$$\textbf{Given:- }$$ The net external force acting on the disc
$$\textbf{Solution:-}$$ Net Force acting on a body is given by the formula:
$$\vec{F_{net}} = m.\vec{a}$$
Where,
$$\vec{F_{net}}$$ is the net force acting on the body
m is the mass of the body
$$\vec{a}$$ is the acceleration of the body
We will insert$$\left ( -2kx + F \right )$$ in the place of $$\vec{F_{net}}$$
$$-2kx + F = Ma_{c}................(1)$$
Where,
k is the spring constant
x is the distance by which the spring has been stretched
F is the friction force on the disk
M is the mass of disk
$$a_{c}$$ is the acceleration of centre of mass of the disk
Net Torque acting on a body is given by the formula,
$$\vec{\tau _{net}} = I\vec{\alpha }...............(2)$$
Where,
$$\vec{\tau _{net}}$$ is the net Torque acting on the body
I is the moment of inertia of the body
$$\vec{\alpha }$$ is the angular acceleration of the body
Additionally, Torque is also calculated as follows,
$$\vec{\tau _{net}} = \vec{F}\times R................(3)$$
Where,
R is the distance of the Force from the center of mass of the body
Now combining equations 2 and 3,
$$\vec{F}\times R = T\vec{\alpha}$$
$$\vec{F} = \dfrac{T\vec{\alpha}}{R}.................(4)$$
In Pure Rolling condition,
$$a_{c} = \vec{\alpha_{c}}R$$
Moment of inertia of a disk is given by the formula,
F $$= \dfrac{\dfrac{1}{2}MR^{2}}{R}\times \dfrac{a_{c}}{R}$$
$$\Rightarrow F = \dfrac{1}{2}Ma_{c}$$
Inserting the value of F in equation 1,
$$\Rightarrow -2kx + \dfrac{1}{2}Ma_{c} = -Ma_{c}$$
$$\Rightarrow \dfrac{1}{2}Ma_{c} + Ma_{c} = 2kx $$
$$\Rightarrow \dfrac{3}{2}Ma_{c} = 2kx$$
$$\Rightarrow Ma_{c} = \dfrac{4}{3}kx$$
$$\Rightarrow MA_{c} = \dfrac{4}{3}kx$$
$$\textbf{Hence the correct option is D}$$