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We will use both of the equations of motion to reach the third equation of motion. This will require a bit of algebra.
S=ut+ 1/2 at²
andv=u+at, include the time variant t
There will be some situations when we do not have any information about time and so it would be a good idea to derive an equation that does not have a t term.
To do this, we rearrange our first equation to get
t=(v−u)/a
and use this to replace t wherever it appears in the second equation. So
S=ut+ 1/2 at²
becomes,
S = u(v−u/a) + 1/2a (v - u/a) ²
2as = 2u(v - u) + ( v - u ) ²
⇒2aS = 2uv−2u² - v² - 2uv - u²
⇒2aS = v²- u²
⇒v2 = u² + 2aS
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