Hooke's law is written similarly, according to which the elastic force $F$ arising during deformation of an elastic body (spring, rod, etc.) is proportional to the change in the length of the body $\Delta l$: $F = k \cdot \Delta l$, where $k$ is the coefficient of elasticity (stiffness) of the body. If $F > 0$ ($\Delta l > 0$), the spring is stretched. If $F < 0$ ($\Delta l < 0$), then the spring is compressed.
In what follows, when solving all parts of the problem, assume that the elements connecting the springs are light, non-deformable, and the system parameters are chosen so that these elements do not rotate under load (for example, they move along smooth vertical guides), the springs remain vertical under any deformation and are never compressed so much that the coils are tightly pressed against each other.
The equations describing the electrical circuit and the mechanical system are analogous. For example, the inverse stiffness of a spring $1/k$ in the mechanical system is a quantity analogous to electrical resistance $R$ in the electrical circuit.
Note. The effective stiffness coefficient of the system in this case is the ratio of the magnitude of the force applied to point $C$ to the magnitude of the displacement of the point of application of this force.