Answer: 2. \(100\sqrt{3}\) N
Key idea: the wall is smooth, so the wall force \(N\) is horizontal. For equilibrium, floor friction \(f\) equals \(N\), and torques about the bottom end must balance.
The rod makes \(60^\circ\) with the wall (vertical), length \(L=5\) m, \(mg=200\) N.
Torque about the foot of the rod: weight acts at \(L/2\) with horizontal arm \(\tfrac L2\sin60^\circ\); the wall force acts at the top with vertical arm \(L\cos60^\circ\).
$$mg\cdot\frac L2\sin60^\circ=N\,L\cos60^\circ\Rightarrow N=\frac{mg}{2}\tan60^\circ=100\sqrt3\ \mathrm N$$
So the friction force is \(f=N=100\sqrt3\) N.