Let us change the problem description so that it makes a bit of physical sense.
We have a bead on a uniform, straight wire. Our lab is in space, far from any gravitational source. There is vacuum. No air resistance.
The bead grips the wire with a fixed and even pressure so that it resists motion along the wire. The maximum force of static friction is ##F##. The force of kinetic friction is also ##F##.
This force of friction is fixed. It remains the same as the bead moves. It remains the same if the bead happens to be subject to a lateral force.
We push on the bead, parallel to the wire with force ##F##. It moves at a steady pace. The force is in balance with friction.
We now push on the bead, at an angle ##\theta## to the wire with force ##F_2## so that it moves at a steady pace. The force is in balance with friction.
What is ##F_2##? How does it depend on ##\theta##?