In Simple Harmonic Motion (SHM), the total mechanical energy is conserved and is equally distributed between the kinetic energy (\( K \)) and the potential energy (\( U \)) at any point in time. The total energy \( E \) of an object performing SHM is given by:
\[
E = K + U
\]
At any position during the SHM:
1. Kinetic Energy (\( K \)) is given by:
\[
K = \frac{1}{2} m v^2
\]
Where \( m \) is the mass of the object and \( v \) is its velocity at that position.
2. Potential Energy (\( U \)) is given by:
\[
U = \frac{1}{2} k x^2
\]
Where \( k \) is the spring constant and \( x \) is the displacement from the equilibrium position.
At extreme positions (when \( x = A \), the amplitude), the velocity is zero, so all the energy is stored as potential energy, and at the mean position (when \( x = 0 \)), all the energy is converted to kinetic energy.
Now, the average values of kinetic energy and potential energy over a complete cycle of SHM can be derived as:
- The average kinetic energy \( \langle K \rangle \) is:
\[
\langle K \rangle = \frac{1}{2} E
\]
- The average potential energy \( \langle U \rangle \) is:
\[
\langle U \rangle = \frac{1}{2} E
\]
Therefore, the ratio of average kinetic energy to average potential energy is:
\[
\frac{\langle K \rangle}{\langle U \rangle} = \frac{\frac{1}{2} E}{\frac{1}{2} E} = 1:1
\]
Thus, the ratio of the average kinetic energy to the average potential energy for an SHM is \( 1:1 \).