FM1-3 Elastic strings and springs and elastic energy — coverage pack

2 specification leaves · notes, questions, answers and worked methods

FM1-3.1 · Elastic strings and springs. Hooke's law.

  • For a spring obeying Hooke's law, the tension has magnitude T=kxT=kx, where kk is the spring constant and xx is the extension.
  • For an elastic string of natural length ll and modulus λ\lambda, Hooke's law is T=λx/lT=\lambda x/l while the string is taut.
  • Extension is stretched length minus natural length. A string becomes slack rather than exerting a compressive force when this value is non-positive.
  • Keep spring constant and modulus distinct: kk has units N m1\text{N m}^{-1}, whereas λ\lambda has units N\text{N}.

Tier 1 · Easy

  1. 1. A light spring has spring constant 80N m180\,\text{N m}^{-1} and is extended by 0.06m0.06\,\text{m}. Find its tension.[2 marks]

    Answer

    • 4.8N4.8\,\text{N}

    Method: Hooke's law for a spring gives T=kx=80(0.06)=4.8NT=kx=80(0.06)=4.8\,\text{N}.

Tier 2 · Standard

  1. 1. An elastic string has natural length 1.5m1.5\,\text{m} and modulus 120N120\,\text{N}. It is stretched to length 1.8m1.8\,\text{m}. Calculate its tension.[3 marks]

    Answer

    • 24N24\,\text{N}

    Method: The extension is x=1.81.5=0.3mx=1.8-1.5=0.3\,\text{m}. Therefore T=λx/l=120(0.3)/1.5=24NT=\lambda x/l=120(0.3)/1.5=24\,\text{N}.

Tier 3 · Hard

  1. 1. A 1.5kg1.5\,\text{kg} particle hangs in equilibrium from a vertical elastic string of natural length 0.8m0.8\,\text{m} and modulus 49N49\,\text{N}. Taking g=9.8m s2g=9.8\,\text{m s}^{-2}, determine the extension and the equilibrium length of the string.[4 marks]

    Answer

    • Extension 0.24m0.24\,\text{m}
    • Equilibrium length 1.04m1.04\,\text{m}

    Method: Equilibrium gives T=mg=1.5(9.8)=14.7NT=mg=1.5(9.8)=14.7\,\text{N}. Hooke's law gives 14.7=49x/0.814.7=49x/0.8, so x=0.24mx=0.24\,\text{m}. Adding the natural length gives 0.8+0.24=1.04m0.8+0.24=1.04\,\text{m}.

FM1-3.2 · Energy stored in an elastic string or spring.

  • A spring of constant kk stores elastic energy 12kx2\tfrac12kx^2 when extended or compressed by xx.
  • A taut elastic string of natural length ll and modulus λ\lambda stores energy λx2/(2l)\lambda x^2/(2l) at extension xx.
  • Elastic energy is the area under the tension-extension graph, so it is quadratic in extension rather than equal to final tension times extension.
  • In an energy equation, include elastic energy only while the string is taut, and measure extension from the natural length at each position.

Tier 1 · Easy

  1. 1. A spring of constant 200N m1200\,\text{N m}^{-1} is compressed by 0.08m0.08\,\text{m}. Calculate the elastic energy stored.[2 marks]

    Answer

    • 0.64J0.64\,\text{J}

    Method: E=12kx2=12(200)(0.08)2=0.64JE=\tfrac12kx^2=\tfrac12(200)(0.08)^2=0.64\,\text{J}.

Tier 2 · Standard

  1. 1. An elastic string has natural length 1.2m1.2\,\text{m} and modulus 60N60\,\text{N}. Find the energy stored when its length is 1.5m1.5\,\text{m}.[3 marks]

    Answer

    • 2.25J2.25\,\text{J}

    Method: The extension is x=1.51.2=0.3mx=1.5-1.2=0.3\,\text{m}. Thus E=λx2/(2l)=60(0.3)2/[2(1.2)]=2.25JE=\lambda x^2/(2l)=60(0.3)^2/[2(1.2)]=2.25\,\text{J}.

Tier 3 · Hard

  1. 1. A 2kg2\,\text{kg} particle is attached to the lower end of a vertical elastic string with natural length 1m1\,\text{m} and modulus 49N49\,\text{N}. It is released from rest when the string is at natural length. Taking g=9.8m s2g=9.8\,\text{m s}^{-2}, find its speed after descending 0.6m0.6\,\text{m}.[5 marks]

    Answer

    • 2.94m s11.71m s1\sqrt{2.94}\,\text{m s}^{-1}\approx1.71\,\text{m s}^{-1}

    Method: The loss of gravitational potential energy is 2(9.8)(0.6)=11.76J2(9.8)(0.6)=11.76\,\text{J}. At extension 0.6m0.6\,\text{m}, elastic energy is 49(0.6)2/[2(1)]=8.82J49(0.6)^2/[2(1)]=8.82\,\text{J}. Conservation of mechanical energy gives 11.76=12(2)v2+8.8211.76=\tfrac12(2)v^2+8.82, so v2=2.94v^2=2.94 and v=2.94m s1v=\sqrt{2.94}\,\text{m s}^{-1}.