The work performed by a force is calculated as the dot product of the force vector and the displacement vector: \( W = \vec{F} \cdot \vec{d} = F d \cos\theta \).
Given values are:
- \( F = 20 \, \text{N} \) (magnitude of the applied force),
- \( d = 10 \, \text{m} \) (displacement),
- \( \theta = 30^\circ \) (the angle between the applied force and the horizontal displacement).
The horizontal component of the applied force is:
\[ F_x = F \cos\theta = 20 \cos 30^\circ \]
Since \( \cos 30^\circ = \frac{\sqrt{3}}{2} \approx 0.866 \), the horizontal force component is:
\[ F_x = 20 \times 0.866 \approx 17.32 \, \text{N} \]
The work done by the applied force is then:
\[ W = F_x \cdot d = 17.32 \times 10 = 173.2 \, \text{J} \]
Alternatively, applying the direct formula:
\[ W = F d \cos\theta = 20 \times 10 \times \cos 30^\circ = 200 \times 0.866 \approx 173.2 \, \text{J} \]
The work done by the applied force is \( 173.2 \, \text{J} \). Frictional or normal forces are not relevant for this specific calculation of work done by the applied force.