91Ó°ÊÓ

Mass of the block,$m=2.5\mathrm{kg}$

Spring constant,$\mathrm{k}=320\mathrm{N}/\mathrm{m}$

Spring is compressed by distance, x = 7.5 cm

Coefficient of kinetic friction between block and floor,$\mathrm{μ}=0.25$

The block with initial kinetic energy strikes the spring and compresses it. This converts the kinetic energy of the block to the potential energy of the spring. But since there is friction between the block and the floor, some energy is lost as thermal energy. Thus, we have to apply the conservation of energy principle to study the system.

Formulae:

The kinetic energy of the body in motion,$KE=\frac{1}{2}m{v}^2$

The potential energy of a body in motion,$PE=\frac{1}{2}k{x}^2$

Thermal energy of the system due to frictional force,$E_{th}\left(W\right)=F_{f}x$

The frictional force acting on a body, $F_f={\mathrm{μ}}_{k}N={\mathrm{μ}}_{k}mg$

Using thework energy theorem, the work done by the spring = change in the energy of the spring. Thus, the work done by the spring is given: (negative as it is case of compression)

$$\begin{gathered} W=\frac{1}{2}k{x}^2 \\ W=-\frac{1}{2}×320×{\left(0.075\right)}^2 \\ =-0.90\mathrm{J} \end{gathered}$$

Hence, the value of the work is -0.90 J.

The increase in thermal energy of the block –floor system occurs because of the friction between the block and the floor surface. Thus, the thermal energy of the system can be given:

$$\begin{gathered} KE\left(block\right)=PE\left(spring\right)+E_{th} \\ \frac{1}{2}m{v}^2=0.90+0.46 \\ =1.36 \\ {v}^2=\frac{1.36×2}{2.5} \\ =1.09 \\ v=1.0\mathrm{m}/\mathrm{s} \end{gathered}$$

Hence, the value of the thermal energy is 1.0 m/s

Now, for getting the speed of the block, we use the conservation of energy principle,

$$\begin{gathered} \mathrm{KE}\left(\mathrm{block}\right)=\mathrm{PE}\left(\mathrm{spring}\right)+{\mathrm{E}}_{\mathrm{th}} \\ \frac{1}{2}{\mathrm{mv}}^2=0.90+0.46 \\ {\mathrm{v}}^2=\frac{1.36×2}{2.5} \\ =1.09 \\ \mathrm{v}=1.0\mathrm{m}/\mathrm{s} \end{gathered}$$

Hence, the speed of the block is 1.0 m/s .