First of all, great job on attempting to use the formula for force due to a spring, F=-kx. However, in this case, the particle is being pulled in a direction perpendicular to the initial configuration of the springs, so we cannot simply use the displacement x as the distance from the equilibrium position.
To solve this problem, we need to consider the geometry of the situation. Let's draw a diagram to visualize it.
We have a particle of mass m attached to two identical springs with spring constant k and unstretched length L. The particle is pulled a distance x along a direction perpendicular to the initial configuration of the springs. Let's label the angle between the displacement vector and the horizontal axis as θ.
Now, let's consider the forces acting on the particle. The two springs will exert equal and opposite forces on the particle, each with a magnitude of F=-kx. However, these forces are not acting in the same direction. The force from the left spring is acting in the direction of the displacement, while the force from the right spring is acting in the opposite direction.
Using trigonometry, we can see that the component of the force from the left spring in the direction of the displacement is F_left = -kx cosθ, and the component of the force from the right spring in the direction of the displacement is F_right = kx cosθ.
Since the two forces are acting in opposite directions, we can simply subtract them to get the net force on the particle in the direction of the displacement:
F = F_left - F_right = -kx cosθ - kx cosθ = -2kx cosθ
Now, we need to find the value of cosθ. From the diagram, we can see that cosθ = x/(x^2+L^2)^0.5. Substituting this into the equation for F, we get:
F = -2kx(x/(x^2+L^2)^0.5)
Next, we need to simplify this expression. We can use the identity (a^2+b^2)^0.5 = c to rewrite (x^2+L^2)^0.5 as (x^2+(L^2)^0.5)^0.5. This allows us to write the expression as:
F = -2kx(1-(L/(x^2+L^2)^0.5))