Attempt these before you open a book or a video. Write the argument in the work box and the conclusion in the answer box. Check counts the problem only when both pass, and it does not open the solution. The solution stays locked for twenty minutes after you start the timer.
Attack 1
A block slides down a frictionless incline of angle \(\theta\). Find its acceleration along the incline.
Timer not started. Twenty minutes of real work before a solution.
The forces are gravity and the normal. Along the incline, the component of weight is \(mg\sin\theta\) and the normal does no work along that direction. Newton’s second law gives \(a=g\sin\theta\) down the incline.
Attack 2
Atwood’s machine: masses \(m_1>m_2\) over a massless frictionless pulley. Find the acceleration.
Timer not started. Twenty minutes of real work before a solution.
A projectile is launched with speed \(v\) at angle \(\theta\) from level ground. Show the trajectory is a parabola and that the range is maximized at \(45^\circ\).
Timer not started. Twenty minutes of real work before a solution.
\(x=v\cos\theta\, t\), \(y=v\sin\theta\, t-\tfrac12 gt^2\). Eliminate \(t\): \(y=x\tan\theta-gx^2/(2v^2\cos^2\theta)\), a parabola. Range is the positive \(x\) when \(y=0\): \(R=v^2\sin 2\theta/g\), maximized when \(\sin 2\theta=1\), so \(\theta=45^\circ\).
Newtonian mechanics is the claim that a force changes momentum, together with the models of the forces you actually meet: gravity near the earth, gravity between point masses, springs, and friction. The subject becomes mathematics the moment you write \(\mathbf F=d\mathbf p/dt\) as a differential equation. Energy and momentum are not extra laws. They are the consequences of Newton’s laws when the forces are what they are: momentum is conserved when the total external force vanishes, and mechanical energy is conserved when the forces are gradients of a potential.
OpenStax University Physics Volume 1 is free, calculus-based, and the working book. Halliday, Resnick, and Walker is the traditional paid text; no edition was verified. Kleppner and Kolenkow, and Morin’s Introduction to Classical Mechanics (ISBN 978-0-521-87622-3), are the harder books. Morin’s ISBN was confirmed in the Open Library catalog. MIT 8.01 is the course with exams. Irodov is the ceiling. Feynman is the preview, and Feynman is a bad place to learn to solve problems.
A free-body diagram that does not name the body is a decoration. Draw the body, then the arrows that act on it, then the equation.
Core results
Statements only. Write the argument before you reveal it. A revealed proof you did not attempt is a paragraph you will not be able to rebuild at 2am.
Newton. In an inertial frame, \(\mathbf F_{\mathrm{net}}=d\mathbf p/dt\). For constant mass this is \(m\mathbf a\). Superposition: the net force is the vector sum. The third law, in the form of equal-and-opposite central forces, is what makes internal forces cancel in the momentum balance of a system.
These are the laws, not theorems. The derived statement you must prove is the momentum theorem: the total external force equals the derivative of total momentum, once internal forces cancel by the third law.
Energy. The work–energy theorem: the work of the net force equals the change in kinetic energy. If every force is conservative, mechanical energy is conserved. Gravity near Earth has potential \(mgy\). A spring has potential \(\tfrac12 kx^2\).
Work–energy is the chain rule: \(\mathbf F\cdot\mathbf v=m\mathbf a\cdot\mathbf v=\frac{d}{dt}(\tfrac12 mv^2)\). A conservative force is minus the gradient of a potential, so its work is minus the change in potential.
Momentum and rotation. External impulse equals change in momentum. For a rigid body about a fixed axis, \(\tau=I\alpha\), and \(I\) depends on the axis by the parallel-axis theorem. Angular momentum about a point fixed in an inertial frame, or the center of mass, satisfies \(\boldsymbol\tau=d\mathbf L/dt\) under the usual hypotheses.
The rotational law for a particle is \(\mathbf r\times\mathbf F=d(\mathbf r\times\mathbf p)/dt\) because \(\mathbf v\times\mathbf p=0\). Sum over particles. The parallel-axis theorem is the expansion of \(\int |\mathbf r-\mathbf r_{\mathrm{cm}}+\mathbf d|^2 dm\).
Orbits. An inverse-square central force conserves angular momentum and energy, and the orbit is a conic. For gravity, closed orbits are ellipses with the center of force at a focus.
Angular momentum conservation is the torque of a central force vanishing. The orbit equation comes from the substitution \(u=1/r\) in the radial equation. The conic section is the solution of that linear oscillator equation for \(u(\theta)\).
Oscillations. \(m\ddot x=-kx\) has solutions of period \(2\pi\sqrt{m/k}\). Small oscillations about a stable equilibrium are harmonic, with \(k\) equal to the second derivative of the potential at the minimum. Damping and driving add the standard linear terms.
The characteristic equation \(r^2+\omega^2=0\) gives the period. The small-oscillation claim is Taylor expansion of the potential to second order; the linear term vanishes at an equilibrium.
The ladder
Four rungs, in order. Do not skip a rung because the next one looks more serious.
OpenStax University Physics Volume 1, and MIT 8.01SC Free calculus-based text. The course with exams is https://ocw.mit.edu/courses/8-01sc-classical-mechanics-fall-2016/ . Halliday is the paid traditional book; no edition was verified. OpenStax plus 8.01 is the better pair because you can start tonight and sit a real exam.
Irodov, Problems in General Physics, and Krotov Irodov is the ceiling. Krotov’s Aptitude Test Problems in Physics is the olympiad companion: https://archive.org/details/ptitudetestproblemsinphysics . Use the mechanics parts. The answers in the back of Irodov are a check after the writeup.
Hardest questions
Names and links. The problem text stays on the source site. Copyrighted contest problems are not copied here. What follows is where they are and why they hurt.
Krotov, mechanics Olympiad flavor: the setup is the problem, and the physics is short once you see it.
MIT 8.01 exams Timed, with free-body diagrams that are part of the grade.
Morin, the problems on oscillations and central forces Morin is paid and unlinked as a file. These 8.01 topics are the public stand-in. Morin’s problems are hard because they ask for a clever frame or a conserved quantity.
Pass: one 8.01 exam, timed, plus ten Irodov mechanics problems with free-body diagrams and a sentence naming the conserved quantity if there is one. Fail if a solution uses a formula you cannot derive from \(\mathbf F=m\mathbf a\) in one line.
Diagrams
Weight is vertical. The axes you compute in are along the incline. Do not mix them.
Escalating sets
Five sets. Finish a set before you touch the next. Full sentences, not a circled answer.
Set 1. Newton
Incline, frictionless.
Incline with friction \(\mu\), find the acceleration and the condition for sliding.
Atwood machine.
Two blocks in contact, a force on the first. Find the contact force.
A mass on a string in a horizontal circle. Tension.
Set 2. Energy and momentum
Prove the work–energy theorem in one dimension.
A spring launches a mass. Find the speed.
Elastic collision in one dimension, equal masses.
Inelastic collision, the combined speed.
Ballistic pendulum: combine the two conservation laws and say which applies to which stage.
Set 3. Rotation
Parallel-axis theorem for a point mass.
A pulley of nonzero moment of inertia in an Atwood machine. Write the equations. You need \(\tau=I\alpha\).
Rolling without slipping: \(v=\omega R\). Where does it come from?
Angular momentum of a particle, \(\mathbf r\times\mathbf p\).
A force through the center of mass does not torque about the center of mass. Prove it.
Set 4. Orbits and oscillators
Period of a spring.
Physical pendulum, small angles, period \(2\pi\sqrt{I/mgd}\). Derive it.
Circular orbit speed for gravity, from \(GMm/r^2=mv^2/r\).
Escape speed.
Projectile range, the attack, written cleanly.
Set 5. Ceiling
Ten Irodov mechanics problems.
Three Krotov problems.
One 8.01 exam.
Derive Kepler’s equal-area law from angular momentum.
Oral free-body diagram of the incline.
Return bank
Ten problems to meet again. Logging a writeup schedules them at 1 day, 7 days, and 30 days in this browser.
Frictionless incline.
Atwood.
Projectile range at 45°.
Work–energy theorem.
Ballistic pendulum.
Spring period.
Escape speed.
Rolling condition \(v=\omega R\).
One Irodov problem that took over an hour.
Kepler equal areas.
Oral pass
State Newton’s second law, derive the incline acceleration, and explain when mechanical energy is conserved. No notes.