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when it's okay and when it's not okay.
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What this means is, in a time Δt,
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this quantity changes by some amount,
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and in the same time, Δt,
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that quantity changes by some amount,
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then keeping the Δt equal to some number
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we may equate the changes of the two quantities,
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provided it is understood
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that Δ(v^(2)) is a change in v^ over 2
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in the same time in which the particle moved a distance, Δx.
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Adding the differences,
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we eliminate time and we get this final result.