Problem 15-17 Source:
Problem developed by the site author.
In the circuit shown in Figure 15-17.1, using the theorem of Thévenin , determine the value
R so that it dissipates the maximum power.
Solution of the Problem 15-17
To use the Thevenin theorem, we must remove the resistor R from the circuit. Thus, the
pair of terminals a and b appears. In these terminals we must determine the voltage
of Thévenin in open circuit.
For this, and based on the circuit shown in Figure 15-17.2 , using a current
divider we can
determine the values of I1 and I2. So
I1 = 10 (30 + 100) / (30 + 100 + 120 + 150)
Performing the calculation we find the value of I1, or
I1 = 3.25 A
We use the same method to find the value of I2.
I1 = 10 (120 + 150) / (30 + 100 + 120 + 150)
Performing the calculation we find the value of I2, or
I2 = 6.75 A
Naturally, knowing the relation 10 = I1 + I2, we also find
I2 = 10 - I1 = 6.75 A.
Now, knowing the values of I1 and
I2 we can calculate the potential at terminals a and b, remembering that by
resistors 4 Ω and 2.25 Ω current does not circulate.
Then, making the mesh highlighted in
orange, as shown in Figure 15-17.2, we have:
- 150 I1 + Vab + 100 I2 = 0
Then, we have:
Vab = Vth = - 187.5 V
To determine the value of Rth, we must eliminate the current source and after some
arrangement in the circuit, the Figure 15-17.3 shows the new topology.
Through the circuit, it is verified that the resistors of 100 Ω
and 150 Ω
are in series, as well as the resistors of 120 Ω and 30 Ω . Therefore, adding the
values we find 250 Ω e 150 Ω.
After the calculation, we verify that these two resistors are in parallel.
Then the equivalent resistance of the parallel will be:
Req = 250 x 150 / (250 + 150) = 93.75 Ω
Now, this equivalent resistance is in series with the resistors of 4 Ω
and 2.25 Ω.
Therefore, the resistance of Thévenin is
Rth = 93,75 + 2,25 + 4 = 100 Ω
In the Figure 15-17.4 we see the final result. Notice that point b has a greater potential
than the point a . To determine the value of R that dissipates the greatest power, we will use the
maximum power transfer theorem. This theorem says that for maximum transfer
of power for the load, it must have the same value as the resistance of Thévenin . Therefore