The displacement equation of simple harmonic motion obtained by combining the motions is the result of vector addition of the displacements.
We first need to sum the two displacements:
The displacements \( x_1 \) and \( x_3 \) have the same phase and can be added directly:
\[
x_1 + x_3 = 2 \sin(\omega t) + 6 \sin(\omega t) = 8 \sin(\omega t)
\]
Next, \( x_2 \) has a phase shift of \( \frac{\pi}{2} \), and we use the trigonometric identity to combine it with the sum of the other two:
\[
x_2 = 4 \sin(\omega t + \frac{\pi}{2}) = 4 \cos(\omega t)
\]
Now, we combine \( 8 \sin(\omega t) \) and \( 4 \cos(\omega t) \) using the trigonometric identity:
\[
R \sin(\omega t + \phi) = \sqrt{8^2 + 4^2} \sin(\omega t + \phi) = 8.944 \sin(\omega t + \phi)
\]
The combined displacement is approximately:
\[
x = 11.25 \sin(\omega t + \phi)
\]
Thus, the correct answer is (c).