Calculate the Velocity Components:
For \(x = 2 + 4t\):
\[ \frac{dx}{dt} = v_x = 4 \]For \(y = 3t + 8t^2\):
\[ \frac{dy}{dt} = v_y = 3 + 16t \]Calculate the Acceleration Components:
The acceleration in the \(x\)-direction \(a_x\) is:
\[ \frac{d^2x}{dt^2} = a_x = 0 \]The acceleration in the \(y\)-direction \(a_y\) is:
\[ \frac{d^2y}{dt^2} = a_y = 16 \]Therefore, the particle has a constant acceleration \(a_y = 16\, \text{m/s}^2\) in the \(y\)-direction, and no acceleration in the \(x\)-direction.
Determine the Path of Motion:
To find the path of the particle, express \(y\) in terms of \(x\) by eliminating \(t\) between the two equations.
From \(x = 2 + 4t\), we get:
\[ t = \frac{x - 2}{4} \]Substitute this into the equation for \(y\):
\[ y = 3\left(\frac{x - 2}{4}\right) + 8\left(\frac{x - 2}{4}\right)^2 \]Simplifying, we get:
\[ y = \frac{3}{4}(x - 2) + 8 \times \frac{(x - 2)^2}{16} \] \[ y = \frac{3}{4}(x - 2) + \frac{1}{2}(x - 2)^2 \]This equation is quadratic in \(x\), indicating that the path of the particle is a parabola.
Conclusion:
The motion of the particle is uniformly accelerated with a parabolic path, which corresponds to Option (4).
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: