Conservation of energy in SHM — kinetic and potential energy at any displacement

medium CBSE JEE-MAIN NEET JEE Main 2023 3 min read

Question

A particle of mass 0.5 kg executes SHM with amplitude 10 cm and angular frequency ω=20\omega = 20 rad/s. Find the kinetic energy and potential energy when the displacement is 6 cm from the mean position. Verify that total energy is conserved.

(JEE Main 2023, similar pattern)


Solution — Step by Step

For a particle executing SHM with amplitude AA and angular frequency ω\omega:

KE=12mω2(A2x2)KE = \frac{1}{2}m\omega^2(A^2 - x^2) PE=12mω2x2PE = \frac{1}{2}m\omega^2 x^2 Etotal=12mω2A2E_{\text{total}} = \frac{1}{2}m\omega^2 A^2

where xx is the displacement from the mean position.

Etotal=12×0.5×(20)2×(0.10)2E_{\text{total}} = \frac{1}{2} \times 0.5 \times (20)^2 \times (0.10)^2 =12×0.5×400×0.01=1.0 J= \frac{1}{2} \times 0.5 \times 400 \times 0.01 = \mathbf{1.0 \text{ J}} PE=12×0.5×400×(0.06)2=12×0.5×400×0.0036=0.36 JPE = \frac{1}{2} \times 0.5 \times 400 \times (0.06)^2 = \frac{1}{2} \times 0.5 \times 400 \times 0.0036 = \mathbf{0.36 \text{ J}} KE=12×0.5×400×[(0.10)2(0.06)2]KE = \frac{1}{2} \times 0.5 \times 400 \times [(0.10)^2 - (0.06)^2] =12×0.5×400×[0.010.0036]=12×0.5×400×0.0064=0.64 J= \frac{1}{2} \times 0.5 \times 400 \times [0.01 - 0.0036] = \frac{1}{2} \times 0.5 \times 400 \times 0.0064 = \mathbf{0.64 \text{ J}}

Verification: KE+PE=0.64+0.36=1.0KE + PE = 0.64 + 0.36 = 1.0 J =Etotal= E_{\text{total}}


Why This Works

In SHM, the restoring force is conservative (F=kx=mω2xF = -kx = -m\omega^2 x), so total mechanical energy is conserved. Energy continuously converts between kinetic and potential forms:

  • At mean position (x=0x = 0): KE is maximum, PE = 0
  • At extreme position (x=±Ax = \pm A): PE is maximum, KE = 0
  • At any intermediate point: both KE and PE are non-zero, but their sum equals EtotalE_{\text{total}}

The KE and PE are complementary — they add up to a constant. If you plot both against displacement, KE is an inverted parabola and PE is an upright parabola. They intersect at x=A/2x = A/\sqrt{2}, where KE = PE = Etotal/2E_{\text{total}}/2.


Alternative Method

Use the velocity formula directly:

v=ωA2x2=200.010.0036=200.0064=20×0.08=1.6 m/sv = \omega\sqrt{A^2 - x^2} = 20\sqrt{0.01 - 0.0036} = 20\sqrt{0.0064} = 20 \times 0.08 = 1.6 \text{ m/s} KE=12mv2=12×0.5×(1.6)2=0.64 JKE = \frac{1}{2}mv^2 = \frac{1}{2} \times 0.5 \times (1.6)^2 = 0.64 \text{ J} PE=EtotalKE=1.00.64=0.36 JPE = E_{\text{total}} - KE = 1.0 - 0.64 = 0.36 \text{ J}

Quick ratio trick: At displacement xx, the fraction of total energy that is PE = (x/A)2(x/A)^2 and the fraction that is KE = 1(x/A)21 - (x/A)^2. At x=6x = 6 cm, A=10A = 10 cm: PE fraction = (6/10)2=0.36(6/10)^2 = 0.36, KE fraction = 0.640.64. No need to calculate absolute values if the question only asks for the ratio.


Common Mistake

Students often use PE=mghPE = mgh for SHM problems. That formula applies only to gravitational potential energy. In SHM, the potential energy is 12kx2=12mω2x2\frac{1}{2}kx^2 = \frac{1}{2}m\omega^2 x^2 — it comes from the elastic restoring force. Unless the SHM is specifically a vertical spring (where gravity also contributes), always use the spring PE formula, not the gravitational one.

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