Call the point where the ladder touches the floor, a point half way along the ladder and the point where the ladder touches the wall A, B and C respectively. Assume the mass of the ladder is all at point B.
Resolve vertically. So the downward force at B of 30g is matched with an upward force at A of 30g.
Resolve horizontally. At A there is a horizontal force of friction, F, towards the wall, matched by a force at C, out from the wall.
You can then take moments about point C. These are assumed to be perpendicular to the ladder. The clockwise and anti-clockwise moments need to balance.
So 230gcos70+4Fsin70=430gcos70.
So Fsin70=2*30gcos70
F=2*30gcos70/sin70
It is in limiting equilibrium and I do not have a symbol for mu on my keyboard so I'm calling the coefficient of friction m.
So F=m30g
We now have 2 equations for F, so can out them equal to each other.
So m30g=2*30g/tan70
m=2/tan70
This is what I am remembering from dd's maths 2 years ago, so it could be horribly wrong. I can remember saying to resolve vertically, resolve horizontally, take moments. I would wait for Noblegiraffe or some other good maths person to confirm this.
I know dd used the CGP books for A level maths, and they were really clear and made it seem simple!