Given the displacement equation:
\( x = c_0 (t^2 - 2) + c (t - 2)^2 \)
Expanding the equation yields:
\( x = c_0 t^2 - 2c_0 + c (t^2 - 4t + 4) \)
\( x = c_0 t^2 - 2c_0 + c t^2 - 4ct + 4c \)
\( x = (c_0 + c) t^2 - 4ct + (4c - 2c_0) \)
Velocity is found by differentiating the displacement with respect to time:
\( v = \frac{dx}{dt} = \frac{d}{dt} [(c_0 + c) t^2 - 4ct + (4c - 2c_0)] \)
\( v = 2(c_0 + c) t - 4c \)
Acceleration is found by differentiating the velocity with respect to time:
\( a = \frac{dv}{dt} = \frac{d}{dt} [2(c_0 + c) t - 4c] \)
\( a = 2(c_0 + c) \)
The particle's acceleration is \( 2(c_0 + c) \).
Therefore, 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 \( 2(c + c_0) \)
A bead P sliding on a frictionless semi-circular string... bead Q ejected... relation between $t_P$ and $t_Q$ is 