I don't understand how one rope, when dividing it's load over the wheel in the pully can withstand close to double what it could as an individual.
But the rope
tension is not 'divided,' it adds. Meaning with a given tension of 10lbs on the roope, when through a pulley, will add to 20lbs of supporting force.
As said before, the rope tension is (theoretically) constant throughout the system when going through pulley's. So it is not 'withstanding double' of anything.
Just think of a 100 lb weight dangling from 4 equalized ropes. Would you expect all 4 ropes to experience 100 lbs of tension? Or 25.
Perhaps what you are thinking is that since the axle of a pulley would see twice the rope tension, somewhere the rope must also 'see' twice it's own tension since it's wrapped around that axle.
What might help you here is to consider vectors. In the line created by the pulley axle and the load, the rope is normal (perpendicular) to that force. I.e. there is no tension component on the rope at that point. But there is compression.
You could also—instead of a wheel—picture a spreader bar with the load in the center and the two supporting ropes on either side. If you cut one supporting rope, the system will become unbalanced and the load will seek to align with the one remaining rope.
In the case of a pulley, this means you could wrap the rope around the pulley and tie it back onto itself and the axle would then align between the load and rope. The rope would then be experiencing the full load under tension (though split along the looped portion according to the vector forces based on the angles created by where the knot is tied). That's when you need trig to access those forces.