The force acting on the man can be determined by taking the derivative of the potential energy function with respect to x: F(x) = -dU(x)/dx = 6x - 9x^2. This means that the force acting on the man is a function of the position, with a maximum value of 6 joules at x = 1/3 metres, and a minimum value of 0 joules at x = 0 and x = 2 metres.
The man is in equilibrium at the positions where the force acting on him is zero, which are x = 0 and x = 2 metres. This means that at these positions, the man is not experiencing any force and is in a state of balance.
To determine the stability of these equilibrium positions, we can look at the second derivative of the potential energy function: d^2U(x)/dx^2 = 6 - 18x. At x = 0, the second derivative is positive (6), indicating a stable equilibrium position. This means that if the man is slightly displaced from this position, he will experience a restoring force that will bring him back to the equilibrium position.
At x = 2 metres, the second derivative is negative (-6), indicating an unstable equilibrium position. This means that if the man is slightly displaced from this position, he will experience a force that will continue to push him away from the equilibrium position.
In summary, the force acting on the man is a function of his position, and he is in equilibrium at x = 0 and x = 2 metres. However, only the equilibrium position at x = 0 is stable, while the equilibrium position at x = 2 is unstable.
