The acceleration of a particle which moves along the positive \( x \)-axis varies with its position as shown in the figure. If the velocity of the particle is \( 0.8 \, \text{m/s} \) at \( x = 0 \), then its velocity at \( x = 1.4 \, \text{m} \) is:
The velocity of the particle can be found using the work-energy theorem, which relates the change in velocity to the area under the acceleration versus position curve.
Given that the velocity at \( x = 0 \) is \( 0.8 \, \text{m/s} \), and from the graph, the area under the curve between \( x = 0 \) and \( x = 1.4 \) is the work done,
which contributes to the change in velocity.
From the graph, we can estimate the area, which leads to a velocity of \( 1.2 \, \text{m/s} \) at \( x = 1.4 \).
Thus, the velocity at \( x = 1.4 \, \text{m} \) is: \[ \boxed{1.2 \, \text{m/s}} \]
The range of the real valued function \( f(x) =\) \(\sin^{-1} \left( \frac{1 + x^2}{2x} \right)\) \(+ \cos^{-1} \left( \frac{2x}{1 + x^2} \right)\) is:
If \(3A = \begin{bmatrix} 1 & 2 & 2 \\[0.3em] 2 & 1 & -2 \\[0.3em] a & 2 & b \end{bmatrix}\) and \(AA^T = I\), then\(\frac{a}{b} + \frac{b}{a} =\):
\(\begin{vmatrix} a+b+2c & a & b \\[0.3em] c & b+c+2c & b \\[0.3em] c & a & c+a2b \end{vmatrix}\)