Three constant-force pushes close the loop from work input to final kinetic energy.
Example
Three constant-force pushes close the loop from work input to final kinetic energy. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.
highlighted = computed this step
Audit work against final speed
Start from rest and push in the direction of motion with the same force each time. Work added by the push must equal the final kinetic energy.
Fd=ΔKE=21mv2
First push closes
The 4 N push over 4 m adds 16 J. That is exactly the kinetic energy of 4 m/s.
Fd=4N⋅4m=16J=212kg(4m/s)2=16J
Second push closes
Over 9 m, the same force adds 36 J. The final speed 6 m/s gives the matching kinetic energy.
Fd=4N⋅9m=36J=212kg(6m/s)2=36J
Third push closes
Over 16 m, the same force adds 64 J. The final speed 8 m/s closes the largest row.
Fd=4N⋅16m=64J=212kg(8m/s)2=64J
Work and kinetic energy agree row by row
The distance column controls the work because the force is fixed. The speed column is accepted only when its kinetic energy equals that work.
d4m9m16mW16J36J64Jv4m/s6m/s8m/sKE16J36J64J
mechanicsWith the force and mass fixed, the push distance sets the work, and the final speed must make exactly the same kinetic energy.