Given the displacement equation:
\( x = c_0 (t^2 - 2) + c (t - 2)^2 \)
We can expand this:
\( x = c_0 t^2 - 2c_0 + c (t^2 - 4t + 4) \)
\( x = c_0 t^2 - 2c_0 + c t^2 - 4ct + 4c \)
\( x = (c_0 + c) t^2 - 4ct + (4c - 2c_0) \)
To find the velocity, we differentiate the displacement equation with respect to time:
\( v = \frac{dx}{dt} = \frac{d}{dt} [(c_0 + c) t^2 - 4ct + (4c - 2c_0)] \)
\( v = 2(c_0 + c) t - 4c \)
To find the acceleration, we differentiate the velocity equation with respect to time:
\( a = \frac{dv}{dt} = \frac{d}{dt} [2(c_0 + c) t - 4c] \)
\( a = 2(c_0 + c) \)
The acceleration of the particle is \( 2(c_0 + c) \).
Thus, the correct statement is:
the acceleration of the particle is \( 2(c + c_0) \)
Final Answer: The final answer is the acceleration of the particle is \( 2(c + c_0) \)
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: