Let us do a demonstration of how the Thevenin Theorem simplifies the calculation of the classical
Loaded Wheatstone bridge(an important "tool" in many areas).
We want to know all aspects of the Load and "Driving Network" and the relationship between them.
Here is the circuit:
We could do that in the traditional Loop method or Node method .
In either case there would be 3 equations with 3 unknowns to solve.
Complicated, and a lot of potential for errors...
Like so:
Solving it with Thevenin:
1) First step, we disconnect the Load and calculate the open circuit voltage that is Vab.
That is immediate and intuitive.
we have two parallel branches:
one consists of R1 and R2 in series and the other of R3 and R4 in series.
Voltages are relative to "GND"(the negative of Vs,our reference point).
The simplest voltage divider yields:
Va=VR2= Vs*[R2/(R1+R2)]
Vb=VR4= Vs*[R4/(R3+R4)]
Vab=Va-Vb=Vs*[R2/(R1+R2)]-Vs*[R4/(R3+R4)]
Vth=Vab=
Vs*[R2/(R1+R2) - R4/(R3+R4)]
That is kids stuff easy,isn't it?

Not only that ,
there is great insight here(very often overlooked):
Vth is the maximum absolute possible voltage on any RL connected
i.e
for a given bridge and Vs values we can't get above Vth volts on any RL!
Next we calculate Rth (in next post)