Introduction to Energy in Simple Harmonic Motion
Simple Harmonic Motion (SHM) is one of the most fundamental and elegant concepts in physics.
When a particle undergoes SHM, energy continuously transitions between kinetic energy (K) and potential energy (U).
In an ideal, frictionless system, the Total Mechanical Energy (E) remains constant throughout the motion.
However, a common misconception among students is that the potential energy must always be zero at the mean position.
This problem beautifully highlights how a non-zero reference potential energy affects the overall energy landscape of a harmonic oscillator.
---
Analyzing the Setup
We are given the following parameters for a linear harmonic oscillator:
- Force constant, k=2×106 N/m
- Amplitude of oscillation, A=0.01 m
- Total mechanical energy, E=160 J
Let's first calculate the energy associated purely with the oscillation itself.
This is the energy required to stretch or compress the spring to its maximum amplitude A relative to the equilibrium position.
Substituting the given values:
Eosc=21×(2×106 N/m)×(0.01 m)2
This 100 J represents the dynamic energy of the oscillation.
It is the maximum kinetic energy the particle can achieve, and it is also the maximum potential energy measured relative to the minimum potential energy.
---
Finding the Maximum Kinetic Energy
At the mean position (x=0), the potential energy of the oscillator is at its minimum value (Umin), and the kinetic energy reaches its maximum value (Kmax).
Since the dynamic oscillation energy is entirely converted into kinetic energy at the mean position:
This directly confirms that Option (b) is correct.
---
Determining the Potential Energy Limits
Now, let's address the potential energy.
The total mechanical energy is the sum of kinetic and potential energy at any point:
At the mean position (x=0):
- Kinetic energy is maximum: Kmax=100 J
- Potential energy is minimum: Umin
Using the conservation of energy:
This tells us that the potential energy does not drop to zero at the mean position; instead, it has a baseline value of 60 J.
Therefore, Option (d) is incorrect.
At the extreme positions (x=±A):
- The particle momentarily comes to rest, so kinetic energy is zero: K=0
- Potential energy reaches its maximum value: Umax
Using the conservation of energy again:
This confirms that Option (c) is correct, while Option (a) is incorrect.
---
Summary of Results
By carefully separating the total mechanical energy into its baseline potential energy and dynamic oscillation energy, we have determined:
1. Maximum Kinetic Energy = 100 J (Option b)
2. Maximum Potential Energy = 160 J (Option c)
3. Minimum Potential Energy = 60 J
Thus, the correct options are (b) and (c).