How to drive the 3rd equation of motion?
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hey mate! here ur answer:)Third Equation
v2 = u2 + 2aS
where,
v = final velocity,
S = displacement,
u = initial velocity,
a = acceleration (must be constant),
This equation DOES NOT relate to final velocity.
Analytical Proof
We know that,
a = dvdt
v = dSdt
Taking their ratio, we get,
av = dvdS
Hence,
a = vdvdS
Cross multiplying ‘dS’ and integrating both sides,
S∫0 a . dS = v∫u v . dv ⇒ aS = v2 - u22
v2 = u2 + 2aS
Graphical Proof
Following is a v − t graph displaying constant acceleration. (Slope of the curve is constant)

At t = 0 seconds, the particle’s velocity is u m/s.
At t = t seconds, the particle’s velocity is v m/s.
Area under the curve of v − t graph gives displacement.
Now,
S = Area of Rectangle + Area of Triangle
S = ut + 12(v - u)(t)
(Substituting t = (v - u)a, from first equation of motion)
S = u(v - ua) + 12(v - u)(v - ua)
Rearranging the terms,
v2 = u2 + 2aS
hope it helps☺
please mark me as brainlist
v2 = u2 + 2aS
where,
v = final velocity,
S = displacement,
u = initial velocity,
a = acceleration (must be constant),
This equation DOES NOT relate to final velocity.
Analytical Proof
We know that,
a = dvdt
v = dSdt
Taking their ratio, we get,
av = dvdS
Hence,
a = vdvdS
Cross multiplying ‘dS’ and integrating both sides,
S∫0 a . dS = v∫u v . dv ⇒ aS = v2 - u22
v2 = u2 + 2aS
Graphical Proof
Following is a v − t graph displaying constant acceleration. (Slope of the curve is constant)

At t = 0 seconds, the particle’s velocity is u m/s.
At t = t seconds, the particle’s velocity is v m/s.
Area under the curve of v − t graph gives displacement.
Now,
S = Area of Rectangle + Area of Triangle
S = ut + 12(v - u)(t)
(Substituting t = (v - u)a, from first equation of motion)
S = u(v - ua) + 12(v - u)(v - ua)
Rearranging the terms,
v2 = u2 + 2aS
hope it helps☺
please mark me as brainlist
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