(a) The situation is as shown below. As shown, we resolve E along $CO$ and also $BO$ into two perpendicular components.
[image:1_image317.emf]
The horizontal components cancel each other.
The vertical (cosine) components add up along $OA$ to give $2E\ \cos\ 60{^\circ}.$
[image:1_image318.emf]
Resultant field along $AO$
$= 2E - 2E\cos\ 60{^\circ}$
$= 2E - 2E \times \frac{1}{2}$
$= 2E - E = E$
Hence, resultant field is $E\ along\ AO$.