Classical MechanicsBSc · Notes

Problems across the course

These problems combine methods and assumptions from different chapters. The chapter exercise sets provide additional practice with each individual concept. Hints and worked solutions are on a separate page.

Geometry and work

  1. F1 A bead of mass mm moves on the rising parabola y=cx2+Uty=cx^2+Ut under gravity. Use q=xq=x to find the velocity, virtual displacement, kinetic energy, generalized gravity force, and equation of motion.

  2. F2 A pendulum is described by arc coordinate s=aθs=a\theta. Construct LL, its momentum, and HH, and compare with angular coordinates.

Lagrangians and forces

  1. F3 Two Atwood masses are joined over a pulley with moment of inertia II and radius RR, with no slip. Find the acceleration.

  2. F4 A pendulum with small angular displacement has viscous torque −bθ˙-b\dot\theta and driving torque τ0cos⁡Ωt\tau_0\cos\Omega t. Construct its equation and persistent amplitude.

  3. F5 For L=12m(x˙2+y˙2)−12k(x−y)2L=\tfrac12m(\dot x^2+\dot y^2)-\tfrac12k(x-y)^2, identify a cyclic coordinate and solve the two independent motions.

Hamiltonians and state space

  1. F6 Construct HH and its equations for L=12a(q)q˙2−V(q)L=\tfrac12a(q)\dot q^2-V(q), and verify the Lagrange equation.

  2. F7 A free particle is described by x=q+X(t)x=q+X(t). Find the Hamiltonian and equations; explain its relation to laboratory momentum.

  3. F8 Describe the pendulum phase portrait on the two sides of energy 2mga2mga, and explain the role of a string constraint.

Radial motion and stability

  1. F9 For V(r)=arnV(r)=ar^n with an>0an>0, find the circular condition and local frequency ratio.

  2. F10 A potential has Veff(rc+η)=Ec+Aη4+O(η5)V_{\rm eff}(r_c+\eta)=E_c+A\eta^4+O(\eta^5) with A>0A>0. What can be said about local radial stability?

Kepler orbits and timing

  1. F11 For μ=k=1\mu=k=1, a particle starts at r=(1,0)\mathbf r=(1,0) with velocity (0,3/2)(0,\sqrt{3/2}). Find E,ℓ,e,a,raE,\ell,e,a,r_a, and period.

  2. F12 Two equal masses mm move on a circular relative orbit of separation dd. Find the period and each body’s speed about the center of mass.

  3. F13 An ellipse has the same angular momentum as a circle of radius rcr_c but eccentricity e=0.8e=0.8. Find its semimajor axis and period ratio to that circle.

Runge–Lenz vector and encounters

  1. F14 For μ=k=1\mu=k=1, r=(1,0,0)\mathbf r=(1,0,0) and p=(1/2,1,0)\mathbf p=(1/2,1,0), calculate the eccentricity vector and periapsis direction.

  2. F15 How must impact parameter change to keep the same attractive deflection if incoming speed doubles?

  3. F16 Explain which conserved quantities remain when a small time-independent radial perturbation is added to inverse-square attraction.

Chapter problem collections

Subject Exercises and solutions
Constraints and virtual work Chapters 1–6, solutions
Lagrangian mechanics Chapters 7–11, solutions
Hamiltonian mechanics Chapters 12–15, solutions
Central-force motion Chapters 16–22, solutions
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