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55 ideas · 9 connections
Spring force and elastic energy Work transfers energy into a spring Work, energy and power3.3 Work and conservation of energy3.3.1 Kinetic and potential energies3.3.2 Power3.3.3 Springs3.4.1 Elastic potential energy
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Physics connection

Work transfers energy into a spring

OCR A AS Physics · Two ideas, one explanation

Work is an energy transfer. Loading a spring transfers energy mechanically, which can later become kinetic energy or be dissipated.

Work input = stored energy + dissipated energy

Follow the reasoning

  1. Define the system and its initial and final states.
  2. Calculate the work transferred to the spring.
  3. Account for friction or other losses before equating stored energy to kinetic energy.
Specification outcomes (4)
  • 3.3.1(a) Define work done by a force and the unit joule.
  • 3.3.1(b) Use W = F x cos θ for work done by a force.
  • 3.4.2(a) Interpret force–extension (or compression) graphs; calculate work done as area under graph.
  • 3.4.2(b) Calculate elastic potential energy using E = ½Fx or E = ½kx².
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H156 v2.0 · May 2026

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PhysicsUK Solve15 marks

A technician calibrates the spring bumper of a small instrument trolley. Figure 1 shows the force F needed to compress the spring by x from its natural length. The graph is a straight line through (0, 0), (0.020 m, 1.2 N), (0.040 m, 2.4 N) and (0.060 m, 3.6 N). The trolley has mass 0.60 kg. It is released from rest against the spring at compression 0.060 m on a horizontal track. A constant resistive force of 0.60 N opposes the motion as soon as the trolley moves. The spring's mass is negligible and its deformation is elastic. The trolley loses contact with the spring at its natural length. There are no other energy losses. (a) Use the gradient of the force-compression graph to determine the spring constant. [2] (b) Use the graph to calculate the work needed to compress the spring from its natural length to 0.060 m. [2] (c) Calculate the acceleration just after release, stating its direction relative to the bumper. [3] (d) Calculate the speed when the trolley loses contact with the spring. Account for the work done against resistance. [3] (e) Explain why a single constant-acceleration equation cannot describe the whole interval while the trolley is in contact with the spring. [2] (f) Calculate the distance travelled after losing contact before the trolley stops. Use a constant-acceleration equation for this part. [3]

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