Step 1: Understanding the Concept:
The problem describes the superposition of two perpendicular simple harmonic motions (SHMs) with different frequencies. The path traced by the particle under this combined motion is known as a Lissajous figure. To determine the shape of the path, we need to eliminate the time variable (\(t\)) from the given parametric equations. Let's assign the motions to the x and y axes, for example, \(x(t) = y_2\) and \(y(t) = y_1\).
Step 2: Key Formula or Approach:
The parametric equations of the motion are:
\[ x(t) = b \cos(\omega t + \phi) \]
\[ y(t) = a \cos(2\omega t) \]
We are given the phase \(\phi = \pi\). We will use trigonometric identities to eliminate \(t\). The relevant identity is the double-angle formula: \(\cos(2\theta) = 2\cos^2(\theta) - 1\).
Step 3: Detailed Explanation:
1. Write down the parametric equations with the given phase:
Let the orthogonal motions be along the x and y axes.
\[ x = b \cos(\omega t + \pi) \]
\[ y = a \cos(2\omega t) \]
2. Simplify the equation for x:
Using the identity \(\cos(\theta + \pi) = -\cos(\theta)\), the x-equation becomes:
\[ x = -b \cos(\omega t) \]
3. Eliminate the time variable \(t\):
From the simplified x-equation, we can express \(\cos(\omega t)\) in terms of \(x\):
\[ \cos(\omega t) = -\frac{x}{b} \]
Now, use the double-angle identity for the y-equation:
\[ y = a \cos(2\omega t) = a (2\cos^2(\omega t) - 1) \]
Substitute the expression for \(\cos(\omega t)\) into the y-equation:
\[ y = a \left[ 2 \left(-\frac{x}{b}\right)^2 - 1 \right] \]
\[ y = a \left( \frac{2x^2}{b^2} - 1 \right) \]
4. Identify the shape of the curve:
Rearranging the equation, we get:
\[ y = \left(\frac{2a}{b^2}\right)x^2 - a \]
This equation is of the form \(y = kx^2 + c\), where \(k = \frac{2a}{b^2}\) and \(c = -a\) are constants. This is the standard equation of a parabola that opens vertically.
Step 4: Final Answer:
The equation relating y and x is \(y = (\frac{2a}{b^2})x^2 - a\), which represents a parabola. Therefore, option (A) is correct.