A.3.8—Mechanical energy transformations
- Syllabus
- First assessment 2025
- Objective
- —
- Level
- SL
Conservative transformations
When mechanical energy is conserved, energy can move between translational kinetic, gravitational potential and elastic potential stores without changing their sum.
Use the endpoints
For a car descending a frictionless track, gravitational potential energy decreases while kinetic energy increases. For a spring system, elastic potential energy can become kinetic energy and then return.
Add non-conservative transfers
If friction or drag acts, part of the mechanical energy transfers to internal energy. The endpoint equation must include that loss from the mechanical stores.
[ 2 ]
Show that the speed of the car at P is 1.7 ms−1.
Account for energy
Define the system, identify energy stores and describe transfers. Work done by a force transfers energy; total energy is conserved even when mechanical energy is not.
Use the mechanical model
E_k=rac12mv^2,\quad \Delta E_{p,g}=mg\Delta h,\quad E_{p,elastic}=rac12k(\Delta x)^2
Conserve their sum only when resistive transfers are absent or included explicitly.
Use rates and ratios
P=rac{\Delta E}{\Delta t}=Fv,\qquad \eta=rac{E_{useful}}{E_{input}}=rac{P_{useful}}{P_{input}}
Fuel energy density connects available input energy to a chosen volume.
Final checks
Check the system boundary, signs of work and potential-energy changes, the reference height, extension from natural length, and whether the quantity is energy, power, efficiency or energy density.