with the body, preventing whiplash.

Problem 6

Two horizontal forces act on a 5 kg object on frictionless ice: 40 N east and 15 N west. Find the object's acceleration.
Answer and explanation

5 m/s²

Net force = 40 − 15 = 25 N east. a = ΣF ÷ m = 25 ÷ 5 = 5 m/s² east.

Problem 7

A 3 kg object accelerates at 2 m/s². Find net force. Show the reasoning, not just the conclusion.
Hints

The reaction to a push acts on the other object, not automatically in this force sum.

Answer and explanation

F_net=ma=6 N in the acceleration direction.

Problem 8

How can a small car and heavy truck exert equal collision forces but have different accelerations?
Hints

State what the supplied observations or conditions establish, and separate that from any assumption.

Answer and explanation

Their interaction forces are equal and opposite; acceleration magnitude depends on each mass.

Problem 9

Interaction partners belong on different free-body diagramsInteraction partners belong on different free-body diagramsbody Abody BB acts on A rightA acts on B leftEqual and opposite; different receiving bodies.
Original separated-body interaction diagram; arrow locations separate labels and are not a contact-geometry claim.
Interpret the supplied visual. Do equal interaction forces require equal accelerations of A and B?
Answer and explanation

No. Different masses can have different accelerations under equal-magnitude forces, and other forces may also act.

Newton’s third law pairs the force B exerts on A with the force A exerts on B. Their magnitudes match and directions oppose, but they act on different bodies. They therefore do not cancel when calculating the acceleration of A alone. In a combined A+B system these mutual forces are internal and cancel in the total external-force account. Identify the agent and receiving body for every arrow before deciding which sum it belongs in.

No. Different masses can have different accelerations under equal-magnitude forces, and other forces may also act.

Response criteria

  • Interpret labels, structures, axes, units and directions correctly.
  • Explain the physical or environmental relationship or mechanism.
  • Respect stated assumptions and distinguish observation from inference.

Problem 10

A 4 kg cart has forces 18 N east and 6 N west. Find acceleration and the partner of the 18 N force.
Answer and explanation

Net=12 N east; a=3 m/s² east. Its third-law partner is the cart’s 18 N force on the pulling agent, not the 6 N resistance on the cart.

Net=12 N east; a=3 m/s² east.

Its third-law partner is the cart’s 18 N force on the pulling agent, not the 6 N resistance on the cart.

Response criteria

  • Use the stated measurements or conditions, with correct units.
  • Connect the result to the physical or environmental mechanism or evidence relationship.
  • Identify the assumption, model limit or further evidence requested.

Problem 11

A 10 kg box on level ground is pushed right with 50 N while friction resists with 20 N. Find the net horizontal force.
Answer and explanation

30 N

Net force = 50 − 20 = 30 N to the right (the vertical weight and normal force cancel).

Problem 12

Two forces act on an object at a right angle: 6 N east and 8 N north. Find the magnitude of the net force.
Answer and explanation

10 N

Perpendicular forces combine by the Pythagorean theorem: √(6² + 8²) = √(36 + 64) = √100 = 10 N.

Problem 13

In a free-body diagram of a book resting on a flat table, which forces should be drawn?
  1. Only the normal force, upward
  2. An applied force and friction
  3. Weight downward and the normal force upward
  4. Only the weight, downward
Answer and explanation

Weight downward and the normal force upward

A resting book feels gravity pulling it down and the table's normal force pushing it up. The two are equal, so it stays in equilibrium.

Problem 14

An object moves in a straight line at constant velocity. Its free-body diagram must show forces that…
  1. include no forces at all
  2. grow larger over time
  3. point in the direction of motion
  4. add up to zero
Answer and explanation

add up to zero

Constant velocity means zero acceleration, so the net force is zero — the forces present must cancel out. (Forces can exist; they simply balance.)

Problem 15

List the forces you would draw on a free-body diagram of a sled being pulled across snow by a horizontal rope, and give the direction of each.
Answer and explanation

Weight pulls straight down; the normal force from the snow pushes straight up; the rope's tension pulls forward (horizontal); and kinetic friction from the snow pushes backward, opposing the sled's motion. If the sled moves at steady speed, the up/down pair cancels and tension equals friction.

Problem 16

A 6.5 kg object on frictionless ice feels two perpendicular forces: 12 N east and 5 N north. Find its acceleration.
Answer and explanation

2 m/s²

Net force = √(12² + 5²) = √(144 + 25) = √169 = 13 N. Then a = ΣF ÷ m = 13 ÷ 6.5 = 2 m/s².

Problem 17

A hanging mass is at rest on one vertical rope, with weight 30 N. Find tension. Show the reasoning, not just the conclusion.
Hints

Normal equals weight only for the specified force and acceleration conditions.

Answer and explanation

30 N upward, balancing weight in the given model.

Problem 18

Why draw only forces acting on the selected object?
Hints

State what the supplied observations or conditions establish, and separate that from any assumption.

Answer and explanation

Newton's second law concerns that object's force sum; partner forces on other objects belong in other diagrams.

Problem 19

Write independent equations along the selected axesWrite independent equations along the selected axesAxisForce equationMotion constraintHorizontalTcosθ−f=maxAcceleration can benonzeroVerticalN+Tsinθ−mg=mayay=0 on a level surfaceTwo component equations share one physical diagram.
Original force equations for a level-table contact model with a single angled tension.
Interpret the supplied visual. Why must N be found before μN in this pulled-block example?
Answer and explanation

The upward tension component changes N, so using mg directly in μN would use the wrong contact force.

A vector equation becomes one scalar equation per perpendicular axis. Independent does not mean unrelated: the same tension angle enters both, and contact constraints can set a component of acceleration. For a block that remains on a horizontal table, ay=0 while ax may be nonzero. Assign signs to every component before substituting values; then solve the vertical support account before using a friction model that depends on N.

The upward tension component changes N, so using mg directly in μN would use the wrong contact force.

Response criteria

  • Interpret labels, structures, axes, units and directions correctly.
  • Explain the physical or environmental relationship or mechanism.
  • Respect stated assumptions and distinguish observation from inference.

Problem 20

A 3 kg block is pulled by 15 N at 30° above horizontal. No vertical acceleration; resistance is 4 N. Find N and ax.
Answer and explanation

N=29.4−7.5=21.9 N. Horizontal net=15cos 30°−4≈8.99 N; ax≈3.00 m/s². The tension is counted once through its components.

N=29.4−7.5=21.9 N.

Horizontal net=15cos 30°−4≈8.99 N; ax≈3.00 m/s².

The tension is counted once through its components.

Response criteria

  • Use the stated measurements or conditions, with correct units.
  • Connect the result to the physical or environmental mechanism or evidence relationship.
  • Identify the assumption, model limit or further evidence requested.

Problem 21

A block is pressed to a surface with a normal force of 50 N. If the coefficient of kinetic friction is 0.40, find the kinetic friction force as it slides.
Answer and explanation

20 N

f = μₖN = 0.40 × 50 = 20 N.

Problem 22

A 15 kg box slides across level ground with μₖ = 0.25. Find the kinetic friction force. (g = 9.8 m/s²)
Answer and explanation

36.75 N

N = mg = 15 × 9.8 = 147 N. f = μₖN = 0.25 × 147 = 36.75 N.

Problem 23

Why is it harder to START a heavy box sliding than to KEEP it sliding once it moves?
  1. The maximum static friction is greater than the kinetic friction
  2. The box loses mass once it moves
  3. Friction disappears the instant the box moves
  4. Kinetic friction is greater than static friction
Answer and explanation

The maximum static friction is greater than the kinetic friction

Maximum static friction (μₛN) exceeds kinetic friction (μₖN), so it takes a bigger force to break the box free than to keep it sliding.

Problem 24

As the tilt angle of a ramp increases, the normal force on a box resting on it…
  1. stays exactly the same
  2. decreases
  3. immediately becomes zero
  4. increases
Answer and explanation

decreases

The normal force equals mg cosθ. As θ grows, cosθ shrinks, so the normal force decreases (reaching zero only at a vertical 90° 'ramp').

Problem 25

Explain the difference between static and kinetic friction, and describe a situation where you can feel the switch between them.
Answer and explanation

Static friction acts between surfaces that aren't sliding yet and adjusts up to a maximum to prevent motion; kinetic friction acts between surfaces already sliding and is a bit weaker. You feel the switch when pushing a heavy couch: it resists until you push past the static maximum, then suddenly 'gives' and slides more easily under the smaller kinetic friction.

Problem 26

A 10 kg box slides down a 30° incline where the coefficient of kinetic friction is μₖ = 0.20. Find its acceleration down the slope. (g = 9.8 m/s²)
Answer and explanation

3.2 m/s²

Along the slope: a = g(sinθ − μₖcosθ) = 9.8(0.5 − 0.20 × 0.866) = 9.8(0.5 − 0.173) = 9.8 × 0.327 ≈ 3.2 m/s². (Mass cancels out.)

Problem 27

A box requires 12 N static friction, while μ_sN=20 N. What is actual static friction? Show the reasoning, not just the conclusion.
Hints

Static friction instead adjusts up to its limiting value.

Answer and explanation

12 N, enough to balance the required tangential force without exceeding the maximum.

Problem 28

Why can changing the incline affect friction magnitude?
Hints

State what the supplied observations or conditions establish, and separate that from any assumption.

Answer and explanation

It changes the normal force and potentially the sliding tendency; friction depends on N and the motion regime.

Problem 29

Use kinetic friction only during relative slidingUse kinetic friction only during relative slidingQuantityValueCalculationMass / support2 kg / 19.6 NLevel, no verticalaccelerationμk0.25fk=0.25×19.6=4.9 NHorizontal pull8.9 Na=(8.9−4.9)/2=2 m/s²Kinetic friction is an approximation for specified contact.
Illustrative supplied coefficient and forces; not an experimental coefficient determination.
Interpret the supplied visual. What changes first if the pull is angled partly upward?
Answer and explanation

Recalculate N using the vertical force balance; then update the kinetic-friction estimate and horizontal net force.

Kinetic friction acts during relative sliding. The school approximation fk≈μkN can model a limited range of surface conditions, although real friction may depend on speed, temperature, deformation and wear. On a level table with no vertical acceleration or extra vertical forces, N=mg here. That equality came from the force account, not from the friction law. State the sliding direction before assigning the sign of fk in Newton’s second law.

Recalculate N using the vertical force balance; then update the kinetic-friction estimate and horizontal net force.

Response criteria

  • Interpret labels, structures, axes, units and directions correctly.
  • Explain the physical or environmental relationship or mechanism.
  • Respect stated assumptions and distinguish observation from inference.

Problem 30

A 5 kg block has μs=0.40 and μk=0.30 on a level surface. For a 15 N push, find static friction; for a 25 N push during sliding, find acceleration.
Answer and explanation

N=49 N; static limit=19.6 N, so 15 N is balanced by 15 N friction. During sliding fk=14.7 N; a=(25−14.7)/5=2.06 m/s² along the push.

N=49 N; static limit=19.6 N, so 15 N is balanced by 15 N friction.

During sliding fk=14.7 N; a=(25−14.7)/5=2.06 m/s² along the push.

Response criteria

  • Use the stated measurements or conditions, with correct units.
  • Connect the result to the physical or environmental mechanism or evidence relationship.
  • Identify the assumption, model limit or further evidence requested.

Problem 31

A car rounds a curve of radius 50 m at a speed of 10 m/s. Find its centripetal acceleration.
Answer and explanation

2 m/s²

a = v²/r = 10² ÷ 50 = 100 ÷ 50 = 2 m/s², directed toward the center of the curve.

Problem 32

A 2 kg ball moves in a horizontal circle of radius 4 m at 6 m/s. Find the centripetal force on it.
Answer and explanation

18 N

F = mv²/r = 2 × 6² ÷ 4 = 2 × 36 ÷ 4 = 72 ÷ 4 = 18 N.

Problem 33

An object moves in a circle at constant speed. In which direction does the net force on it point?
  1. Along the direction of motion (tangent to the circle)
  2. Outward, away from the center
  3. Toward the center of the circle
  4. There is no net force
Answer and explanation

Toward the center of the circle

Uniform circular motion requires a center-seeking (centripetal) net force. The outward feeling is an illusion of the accelerating frame.

Problem 34

If the distance between two masses is doubled, the gravitational force between them becomes…
  1. one-half as strong
  2. twice as strong
  3. unchanged
  4. one-quarter as strong
Answer and explanation

one-quarter as strong

Gravitation is an inverse-square law (F ∝ 1/r²). Doubling r multiplies the force by 1/2² = 1/4.

Problem 35

A satellite orbits Earth at constant speed. Explain why it is still accelerating, and name the force that provides its centripetal force.
Answer and explanation

Even at constant speed the satellite's direction is always changing, and any change in velocity is acceleration — here it is centripetal acceleration pointing toward Earth's center. The force supplying it is gravity: Earth's gravitational pull provides exactly the mv²/r needed to bend the satellite's path into a circle, so it 'falls around' the planet.

Problem 36

A 1,200 kg car rounds a flat curve of radius 80 m at 20 m/s. What centripetal force must friction supply?
Answer and explanation

6000 N

F = mv²/r = 1,200 × 20² ÷ 80 = 1,200 × 400 ÷ 80 = 1,200 × 5 = 6,000 N, directed toward the center of the curve.

Problem 37

At fixed mass and radius, how does doubling circular speed change required force? Show the reasoning, not just the conclusion.
Hints

Centripetal describes net inward force, not an additional mysterious interaction.

Answer and explanation

It quadruples force because F=mv²/r.

Problem 38

A satellite moves farther from the same spherical planet. How does gravitational field vary outside it?
Hints

State what the supplied observations or conditions establish, and separate that from any assumption.

Answer and explanation

g=GM/r² decreases with distance from the center; doubling r gives one quarter the field.

Problem 39

Gravitational separation is measured between centersGravitational separation is measured between centerscenter-to-center rEarthF = GMm/r²; altitude h is not the same as r.For Earth radius R: r = R+h.
Original spherical-source separation model; Earth/satellite sizes and distances are not to scale.
Interpret the supplied visual. At altitude h=R, what fraction of surface g does this model predict?
Answer and explanation

r=2R, so g is one quarter of its surface value.

For ideal point masses or a spherical source outside its surface, Newtonian gravitation gives F=GMm/r² with center-to-center separation r. A satellite’s altitude h above a spherical Earth is not r; use r=R+h. Doubling center distance reduces force and gravitational acceleration to one quarter. The familiar near-surface g≈9.8 m/s² is an approximation over modest height differences, not the same value at every orbital distance.

r=2R, so g is one quarter of its surface value.

Response criteria

  • Interpret labels, structures, axes, units and directions correctly.
  • Explain the physical or environmental relationship or mechanism.
  • Respect stated assumptions and distinguish observation from inference.

Problem 40

A 0.50 kg mass moves at 4.0 m/s in a 2.0 m horizontal circle. Find inward acceleration and required net force; name what else is needed to identify tension.
Answer and explanation

ac=16/2=8.0 m/s² and inward net force=0.50×8=4.0 N. Tension equals that net only if the specified geometry and other forces establish it as the sole inward contribution.

ac=16/2=8.0 m/s² and inward net force=0.50×8=4.0 N.

Tension equals that net only if the specified geometry and other forces establish it as the sole inward contribution.

Response criteria

  • Use the stated measurements or conditions, with correct units.
  • Connect the result to the physical or environmental mechanism or evidence relationship.
  • Identify the assumption, model limit or further evidence requested.

Problem 41

k=100N/m,x=.03 m. Find force magnitude.
Hints

Write the relationship first; substitute with consistent units.

Answer and explanation

3 N

100×.03=3.

Problem 42

Why can zero net force still permit rotation?
Answer and explanation

The force lines can produce a nonzero net torque about the object.

Response criteria

  • State a scientifically accurate conclusion.
  • Show the calculation or mechanism that supports it.
  • Include units, conditions, or limits where relevant.

Problem 43

Find spring energy for k=200 N/m and x=.10 m.
Hints

List the given quantities, select a relationship, and check units before substituting.

Answer and explanation

1 J

½×200×.10²=1.

Problem 44

Why is spring work not final force times extension?
Answer and explanation

Force varies with extension; integrate or use the triangular graph area.

Response criteria

  • State a scientifically accurate conclusion.
  • Show the calculation or mechanism that supports it.
  • Include units, conditions, or limits where relevant.

Problem 45

A spring of k=200 N/m is stretched 0.05 m within its linear range. Find force magnitude. Show the reasoning, not just the conclusion.
Hints

Use perpendicular lever arm and rotational sign.

Answer and explanation

F=kx=10 N, directed toward restoring equilibrium.

Problem 46

Why does static equilibrium require both zero net force and zero net torque?
Hints

State what the supplied observations or conditions establish, and separate that from any assumption.

Answer and explanation

Zero net force prevents translational acceleration; zero net torque prevents angular acceleration.

Problem 47

Static equilibrium requires force and torque balanceStatic equilibrium requires force and torque balance30 N at 0.30 m30 N at 0.30 msupport 60 NΣF=0 and Στ=0 are both required.
Original symmetric weightless-bar model; distributed bar weight is intentionally excluded here.
Interpret the supplied visual. Could a zero-torque calculation alone establish static equilibrium?
Answer and explanation

No. The vector force sum must also vanish, and the starting state must be at rest.

Static equilibrium means the body remains at rest without translational or rotational acceleration. It needs ΣF=0 and Στ=0 about a selected pivot in the rigid-body model. Equal opposing torques alone can coexist with nonzero net force, while balanced forces can still form a turning couple. For this weightless-bar example equal downward loads at equal opposite arms balance torque, and the upward support must balance their combined 60 N force.

No. The vector force sum must also vanish, and the starting state must be at rest.

Response criteria

  • Interpret labels, structures, axes, units and directions correctly.
  • Explain the physical or environmental relationship or mechanism.
  • Respect stated assumptions and distinguish observation from inference.

Problem 48

A weightless 2 m beam is pivoted at its left end. A 60 N load acts 0.50 m from the pivot. An upward force acts at the right end. Find that force and vertical pivot reaction for equilibrium.
Answer and explanation

Torque balance: F×2=60×0.50, so F=15 N upward. Vertical balance gives pivot reaction=60−15=45 N upward. Both balances are necessary.

Torque balance: F×2=60×0.50, so F=15 N upward.

Vertical balance gives pivot reaction=60−15=45 N upward.

Both balances are necessary.

Response criteria

  • Use the stated measurements or conditions, with correct units.
  • Connect the result to the physical or environmental mechanism or evidence relationship.
  • Identify the assumption, model limit or further evidence requested.

Problem 49

OpenSciEd drawing of six cushioning rings arranged in a triangle with a broad base on the table and one top ring touching the loaded plate.
The source arrangement shows rings supporting a plate/load; it contains no quantitative force–time or force–extension record. Triangular stack of cushioning rings · OpenSciEd · 8.1 Contact Forces, Lesson 13, source, CC BY 4.0. Figure excerpt rendered from the PDF and resized for the web.
Select the loaded plate as the body. Name its vertical forces at rest, identify the support force’s third-law partner and explain why this drawing alone cannot establish impact peak force.
Answer and explanation

The rings push the loaded plate upward and Earth attracts that selected plate/load downward. Their magnitudes balance at rest but they are not a third-law pair. The plate pushes the rings downward as the support force’s partner on a different body. Impact peak force requires a time-resolved interaction and motion record, not a static layout.

Read source labels, scope, axes and intentional omissions.

Use the complete local explanation to draw a justified mechanism or calculate a supported quantity.

State what is observed, what is assumed and what evidence remains needed.

Response criteria

  • Interpret the source labels, units and scope accurately.
  • Explain the relevant mechanism with a labeled model or supported calculation.
  • Identify a meaningful assumption, uncertainty or missing comparison.

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