The work-energy theorem states that work done equals the change in kinetic energy:
\[
W = \Delta K = \frac{1}{2} m v_{\text{initial}}^2 - \frac{1}{2} m v_{\text{final}}^2
\]
Given:
- \( m = 10 \, \text{kg} \) (mass)
- \( v_{\text{initial}} = 4 \, \text{m/s} \) (initial velocity)
- \( v_{\text{final}} = 0 \, \text{m/s} \) (final velocity, as the body stops).
Calculate the work done:
\[
W = \frac{1}{2} \times 10 \times (4^2 - 0^2)
\]
\[
W = 5 \times 16 = 80 \, \text{J}
\]
The work performed by the force is \( 80 \, \text{J} \).