Maria said:
Circle there is just to show where points are allowed to move but is not a physical object.
Actually, it helps to have a real wire circle and imagine the points to be beads that are free to move around. The wire allows the beads to move freely on the circle in a tangential direction and prevents them from moving in a radial direction. Regardless of how you model this, the most basic problem to understand how forces add as vectors. Imagine walking in a straight line in some direction a certain distance. Then you change direction and walk another distance, and another and another, four changes in direction until you end up where you started. Your overall displacement is zero because you end up where you started. This is another way of saying that the sum of the four individual displacement vectors is zero. Note that if you were to draw the four vectors as arrows with the end of one at the tip of the other, you will get a closed quadrilateral loop representing the path you took. The same idea applies to all vectors including forces: if you have N vectors adding up to zero, they must form a closed N-sided polygon.
So in this case you need to find a quadrilateral that can have a circle passing through its four apices. The length of the ropes between adjacent beads can be viewed as proportional to the force acting on a particular bead. So the sides of the quadrilateral must all be equal, which makes it a rhombus. The additional constraint that the points are on circle makes the rhombus a square. So a square is the only shape that satisfies all the constraints. This means that each bead experiences the same radial force. This is the obvious symmetrical solution and probably of little interest to you.
If you relax the constraint that the forces be equal, you can construct a quadrilateral of unequal sides inside a circle as long as two of diagonally opposite angles are 90
o each. Then the beads will be in translational equilibrium, i.e. the center of the circle will not accelerate. However, there will be an unbalanced torque on the four-bead system which will give the system a spin about the center. Shown below is a picture of what I mean. The opposing right angles are DAB and DCB and you may imagine that the dotted lines are light rigid rods connecting the beads. The force on each bead is along the length of the rod attached to it on one side and proportional to the length of the rod. The diagram on the left shows force arrows connected to the sides of the quadrilateral that are proportional to them. The diagram on the right has swapped the forces (A →D, D→C, C→A), keeping their magnitudes and directions fixed, so that the sum will still be zero. I leave it up to you to figure out how many different such swaps are possible.