state and prove work energy theorem by constant force
Answers
Answered by
96
From Newton’s Second Law of motion, we know that F = ma, and because of the definition of acceleration we can say that

If we multiply both sides by the same thing, we haven’t changed anything, so we multiply by v:

But remember that v = dx/dt:

We rearrange and integrate:
F dx = mv dv

Fx = m(½v2) = ½mv2 = Ek
But Fx = Work; therefore Work = ΔEk

If we multiply both sides by the same thing, we haven’t changed anything, so we multiply by v:

But remember that v = dx/dt:

We rearrange and integrate:
F dx = mv dv

Fx = m(½v2) = ½mv2 = Ek
But Fx = Work; therefore Work = ΔEk
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Answered by
62
Answer:
suppose a constant force F acting on a body of mass m produces accelaration 'a' in it. After covering distance 's', suppose the velocity of the body changes from u 2 v.
Explanation:
The equation v^2-u^2=2as------- 1
multiplying both side with 1/2m we get---
1/2mv^2-1/2mu^2=mas---2
now from F=ma
1/2mv^2-1/2mu^2=Fs
1/2mv^2-1/2mu^2=W
=Kf-ki=W
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