Let F→ be the force acting on a particle having position vector r→ and τ→ the torque of this force about the origin. Then
r→⋅τ→=0 and F→⋅τ→=0
r→∙τ→=0 and F→∙τ→≠0
r→∙τ→≠0 and F→∙τ→=0
r→∙τ→≠0 and F→∙τ→≠0
We know that,τ→ = r→×F→ . So τ→ is perpendicular to both r→ and F→so, r→.τ→=0and F→.τ→=0