The easiest way to take moments about a point
for a force not at right angles to the line joining the point of action
of the force to A is to resolve the force into components parallel to
and perpendicular to![]()

The 50N force above has components
perpendicular to
and
parallel to![]()
The 80N force has components
perpendicular to
and
parallel to![]()

The moments of the forces are then
anticlockwise and
clockwise so the net moment due to the two forces is![]()
The components of the forces parallel to![]()
and
pass through
and do not contribute to the moment.