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 \( 2(c + c_0) \)
To determine the correct statement about the particle's motion, we need to analyze the displacement equation given:
\(x = c_0 (t^2 - 2) + c (t - 2)^2\)
Let's proceed step-by-step to compute the velocity and acceleration of the particle:
\(v = \frac{dx}{dt} = \frac{d}{dt}[c_0 (t^2 - 2) + c (t - 2)^2]\)
\(= c_0 \cdot 2t + c \cdot 2(t - 2)\)
\(= 2c_0 t + 2c(t - 2)\)
\(= 2c_0 t + 2ct - 4c\)
\(= (2c_0 + 2c)t - 4c\)
\(a = \frac{dv}{dt} = \frac{d}{dt}[(2c_0 + 2c)t - 4c]\)
\(= 2c_0 + 2c\)
The acceleration of the particle is thus \(2(c_0 + c)\).
\(v_0 = (2c_0 + 2c)\cdot 0 - 4c = -4c\)
This confirms that the initial velocity is not \(4c\).
Thus, the correct statement is that the acceleration of the particle is \(2(c + c_0)\).
The motion of an airplane is represented by the velocity-time graph as shown below. The distance covered by the airplane in the first 30.5 seconds is km.

Which of the following curves possibly represent one-dimensional motion of a particle?
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: