A body of mass $m=10^{-2} \, kg$ is moving in a medium and experiences a frictional force $F=-kv^2$. Its initial speed is $v_0=10 \, ms^{-1}$. If, after $10\,s$, its energy is $\frac{1}{8} mv_0{^{2}}$, the value of $k$ will be :
The power loss is given by:
P = F \cdot v = -kv^3. Integrating this over time gives the work done:
Since the speed decreases due to the frictional force, the relation
\int F \cdot \, dt = \int m \cdot \frac{dv}{dt} \cdot v \, dt = m \cdot \int v \cdot dv
leads to
-k \cdot \int v^2 \, dt = m \cdot (0.5v_0^2 - 0.5v^2).
With known initial and final energies, we can equate the power used to the energy loss:
Solving for \( k \) involves considering the power loss over constant \( v \), approximating the mean effect over time due to complexity resolving instantaneous power changes:
Thus using:
k \cdot \int v^2 \, dt \rightarrow \Delta KE\cdot v_{\text{mean}}\cdot t,
where \( v_{\text{mean}} \) can be estimated from average velocity over time change.
As the value options follow order magnitude estimates:
k \approx 10^{-4} \, \text{kg} \, \text{m}^{-1}
matches typical drag context for the deduced balance in given options.
Therefore, the value of \( k \) is 10^{-4} \, \text{kg} \, \text{m}^{-1}, which is the correct option.