The position of the particle is given by the function $s(t) = \alpha t^2 - \beta t + \gamma$. The provided constants are $\alpha = 1\text{ ms}^{-2}$, $\beta = 6\text{ ms}^{-1}$, and $\gamma = 5\text{ m}$.
First, find the position at the start time, $t = 0\text{ s}$:
$s(0) = (1)(0)^2 - (6)(0) + 5 = 5\text{ m}$
Next, find the position at the end time, $t = 6\text{ s}$:
$s(6) = (1)(6)^2 - (6)(6) + 5 = 36 - 36 + 5 = 5\text{ m}$
To determine the total distance traveled, we need to check if the particle changed direction. This occurs when the velocity, $v(t)$, is zero.
The velocity function is the derivative of the position function:
$v(t) = s'(t) = \frac{d}{dt}(\alpha t^2 - \beta t + \gamma) = 2\alpha t - \beta$
Substitute the values for $\alpha$ and $\beta$:
$v(t) = 2(1)t - 6 = 2t - 6\text{ ms}^{-1}$
Set the velocity to zero to find the time(s) of direction change:
$2t - 6 = 0 \implies 2t = 6 \implies t = 3\text{ s}$
Since $t = 3\text{ s}$ falls within the interval $[0, 6\text{ s}]$, the particle does change direction.
Calculate the position at the time of direction change, $t = 3\text{ s}$:
$s(3) = (1)(3)^2 - (6)(3) + 5 = 9 - 18 + 5 = -4\text{ m}$
Now, calculate the distance traveled during each part of the motion:
The total distance traveled is the sum of these distances:
$ \text{Total Distance} = 9\text{ m} + 9\text{ m} = 18\text{ m} $
The total time elapsed is $T = 6\text{ s} - 0\text{ s} = 6\text{ s}$.
Average speed is defined as the total distance traveled divided by the total time taken:
$ \text{Average Speed} = \frac{\text{Total Distance}}{\text{Total Time}} = \frac{18\text{ m}}{6\text{ s}} = 3\text{ ms}^{-1} $
Therefore, the average speed of the particle is $3\text{ ms}^{-1}$.
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Bob B of mass $m$ at rest is hanging vertically from the ceiling via a massless string of length $10\text{ m}$, as shown in the figure. Point mass A of mass $m$ travelling horizontally with speed $10\text{ ms}^{-1}$ hits bob B elastically. The bob B rises $h$ meter after the collision. Taking the acceleration due to gravity $g = 10\text{ ms}^{-2}$ and neglecting the size of the bob, the value of $h$ is :
A thin horizontal disc is rotating about a vertical axis passing through its fixed centre O. Its angular momentum is $L_A$ and $L_B$ computed about points A and B, respectively, with $OB = 2 \times OA$. The value of $\frac{L_A}{L_B}$ is :
Two circular discs of radius each $10 \text{ cm}$ are joined at their centres by a rod of length $30 \text{ cm}$ and mass $600 \text{ gm}$ as shown in figure.
If the mass of each disc is $600 \text{ gm}$ and applied torque between two discs is $43 \times 10^5 \text{ dyne.cm}$, the angular acceleration of the discs about the given axis $AB$ is________$\text{rad/s}^2$.
