Problem 4-82

a) Find the value of Ro so that it absorbs the maximum possible power from the circuit.


For maximum power transfer to Ro, it should equal the Thevenin equivalent resistance of the circuit to which it is connected, thus we need to determine that equivalent resistance.

I will do this by "killing" the independent sources and cannecting a test source in place of Ro. If a voltage source is chosen, we immediately know iD which should simplify the analysis a bit. We will thus need to find the current I delivered to the circuit by the test voltage source. I will use nodal analysis to determine I. The new circuit is thus


First, since the 80 ohm resistor is in parallel with the 1 volt source, the dependent source parameter iD is easily seen to be

iD = - 1 / 80 = - 12.5 mA


Next, both voltage sources directly connect two essential nodes forming supernodes. Expressing the value of each source in terms of the node voltages gives

VB = 1

124 iD = VA - VC

but since iD = - 12.5 mA

VA - VC = 124 (- 12.5m) = - 1.55 (equation 1)


Since node B is directly connected to the reference node by the 1 volt source, no KCL equation is written at node B.

Nodes A and C form a supernode, and we must write KCL for that supernode. I will sum the currents out of the supernode, and I will also immediately substitute 1 volt for VB.

VA / 16 + (VA -1) / 4 + VC / 12 + (VC - 1) / 8 = 0

Multiply through by 48

3 VA + 12 VA -12 + 4 VC + 6 VC - 6 = 0
15 VA + 10 VC = 18 (equation 2)

Solving the two equations gives

VA = 0.1
VC = 1.65


We can now get the current I using KCL at node B

I = (VB - VA) / 4 + (VB - VC) / 8 + VB / 80
I = (1 - 0.1) / 4 + (1 - 1.65) / 8 + 1 / 80
I = 156.25 mA


Finally, Ohm's Law yields the equivalent resistance

RTh = 1 / I = 1 / 156.25m = 6.4
Ro = 6.4 W


Part b) Find the maximum power that can be delivered to Ro.

There are basically two ways to proceed here.
One is to find the Thevenin or Norton Equivalent source, then attach the load resistance to the equivalent circuit to determine the power.
The other is to simply insert the load resistance into the original circuit to determine the power absorbed.

I will go the extra mile and find BOTH Voc and Isc which will then give us a check of the Thevenin equivalent resistance found directly in part a).


Voc: I will use mesh analysis


Define dependent source parameter

iD = IC - IB

Write KVL around each mesh

Mesh A:

124 iD + 8 (IA - IC) + 4 (IA - IB) = 0
124 (IC - IB) + 8 (IA - IC) + 4 (IA - IB) = 0
12 IA - 128 IB + 116 IC = 0 (equation 3)

Mesh B:

4 (IB - IA) + 80 (IB - IC) + 16 IB - 100 = 0
- 4 IA + 100 IB - 80 IC = 100 (equation 4)

Mesh C:

8 (IC - IA) + 50 + 12 IC + 80 (IC - IB) = 0
- 8 IA - 80 IB + 100 IC = - 50 (equation 5)

Solving equations 3, 4, and 5 gives

IA = 10.5 A
IB = 4.7 A
IC = 4.1 A

Finally, the open circuit voltage is the same as the voltage across the 80 ohm resistor, thus

Voc = 80 (IB - IC) = 80 (4.7 - 4.1)
Voc = 48 V

So, if we calculated RTh and Voc correctly, the power absorbed by the load resistance (maximum) is

P = Voc2 / Ro = 482 / 6.4
P = 360 W


To check all this (certainly subject to error through all that) we will determine Isc and verify that it agrees with the values we obtained for Voc and RTh.
Ohm's Law tells us that

Isc = Voc / RTh = 48 / 6.4 = 7.5 A

So direct determination of Isc should agree with this value if our previous results are correct.


With the short circuit in place, the circuit is

Before we dive right in, let's consider this circuit for a moment.

First, note that the 80 ohm resistor is shorted out, thus

iD = 0

This immediately implies that the voltage developed by the dependent source is ZERO.

Since the 80 ohm resistor is shorted out, it can be removed from the circuit without having any effect.
Since the dependent source voltage is zero, it can be replaced with a wire without affecting the circuit. The modified circuit is thus

Although it might appear that we could use source transforms and circuit reduction techniques here, it would be VERY difficult to keep track of the desired current Isc. Therefore, I will use mesh analysis.

Writing KVL around each mesh gives:

Mesh A:

8 (IA - IC) + 4 (IA - IB) = 0
12 IA - 4 IB - 8 IC = 0 (equation 6)

Mesh B:

4 (IB - IA) + 16 IB - 100 = 0
- 4 IA + 20 IB = 100 (equation 7)

Mesh C:

8 (IC - IA) + 50 + 12 IC = 0
- 8 IA + 20 IC = - 50 (equation 8)

Solving equations 6, 7, and 8 gives

IA = 0 A
IB = 5 A
IC = - 2.5 A

Therefore

Isc = IB - IC = 5 + 2.5
Isc = 7.5 A

Since this agrees with the value we calculated for Isc using Voc and RTh, we have a high degree of confidence that the earlier work is correct.

NOTE: This problem well illustrates the desirability of checking your work by an independent method when possible. When I first solved for RTh, I dropped a minus sign, thus the value determined for RTh was incorrect. When my value for Isc did not agree with Voc / RTh, I knew there was an error somewhere.


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