A.3.14—Fuel energy density
- Syllabus
- First assessment 2025
- Objective
- —
- Level
- SL
Energy per volume
For the current IB Physics definition, fuel energy density u is the transferable energy per unit volume:
u=VE
Its SI unit is Jm−3. This lets fuels be compared when storage volume is the constraint.
Connect it to a fuel flow
If fuel flows at volume rate V˙, its input power is Pin=uV˙. Apply efficiency only after finding the input energy or power.
Worked example from local Question Bank row 36970
An engine produces 20kW useful power at 50% efficiency while consuming 1.0×10−5m3s−1 of fuel.
Pin=0.5020kW=40kW
u=V˙Pin=1.0×10−54.0×104=4.0×109Jm−3=4.0GJm−3
Common trap
Specific energy is energy per unit mass, measured in Jkg−1. Some sources use the words loosely, so let the stated definition and units determine whether to divide by volume or mass.
[ 2 ]
At the end of the 30-day period, rockets are fired to bring the ISS back to its initial height. The energy density of liquid hydrogen rocket fuel is 8.5×103MJm−3.
Estimate the volume of fuel needed.
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.