Step 1: Define the force vector and the work integral.
The given force vector is:
F ⃗ = α y i ^ + 2 α x j ^ \vec{F} = \alpha y\hat{i} + 2\alpha x\hat{j} F = α y i ^ + 2 α x j ^
Substituting α = − 1 N m − 1 \alpha = -1\,\text{N}\,\text{m}^{-1} α = − 1 N m − 1 yields:
F ⃗ = − y i ^ − 2 x j ^ \vec{F} = -y\hat{i} - 2x\hat{j} F = − y i ^ − 2 x j ^
The total work done along the closed path is:
W = ∮ F ⃗ ⋅ d r ⃗ W = \oint \vec{F} \cdot d\vec{r} W = ∮ F ⋅ d r
W = ∮ ( − y d x − 2 x d y ) W = \oint (-y\,dx - 2x\,dy) W = ∮ ( − y d x − 2 x d y )
Step 2: Calculate the work done along each segment.
The closed path consists of six segments: A B AB A B , B C BC B C , C D CD C D , D E DE D E , E F EF E F , and F A FA F A .
For segment A B AB A B from ( 0 , 1 ) (0, 1) ( 0 , 1 ) to ( 1 , 1 ) (1, 1) ( 1 , 1 ) , y = 1 y = 1 y = 1 and d y = 0 dy = 0 d y = 0 :
W A B = ∫ 0 1 − 1 d x = − 1 J W_{AB} = \int_{0}^{1} -1\,dx = -1\,\text{J} W A B = ∫ 0 1 − 1 d x = − 1 J
For segment B C BC B C from ( 1 , 1 ) (1, 1) ( 1 , 1 ) to ( 1 , 0.5 ) (1, 0.5) ( 1 , 0.5 ) , x = 1 x = 1 x = 1 and d x = 0 dx = 0 d x = 0 :
W B C = ∫ 1 0.5 − 2 ( 1 ) d y = 1 J W_{BC} = \int_{1}^{0.5} -2(1)\,dy = 1\,\text{J} W B C = ∫ 1 0.5 − 2 ( 1 ) d y = 1 J
For segment C D CD C D from ( 1 , 0.5 ) (1, 0.5) ( 1 , 0.5 ) to ( 0.5 , 0.5 ) (0.5, 0.5) ( 0.5 , 0.5 ) , y = 0.5 y = 0.5 y = 0.5 and d y = 0 dy = 0 d y = 0 :
W C D = ∫ 1 0.5 − 0.5 d x = 0.25 J W_{CD} = \int_{1}^{0.5} -0.5\,dx = 0.25\,\text{J} W C D = ∫ 1 0.5 − 0.5 d x = 0.25 J
For segment D E DE D E from ( 0.5 , 0.5 ) (0.5, 0.5) ( 0.5 , 0.5 ) to ( 0.5 , 0 ) (0.5, 0) ( 0.5 , 0 ) , x = 0.5 x = 0.5 x = 0.5 and d x = 0 dx = 0 d x = 0 :
W D E = ∫ 0.5 0 − 2 ( 0.5 ) d y = 0.5 J W_{DE} = \int_{0.5}^{0} -2(0.5)\,dy = 0.5\,\text{J} W D E = ∫ 0.5 0 − 2 ( 0.5 ) d y = 0.5 J
For segment E F EF E F from ( 0.5 , 0 ) (0.5, 0) ( 0.5 , 0 ) to ( 0 , 0 ) (0, 0) ( 0 , 0 ) , y = 0 y = 0 y = 0 and d y = 0 dy = 0 d y = 0 :
W E F = ∫ 0.5 0 0 d x = 0 J W_{EF} = \int_{0.5}^{0} 0\,dx = 0\,\text{J} W E F = ∫ 0.5 0 0 d x = 0 J
For segment F A FA F A from ( 0 , 0 ) (0, 0) ( 0 , 0 ) to ( 0 , 1 ) (0, 1) ( 0 , 1 ) , x = 0 x = 0 x = 0 and d x = 0 dx = 0 d x = 0 :
W F A = ∫ 0 1 − 2 ( 0 ) d y = 0 J W_{FA} = \int_{0}^{1} -2(0)\,dy = 0\,\text{J} W F A = ∫ 0 1 − 2 ( 0 ) d y = 0 J
Step 3: Sum the work done over all segments.
W = W A B + W B C + W C D + W D E + W E F + W F A W = W_{AB} + W_{BC} + W_{CD} + W_{DE} + W_{EF} + W_{FA} W = W A B + W B C + W C D + W D E + W E F + W F A
W = − 1 + 1 + 0.25 + 0.5 + 0 + 0 W = -1 + 1 + 0.25 + 0.5 + 0 + 0 W = − 1 + 1 + 0.25 + 0.5 + 0 + 0
W = 0.75 J W = 0.75\,\text{J} W = 0.75 J
Step 4: Verify using Green's Theorem.
The curl of the force field is:
∂ F y ∂ x − ∂ F x ∂ y = 2 α − α = α \frac{\partial F_y}{\partial x} - \frac{\partial F_x}{\partial y} = 2\alpha - \alpha = \alpha ∂ x ∂ F y − ∂ y ∂ F x = 2 α − α = α
Since the path is traversed clockwise, the work done is:
W = − ∬ α d A = − α A W = -\iint \alpha\,dA = -\alpha A W = − ∬ α d A = − α A
The enclosed area A A A is:
A = ( 1 × 1 ) − ( 0.5 × 0.5 ) = 0.75 m 2 A = (1 \times 1) - (0.5 \times 0.5) = 0.75\,\text{m}^2 A = ( 1 × 1 ) − ( 0.5 × 0.5 ) = 0.75 m 2
Substituting α = − 1 N m − 1 \alpha = -1\,\text{N}\,\text{m}^{-1} α = − 1 N m − 1 and A = 0.75 m 2 A = 0.75\,\text{m}^2 A = 0.75 m 2 :
W = − ( − 1 ) ( 0.75 ) = 0.75 J W = -(-1)(0.75) = 0.75\,\text{J} W = − ( − 1 ) ( 0.75 ) = 0.75 J
Answer:
The work done on the particle by this force is 0.75 Joule.