Step 1: Understanding Work Done:
Work done (\(W\)) by a force depends on the force applied and the displacement of the object along the direction of the force.
- If the force vector \(\vec{F}\) is constant and the displacement is \(\vec{d}\), then work done is \(W = \vec{F} \cdot \vec{d} = Fd\cos\phi\), where \(\phi\) is the angle between the force and displacement vectors.
- If the force is applied along a path, the work done is the integral of the force component along the path, \(W = \int \vec{F} \cdot d\vec{s}\).
Step 2: Calculating Work Done for Each Case:
The net displacement from A to B is a straight line of length \(d = 20\) m.
Case 1: The force F is applied tangentially along the semi-circular path AJB.
The length of the path is the circumference of the semi-circle, \(s = \pi r\). The radius is \(r = AB/2 = 20/2 = 10\) m.
So, path length \(s = \pi \times 10 = 10\pi\) m.
Since the force is always in the direction of motion, the work done is force \(\times\) distance.
\[ W_1 = F \times s = F \times 10\pi \approx 31.4 F \]
Case 2: The constant force F is applied horizontally, parallel to the displacement AB.
The displacement is \(d = 20\) m. The angle between force and displacement is \(\phi = 0^\circ\).
\[ W_2 = F \times d \times \cos(0^\circ) = F \times 20 \times 1 = 20 F \]
Case 3: The constant force F is applied at an angle \(\theta\) to the horizontal displacement AB.
The displacement is \(d = 20\) m. The angle between force and displacement is \(\theta\).
\[ W_3 = F \times d \times \cos\theta = F \times 20 \times \cos\theta \]
Given that \(0^\circ<\theta<90^\circ\), we know that \(0<\cos\theta<1\).
Therefore, \(W_3\) is less than \(20F\). For example, if \(\theta = 60^\circ\), \(W_3 = 20F \times 0.5 = 10F\).
Step 3: Comparing the Work Done:
We have:
- \(W_1 \approx 31.4 F\)
- \(W_2 = 20 F\)
- \(W_3 = (20 \cos\theta) F\), which is less than \(20F\).
Comparing the three values, we get: \(W_3<W_2<W_1\).
The ascending order is Case 3, Case 2, Case 1.