The picture below can illustrate the concept of static equilibrium. On a pulley hangs an object A on which acts the gravity with the force $G_A$. If on the other end of the cable there is nothing, the system A + cable is not in static equilibrium and A will fall pulling the cable after it. But, if on the other end we hand an object B of the same weight as A, the system will be in equilibrium: nothing moves, and nothing falls.
A net force appears when the weights of A and B are not equal.
To see this let's write the equations. I consider the positive direction of the forces, upwards, and I write the sign of the forces explicitly.
On the left hand side (LHS) $-G_A$ pulls the cable downwards, and by virtue of the 3rd Newton law the cable pulls the object A with a force of tension, $T_1$, equal in magnitude and opposite in direction to $-G_A$.
(1) $T_1 = +G_A$
On the right hand side (RHS), if there is an object B, there appears a tension force $T_2$ in the cable, also upwards directed.
(2) $T_2 = +G_B$
The two tensions have to be equal, otherwise the cable won't be fully stretched, it will tend to gather on the top of the pulley. For that, one should have $G_A = G_B$. If this equality doesn't hold, the system is not in equilibrium. For instance, assume that $G_A - G_B > 0$. This difference produces a torque on the pulley which rolls the cable. Thus, the object A gets a downward acceleration $a$, and the object B gets the same acceleration (because the length of the cable is constant), but upwards. So, on the LHS we have
(3) $T_1 - G_A = -m_A a$.
On the RHS,
(4) $T_2 - G_B = +m_B a$.
Now, since the cable is fully streched, $T_1 = T_2$.
Let's subtract eq. (2) from (1)
(5) $-(m_A + m_B)a = -(G_A - G_B)$
The net force that acts on the system, is the force that imposes an acceleration to the system. This force is $-(G_A - G_B)$, and the acceleration is
(6) $-a = -\frac {G_A - G_B}{(m_B + m_A)}$ .
Remember, the signs are here explicit.