To solve this problem, we need to find the distance covered by the block before it comes to rest using the given parameters: mass of the block \(m = 10 \, \text{kg}\), initial velocity \(u = 9.8 \, \text{ms}^{-1}\), coefficient of friction \(\mu = 0.5\), and acceleration due to gravity \(g = 9.8 \, \text{ms}^{-2}\).
The force of friction \((f)\span> acting on the block can be calculated using the formula:\)
\(f = \mu \cdot N\),
where \(N\) is the normal force, which equals the weight of the block since the block is sliding on a horizontal surface. Thus, \(N = m \cdot g = 10 \cdot 9.8 = 98 \, \text{N}\).
Substituting the values, we get:
\(f = 0.5 \times 98 = 49 \, \text{N}\).
This frictional force causes a deceleration \((a)\span>, which can be found using Newton’s second law:\)
\(f = m \cdot a\)
\(49 = 10 \cdot a\)
\(a = 4.9 \, \text{ms}^{-2}\) (negative because it is deceleration).
We use the kinematic equation to find the distance \((s)\) the block travels before coming to rest:
\(v^2 = u^2 + 2as\).
Given that the final velocity \(v = 0 \, \text{ms}^{-1}\) when the block comes to rest, we have:
\(0 = (9.8)^2 + 2(-4.9)s\).
We solve for \(s\):
\(0 = 96.04 - 9.8s\)
\(9.8s = 96.04\)
\(s = \frac{96.04}{9.8} = 9.8 \, \text{m}\).
Therefore, the block covers a distance of 9.8 meters before coming to rest. Thus, the correct answer is 9.8 m.


Find the value of m if \(M = 10\) \(kg\). All the surfaces are rough.
A non-uniform bar of weight W is suspended at rest by two strings of negligible weight as shown in Fig.6.33. The angles made by the strings with the vertical are 36.9° and 53.1° respectively. The bar is 2 m long. Calculate the distance d of the centre of gravity of the bar from its left end.
