# Choose a mechanics text and justify your model before calculating — Study worksheet

[Study guides](https://unireadinglist.com/guides/mechanics/)

[Course topic: Classical Mechanics](https://unireadinglist.com/subjects/physics/#course-mechanics)

Sources checked: 2026-11-03

Study route and exercise: University Reading List editorial project.

This route connects elementary Newtonian mechanics to an optional analytical extension. It uses College Physics second edition, Taylor’s Classical Mechanics and Cline’s 2021 third-edition PDF, version 3.0. The first is algebra-based; the other two are not first physics books. The tasks and spring example are original study suggestions, not a university syllabus, apparatus test or engineering design specification.

## Choose your starting point

- [ ] I need free first-course mechanics
  Begin with the mechanics chapters of College Physics 2e. Algebra, trigonometry, units and force diagrams are the entry requirements; you do not need calculus to work through that introductory route.

- [ ] I have first-year physics and calculus
  Use Taylor to deepen the connection between differential equations, conservation laws and oscillations. Attempt the first force-and-energy checks before treating the variational chapters as a shortcut around Newtonian reasoning.

- [ ] I want a free analytical extension
  Choose Cline after the stated mathematical preparation. Work selectively from its Newtonian review into variations and Lagrangian dynamics. A free advanced book removes a payment barrier, not a prerequisite barrier.

## Compare the three books

### College Physics 2e

Paul Peter Urone; Roger Hinrichs · 2 · 2022
A free algebra-based foundation

Choose it when: You need to draw and resolve forces, interpret motion and explain energy changes before using a calculus-based formulation.
Use another route when: Your assigned course already requires differential-equation solutions, generalized coordinates or a full analytical mechanics treatment.
Selected reading: Chapters 1–5 establish units, motion and forces; 7–8 cover energy and momentum; selected sections of 16 introduce oscillations.
Limits and trade-offs: It is a broad introductory physics text, not an advanced mechanics replacement. Reading only these selections does not cover all of its physics topics.

#### Try before choosing

After the OpenStax force/energy selections, draw the block’s free-body diagram during compression and state the work signs for friction and the spring.
Check your work: Your diagram has four forces, balanced vertical components, and negative work by both horizontal forces during compression. A zero final speed is not labelled force equilibrium.

Your notes:

________________________________

ISBN: 9781711470832

[Official free reading](https://openstax.org/books/college-physics-2e/pages/preface)

[Book record and access options](https://unireadinglist.com/subjects/physics/college-physics-2e/)

### Classical Mechanics

John R. Taylor · 2005
An intermediate calculus-based bridge

Choose it when: You have introductory mechanics and can differentiate, integrate and work with ordinary differential equations.
Use another route when: You are still confusing velocity with acceleration or cannot yet construct a force diagram; repair that foundation first.
Selected reading: Chapters 1, 3–5 support this route; chapters 6–7 introduce variations and Lagrange’s equations.
Limits and trade-offs: It is not necessary to buy Taylor to attempt the free foundation or Cline extension. The publisher’s 2005 record and current distributor’s 2004 release metadata differ; identify the author and ISBN rather than inventing a revised edition.

#### Try before choosing

With Taylor’s Newtonian and energy route, start from m v dv/dx=−kx−μmg and integrate from contact to the first stop.
Check your work: The integral reproduces ½mv0²=½kx²+μmgx with consistent limits and units. Explain where the relation ceases to describe the subsequent phase.

Your notes:

________________________________

ISBN: 9781891389221

[Book record and access options](https://unireadinglist.com/subjects/physics/classical-mechanics-taylor/)

### Variational Principles in Classical Mechanics

Douglas Cline · 3 · 2021
An open analytical extension

Choose it when: You can connect Newtonian equations to coordinates and want to compare formulations while retaining a free complete text.
Use another route when: You need an algebra-only first explanation or expect variational notation to remove the need to understand constraints and forces.
Selected reading: Version 3.0: chapter 2 for Newtonian review, 3 for oscillators, 5–6 for variations and Lagrangian dynamics, and 10 for nonconservative systems.
Limits and trade-offs: The author’s LibreTexts version is separately revised. Chapter and version claims here are checked against the archived third-edition PDF, not inferred from a current web-page date.

#### Try before choosing

After Cline’s variation/Lagrangian selections, write T, V and the generalized friction force for horizontal x during rightward compression.
Check your work: T=½mẋ², V=½kx² and Qx=−μmg give mẍ+kx=−μmg. Do not hide dry friction inside a conservative potential or keep its sign after reversal.

Your notes:

________________________________

ISBN: 9780998837239

[Official free reading](https://urresearch.rochester.edu/fileDownloadForInstitutionalItem.action?itemId=37135&itemFileId=191022)

[Book record and access options](https://unireadinglist.com/subjects/physics/variational-principles-classical-mechanics-cline/)

## Check your preparation

### A 2 kg object has acceleration 3 m/s². What is its net force?

Your notes:

________________________________

### Does zero instantaneous velocity imply zero net force?

Your notes:

________________________________

### Can you differentiate x=t² twice?

Your notes:

________________________________

## Six steps with a concrete output

- [ ] 1. Describe motion with units and a frame

Selected reading: College Physics chapters 1–3; Taylor chapter 1; Cline 2.2–2.3.

Make this: Choose an origin and positive direction, label position, velocity and acceleration, and describe an event in that frame.

Check your work: State a time interval and units. A negative velocity need not mean slowing down; compare the signs of velocity and acceleration.

Your notes:

________________________________

- [ ] 2. Draw forces on one chosen object

Selected reading: College Physics chapters 4–5; Taylor chapter 1; Cline chapter 2.

Make this: Draw the spring-example block and list the agents exerting forces. Resolve vertical and horizontal equations before inserting numbers.

Check your work: Normal force and weight cancel vertically here, not on every surface. The third-law partners act on different objects and must not be canceled on one diagram.

Your notes:

________________________________

- [ ] 3. Account for work and mechanical energy

Selected reading: College Physics 7.1–7.6; Taylor chapter 4; Cline 2.10.

Make this: Complete the worked compression problem below. Identify the spring energy and the energy transferred by friction, and predict the effect of removing friction.

Check your work: Every term in the balance has units of joules. Do not conserve the block–spring mechanical energy while omitting the friction transfer.

Your notes:

________________________________

- [ ] 4. Separate impulse from a stopped instant

Selected reading: College Physics chapter 8; Taylor chapter 3; Cline 2.4 and 2.8.

Make this: Write a momentum-change statement for the block from spring contact until its first stop. Name the external horizontal interactions on the chosen system.

Check your work: A final zero momentum does not imply zero impulse or momentum conservation. Explain which interactions supply the change.

Your notes:

________________________________

- [ ] 5. Compare an ideal oscillator with the rough track

Selected reading: College Physics 16.1–16.5; Taylor chapter 5; Cline chapter 3.

Make this: Set friction to zero for a separate ideal spring model and compare its compression bound with the rough-track result. Calculus-ready readers can derive its oscillator equation.

Check your work: Do not import the frictionless sinusoidal motion or a constant-acceleration formula into a model whose spring force varies with position.

Your notes:

________________________________

- [ ] 6. Decide whether to change formulation

Selected reading: Taylor chapters 6–7; Cline chapters 5–6 and 10; revisit College Physics chapter 4 if the calculus bridge is not ready.

Make this: State one coordinate and the assumptions that leave it independent. Prepared readers can form L=½mẋ²−½kx² and add the compression-phase generalized force Q=−4 N.

Check your work: During positive compression the equation must agree with Newton: mẍ+kx=−4 N. Beginners should record the missing calculus skills rather than claim to have completed this analytical derivation.

Your notes:

________________________________

## Worked exercise: Original example: how far does a spring compress on a rough track?

A 2.00 kg block meets an uncompressed spring at 3.00 m/s on a horizontal rough track. The spring constant is 100 N/m, kinetic friction coefficient 0.20, and use g=10.0 m/s². Find the first maximum compression.

Assumptions: The spring is massless and linear. The block stays in contact with the horizontal surface; no air drag or other work is included. Kinetic friction opposes motion throughout the positive-compression phase. The invented values describe this model only. Static friction and subsequent motion are not specified.

Your notes:

________________________________

## Change an assumption: The stop does not finish the motion problem

Retain the original block, spring, kinetic coefficient 0.20 and g=10.0 m/s². Add a static coefficient 0.30; keep the same massless linear spring and horizontal contact. Determine whether reversal begins at x≈0.3861 m, then find the speed at the uncompressed spring position if the block returns there. Assume the kinetic coefficient remains 0.20 while sliding.

Your notes:

________________________________

## Before moving on

- Choose the algebra, intermediate or analytical route and name the mathematical skills still needed for the next one.
- Solve the compression model with an explicit system, signs, energy balance, admissible root and frictionless comparison.
- Explain why an alternative force or momentum description agrees with the energy result, and which extra information is needed for the next motion phase.

## Answer and interpretation

### A 2 kg object has acceleration 3 m/s². What is its net force?

6 N, in the acceleration direction. This is the resultant force, not necessarily the value of any one applied force.

### Does zero instantaneous velocity imply zero net force?

No. At the top of an ideal vertical throw, velocity is momentarily zero while gravitational acceleration is still downward. Equilibrium requires a force condition, not just a stopped instant.

### Can you differentiate x=t² twice?

The first derivative is 2t and the second is 2. If this operation is unfamiliar, follow the algebra-based route while learning derivatives and differential equations before the analytical extension.

### Original example: how far does a spring compress on a rough track?

1. Choose positive x into the spring. Vertical balance gives N=mg=20 N, so the kinetic friction magnitude is μN=4 N. During compression the horizontal force is −100x−4 N.
2. The initial kinetic energy is ½×2×3²=9 J. At the first maximum compression the velocity is zero: 9=½×100x²+4x, with x in meters.
3. Solve 50x²+4x−9=0. The nonnegative root is x=(−4+√1816)/100≈0.3861 m. The negative root does not describe positive compression.
4. At that x the spring stores about 7.455 J and friction transfers about 1.545 J; their sum is 9 J. Just before the stop, acceleration tends to (−100x−4)/2≈−21.31 m/s² despite velocity tending to zero.

The first maximum compression is approximately 0.386 m. Zero velocity at this point is not evidence of force equilibrium or a statement about what happens after the stop.

Test the result: Without friction the compression would be √(18/100)≈0.424 m, so the rough-track answer is smaller as expected. Check joule units in 50x² and 4x. To predict sticking or reversal after the stop, specify static friction and apply the new phase’s force conditions.

### Change an assumption: The stop does not finish the motion problem

1. The largest static friction is μs mg=0.30×2×10=6 N. The spring pulls back with kx≈38.61 N, so static friction cannot hold the block and leftward motion begins.
2. During return, friction points right. The stored spring energy is about 7.455 J; return friction dissipates 4×0.3861≈1.545 J. The remaining kinetic energy is about 5.911 J.
3. ½mv²=5.911 gives v≈2.431 m/s at x=0. This is a speed; velocity is negative under the original positive-x convention.

The block reverses and reaches x=0 moving left at about 2.43 m/s. Friction has acted over both the compression and return paths, so the initial 3.00 m/s is not recovered.

Test the result: The two friction losses sum to about 3.089 J, and 9−3.089≈5.911 J. Sticking would require μs≥kx/(mg)≈1.93 in this ideal model; the original unspecified static friction could not determine reversal.

## Common mistakes

### Combining forces from different diagrams

A third-law pair connects two different bodies. Define the object or system before summing forces, and identify which interactions are internal to it.

### Conserving the wrong quantity

Momentum, mechanical energy and total energy have different conditions. A rough track can change block momentum and dissipate block–spring mechanical energy without violating total energy conservation.

### Treating a turning point as equilibrium

Instantaneous rest is a velocity statement. The spring force can be large at maximum compression; friction conditions also change when sliding stops.

## Sources and edition checks

- [OpenStax: College Physics 2e — preface and prerequisites](https://openstax.org/books/college-physics-2e/pages/preface)
  The official preface verifies free web/PDF access and the algebra-and-trigonometry prerequisite. Free access does not include all instructor-only solutions.

- [OpenStax: College Physics 2e — Newton’s laws chapter outline](https://openstax.org/books/college-physics-2e/pages/4-introduction-to-dynamics-newtons-laws-of-motion)
  The chapter outline anchors the force-diagram reading; our tasks and checks are proposed activities.

- [OpenStax: College Physics 2e — work and energy chapter outline](https://openstax.org/books/college-physics-2e/pages/7-introduction-to-work-energy-and-energy-resources)
  The work/energy outline supports the chosen energy selections. The original block, numbers and solution are not copied textbook problems.

- [OpenStax: College Physics 2e — oscillatory motion chapter outline](https://openstax.org/books/college-physics-2e/pages/16-introduction-to-oscillatory-motion-and-waves)
  The chapter outline distinguishes the ideal oscillator selections from the rough-track calculation.

- [University Science Books: Classical Mechanics by John R. Taylor](https://uscibooks.aip.org/books/classical-mechanics/)
  The original publisher identifies Taylor, the print ISBN 9781891389221 and a 2005 record. We retain that bibliographic year and note distributor date differences.

- [MIT Press / University Science Books: Taylor contents](https://mitpress.ublish.com/book/classical-mechanics)
  The publisher-distributed contents establish the Newton, energy, oscillator and variational chapter map; a distributor date is not evidence of a new edition.

- [University of Rochester: Cline third edition, version 3.0](https://urresearch.rochester.edu/institutionalPublicationPublicView.action?institutionalItemId=36044)
  The institutional archive identifies the third edition, version 3.0, issued in 2021. Repository update dates are separate.

- [University of Rochester: official version 3.0 PDF](https://urresearch.rochester.edu/fileDownloadForInstitutionalItem.action?itemId=37135&itemFileId=191022)
  The official PDF confirms the version, chapter map and PDF ISBN 9780998837239. It supplies source evidence, not a claim that our learning sequence was classroom-tested.

These are proposed study activities, not official course assignments or a claim that every book has been read cover to cover.

[How we curate](https://unireadinglist.com/editorial/)
