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The Lumenary

Practice · Early undergraduate

Classical mechanics

Classical mechanics

Warm-upHuman

A football is kicked from the ground at 20 m/s20\ \mathrm{m/s}, at 45∘45^\circ above the horizontal. Ignoring air resistance and taking g=10 m/s2g = 10\ \mathrm{m/s^2}, how far away (in metres) does it land?

Classical mechanics

Warm-upHuman

An astronaut has mass 7070 kg. On the Moon (g≈1.6 m/s2g \approx 1.6\ \mathrm{m/s^2}), which statement is correct?

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Classical mechanics

Warm-upHuman

A hockey puck slides in a straight line at constant speed across perfectly frictionless ice. What is the net horizontal force on it?

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Classical mechanics

CoreHuman

A mass of 0.50.5 kg hangs on a spring of stiffness k=18 N/mk = 18\ \mathrm{N/m}. What is the angular frequency ω\omega of its small oscillations, in rad/s?

Classical mechanics

CoreHuman

An asteroid orbits the Sun on an ellipse with semi-major axis 44 AU (Earth's is 11 AU, with period 11 year). Using Kepler's third law, what is its period in years?

Classical mechanics

CoreHuman

A particle moves under a central force F=f(r,t) r^\mathbf F = f(\mathbf r, t)\,\hat{\mathbf r} (always pointing along the line to the origin). Which of the following are guaranteed to be constant? (Select all that apply.)

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Classical mechanics

StretchHuman

A comet moves under the Sun's gravity with total energy E>0E > 0 and angular momentum L≠0L \ne 0. What is the shape of its orbit?

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Classical mechanics

StretchHuman

For a particle in the plane under a central potential, L=12m(r˙2+r2θ˙2)−V(r)\mathcal L = \tfrac12 m(\dot r^2 + r^2\dot\theta^2) - V(r). What is the Euler–Lagrange equation for θ\theta?

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Classical mechanics

StretchFormal

In Lean, r v : ℝ → Fin 3 → ℝ describe a motion with hr : ∀ t, HasDerivAt r (v t) t. Which extra hypothesis expresses “the force is central”, so that r t ⨯₃ v t is constant?

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Classical mechanics

StretchComputational

Write verlet(x0, v0, h, n, accel) implementing the velocity Verlet method for x′′=a(x)x'' = a(x): each step does v←v+h2a(x)v \leftarrow v + \tfrac h2 a(x), then x←x+hvx \leftarrow x + h v, then v←v+h2a(x)v \leftarrow v + \tfrac h2 a(x). Return the final (x, v). Test it on the harmonic oscillator a(x)=−xa(x) = -x: after one period 2π2\pi the state should return to its start, and the energy 12v2+12x2\tfrac12 v^2 + \tfrac12 x^2 should stay almost constant.

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