Part of ME-04 — Work, Energy & Power

Potential Energy and Energy Conservation

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Gravitational Potential Energy

PEg=mgh[M1L2T2] (J)PE_g = mgh \quad [\text{M}^1\text{L}^2\text{T}^{-2}]\ (\text{J})

  • h = height above chosen reference level
  • Reference level is arbitrary; only ΔP\Delta PE matters
  • For conservative forces: W=ΔPEW = -\Delta PE

Spring Potential Energy

PEs=12kx2[M1L2T2] (J)PE_s = \frac{1}{2}kx^2 \quad [\text{M}^1\text{L}^2\text{T}^{-2}]\ (\text{J})

  • Always ≥ 0 (whether stretched or compressed)
  • k = spring constant [M^{1}$$L^{0}$$T^{-2}] (N/m)
  • x = extension or compression (m)

Conservative vs. Non-Conservative Forces

PropertyConservativeNon-Conservative
Path dependenceIndependent of pathDepends on path
Closed loop workZeroNon-zero (negative)
PE can be definedYesNo
ExamplesGravity, springFriction, air resistance

Conservation of Mechanical Energy

When only conservative forces act: KE+PE=constant (total mechanical energy E)KE + PE = \text{constant (total mechanical energy E)}

When friction acts: Δ(KE+PE)=Wfriction=fkd<0\Delta(KE + PE) = W_{\text{friction}} = -f_k \cdot d < 0

The mechanical energy decreases by the heat generated by friction.

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