A force of - F k^ acts on O, the origin of the coordinate system. The torque about the point (1, - 1) is
F(i^-j^)
-F (i^+j^)
F(i^+j^)
-F(i^-j^)
We know thatτ→=r→×F→The force F and point (1, - 1) is shown in figure.
Now τ→=(i^−j^)×(−Fk^)=F[(−i^×k^)+(j^×k^)]=F[j^+i^]=F(i^+j^)