
To solve this problem, we need to calculate the maximum compression in the spring when the block hits it. We'll use energy conservation principles, factoring in gravitational potential energy, work done by friction, and spring potential energy.
Therefore, the maximum compression in the spring when the block hits the spring is \(2 \, \text{m}\).
Using the work-energy theorem, the total work done by all forces is equal to the change in kinetic energy (\(\Delta KE\)) of the system. Here:
\[w_g + w_{Fr} + w_s = \Delta KE.\]
Substituting the given values:
\[5 \times 10 \times 5 - 0.5 \times 5 \times 10 \times x - \frac{1}{2} Kx^2 = 0 - 0.\]
Simplifying:
\[250 - 25x - 50x^2 = 0.\]
Rewriting:
\[2x^2 + x - 10 = 0.\]
Solving this quadratic equation gives:
\[x = 2.\]
Thus, the maximum compression in the spring is \(x = 2\) m.

Potential energy (V) versus distance (x) is given by the graph. Rank various regions as per the magnitudes of the force (F) acting on a particle from high to low. 
In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
