In simple harmonic motion (SHM), the total mechanical energy \( E \) is the sum of the kinetic energy \( K \) and the potential energy \( U \):
\[
E = K + U
\]
For SHM, the total energy is constant and is given by:
\[
E = \frac{1}{2} m \omega^2 A^2
\]
where \( A \) is the amplitude of oscillation. The kinetic energy and potential energy vary as functions of the displacement \( x \).
- At the maximum displacement (when \( x = \pm A \)), the potential energy is maximum, and the kinetic energy is zero.
- At the equilibrium position (when \( x = 0 \)), the kinetic energy is maximum, and the potential energy is zero.
The point where the kinetic energy is equal to the potential energy occurs when:
\[
K = U
\]
Since \( K + U = E \), at this point:
\[
K = U = \frac{E}{2}
\]
This condition occurs at \( x = \frac{A}{\sqrt{2}} \), which is the displacement where the kinetic and potential energies are equal.
Thus, the correct value of \( x_3 \) is:
\[
\frac{A}{\sqrt{2}}
\]