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Exercise · Q13

Q.Starting from the work-energy theorem and the definition of potential energy, show that the total mechanical energy of a system remains constant whenever only conservative forces act on it.

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Two results are combined here. First, the work-energy theorem (proved in general in Exercise 2 above) states that the net work done on a body always equals the change in its kinetic energy: Wnet=ΔK=Kf−KiW_{\text{net}} = \Delta K = K_f - K_i This holds for any net force, conservative or not.

Second, the definition of potential energy for a conservative force states that the work done by that force equals the negative of the change in potential energy it is associated with: Wconservative=−ΔU=−(Uf−Ui)W_{\text{conservative}} = -\Delta U = -(U_f - U_i)

Now suppose only conservative forces act on the body, so that Wnet=WconservativeW_{\text{net}} = W_{\text{conservative}}. Setting the two expressions for this same quantity equal to each other: ΔK=−ΔU\Delta K = -\Delta U Kf−Ki=−(Uf−Ui)K_f - K_i = -(U_f - U_i) Rearranging so all the "final" and "initial" terms are grouped together: Kf+Uf=Ki+UiK_f + U_f = K_i + U_i …

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