CHAPTER 21. MOTION IN ONE DIMENSION 21.7
~a=∆t~v
where∆~vis the change in velocity, i.e.∆v=~vf-~vi. Thus we have
~a = ~vf−t~vi
~vf = ~vi+~at
Derivation of 21.2
We have seen that displacement can be calculated from the area under a velocity vs. time
graph. Foruniformly accelerated motionthe most complicated velocity vs. time graph we
can have is a straight line. Look at the graph below - it represents an object with a starting
velocity of~vi, accelerating to a final velocity~vfover a total timet.
~v(m·s−^1 )
t(s)
~vi
~vf
t
To calculate the final displacement we must calculate the area under the graph - this is just
the area of the rectangle added to the area of the triangle. This portion of the graph has
been shaded for clarity.
Area△ =^12 b×h
=^12 t×(vf−vi)
=^12 vft−^12 vit
Area = ℓ×b
= t×vi
= vit
Physics: Mechanics 431