State and prove work energy theorem for constant force


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State and prove work energy theorem by constant force

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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


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