Understanding the Concept:
According to the Work-Energy Theorem, the net work done by all forces acting on a system equals its net change in kinetic energy:
\[
W_{\text{spring}} + W_{\text{friction}} = \Delta K = K_{\text{final}} - K_{\text{initial}}
\]
The work done by a spring during compression is $-\frac{1}{2}kx^2$, and the work done by a uniform kinetic friction force over displacement $x$ is $-f_k \cdot x$.
Step 1: Set up the energy balance equation elements.
We are given:
Mass, $m = 1.5\text{ kg}$
Initial speed, $v = 5\text{ m s}^{-1}$
Spring constant, $k = 10000\text{ N m}^{-1}$
Compression distance, $x = 5\text{ cm} = 0.05\text{ m}$
Final speed, $v_f = 0\text{ m s}^{-1}$ (comes to rest)
Let's evaluate the initial kinetic energy:
\[
K_{\text{initial}} = \frac{1}{2} m v^2 = \frac{1}{2} \times 1.5 \times 5^2 = 0.75 \times 25 = 18.75\text{ J}
\]
Step 2: Calculate potential energy stored in the spring.
\[
U_{\text{spring}} = \frac{1}{2} k x^2 = \frac{1}{2} \times 10000 \times (0.05)^2 = 5000 \times 0.0025 = 12.5\text{ J}
\]
Step 3: Apply the work-energy balance to solve for friction force ($f_k$).
\[
-\frac{1}{2}kx^2 - f_k \cdot x = 0 - K_{\text{initial}}
\]
\[
-12.5 - f_k \cdot (0.05) = -18.75
\]
Rearranging terms:
\[
f_k \cdot (0.05) = 18.75 - 12.5 = 6.25
\]
\[
f_k = \frac{6.25}{0.05} = 125\text{ N}
\]