dw = \(\vec F.d\vec r\)
dw = αydx + 2αxdy
\(A\to B\) \(y=1,dy=0\) \(w_{A\to B}=\int \alpha yd\mathrm x,\) \(1\int^1_0d\mathrm x = \alpha\)
\(B\to C\) \(\mathrm x=1, d\mathrm x = 0 \) \(w_{B\to C}=2\alpha.1\int^{0.5}_1dy\) \(=-2\alpha(0.5)=-\alpha\)
\(C\to D\) \(y=0.5,dy=0\) \(w_{C\to D}=\int^{0.5}_1\alpha yd\mathrm x = \alpha.\frac{1}{2}\), \(\int^{0.5}_1d\mathrm x=-\frac{\alpha}{4}\)
\(D\to E\) \(\mathrm x=0.5,d\mathrm x = 0\) \(w_{D\to E}=2\alpha \int \mathrm xdy = 2\alpha.\frac{1}{2}\) \(\int^0_{0.5}dy = -\frac{\alpha}{2}\)
\(E \to F,\) \(y=0, E_{EF}=0\)
\(F\to A,\mathrm x = 0, d\mathrm x = 0, W_{F\to A}=0\)
\(\therefore w=\alpha-\alpha-\frac{\alpha}{4}-\frac{\alpha}{2}\) \(=-\frac{3\alpha}{4}\)
Given α =-1
=>W=+3/4J
=0.75J.