EnergyHard

Spring, rod and body (roto-translation)

A homogeneous rod and a point body, each of mass m₁ = m₂ = 2 kg, lie on a smooth horizontal plane. A spring (k = 40000 N/m) compressed by Δx = 5 cm sits between one end of the rod and the body. Find the speed v of the body after release.
m₁ m₂ Δx
Given data
m₁ = m₂ = 2 kgk = 40000 N/mΔx = 0.05 m
Review the theory: Energia e Lavoro
Steps
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  1. The compressed spring stores elastic potential energy. On release this is the only available energy and it will all convert into kinetic energy of the system: that's why I compute it first. The energy of a spring compressed by Δx is E = ½·k·Δx².
  2. The plane is smooth, so no external forces/torques act: energy, linear momentum and angular momentum are all conserved. The rod does not only translate but also rotates (roto-translation), so the elastic energy is shared between body and rod. Imposing the three conservation laws gives ½kΔx² = (5/2)·m·v², hence v = √(kΔx²/(5m)).
Full worked solution
  1. The compressed spring stores elastic potential energy. On release this is the only available energy and it will all convert into kinetic energy of the system: that's why I compute it first. The energy of a spring compressed by Δx is E = ½·k·Δx².
    E=12k Δx2=12⋅40000⋅0.052E = \tfrac12 k\,\Delta x^2 = \tfrac12\cdot 40000\cdot 0.05^2
    E=12⋅40000⋅0.0025=50 JE = \frac12\cdot40000\cdot0.0025 = \mathbf{50\,J}.
  2. The plane is smooth, so no external forces/torques act: energy, linear momentum and angular momentum are all conserved. The rod does not only translate but also rotates (roto-translation), so the elastic energy is shared between body and rod. Imposing the three conservation laws gives ½kΔx² = (5/2)·m·v², hence v = √(kΔx²/(5m)).
    v=k Δx25m=40000⋅0.00255⋅2v = \sqrt{\frac{k\,\Delta x^2}{5m}} = \sqrt{\frac{40000\cdot 0.0025}{5\cdot 2}}
    v=100/10=10≈3.16 m/sv = \sqrt{100/10} = \sqrt{10} \approx \mathbf{3.16\,m/s}. The 5/2 factor comes from I=mℓ2/12I = m\ell^2/12.
Result:v≈3.16v \approx 3.16 m/s