Concept:
The superposition of two simple harmonic motions at right angles to each other, having the same frequency but different amplitudes and phases, is a classic problem in the study of Lissajous figures.
Step 1: Express the motion equations.
The given equations are:
$$ x = A \sin(\omega t) \implies \frac{x}{A} = \sin(\omega t) $$
$$ y = B \cos(\omega t) \implies \frac{y}{B} = \cos(\omega t) $$
Step 2: Eliminate time to find the path.
We use the fundamental trigonometric identity \(\sin^2 \theta + \cos^2 \theta = 1\):
$$ \left( \frac{x}{A} \right)^2 + \left( \frac{y}{B} \right)^2 = \sin^2(\omega t) + \cos^2(\omega t) $$
$$ \frac{x^2}{A^2} + \frac{y^2}{B^2} = 1 $$
Step 3: Identify the curve.
This is the standard equation of an ellipse centered at the origin. Since \( A \neq B \), the semi-major and semi-minor axes are unequal, resulting in an ellipse. If \( A = B \), the path would reduce to a circular path.
$$\boxed{\text{Elliptical path}}$$