C1-3. SHM Dynamics and Energy
1. Energy Changes in SHM
In an undamped oscillator, energy transfers seamlessly between Kinetic ($E_K$) and Potential ($E_P$) energy. Total Energy ($E_T$) remains perfectly constant.
Energy Equations:HL Only
$$E_K = \dfrac{1}{2} m \omega^2 (x_0^2 - x^2)$$
$$E_T = \dfrac{1}{2} m \omega^2 x_0^2$$
Simple Pendulum: $x, v, a, E_T, E_P$, and $E_K$ vs. $t$ Example
Horizontal Spring System: $x, v, a$, and $E_T$ vs. $t$ Example
Example 1
How does the period of the kinetic energy oscillation ($T_{KE}$) compare to the period of the oscillating mass ($T$)?
Solution:
- In a single mechanical cycle, the mass passes the center (maximum speed and max $E_K$) twice—once moving left, once moving right.
- Therefore, the kinetic energy peaks twice per cycle. The frequency of energy oscillation is double the mechanical frequency ($f_{energy} = 2f$).
- Conclusion: Since frequency is doubled, the period is halved. $\mathbf{T_{KE} = \dfrac{1}{2}T}$.
Example 2
Problem: A particle oscillates with SHM of period $T$. Which graph shows the variation with time of the kinetic energy of the particle?
Solution:
Graph B is correct. Since kinetic energy must remain strictly positive (it relies on $v^2$) and completes exactly two full cycles within one standard mechanical period ($T$), option B perfectly satisfies the required conditions.