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Finding Output Voltage in a Circuit using Node Method, Exercises of Signals and Systems Theory

Instructions on how to find the output voltage, v0, in a circuit with two voltage sources and multiple resistors using the node method in signals and systems. The document also mentions the use of the supernode method when one of the voltage sources is floating. The circuit schematic and resistor and voltage source values are given.

Typology: Exercises

2011/2012

Uploaded on 07/20/2012

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Unified Engineering I Fall 2003
Problem S5 (Signals and Systems)
Consider the circuit below:
+
+
R3R6
R5
R4R7
V2
V1
+
vo
Supernode
where
R3 = 2 Ω, R4 = 1 Ω, R4 = 2 Ω, R6 = 2 Ω, R7 = 1 Ω,
V1 = 10 V, V2 = 5 V
Find the output voltage, v0, using the node method. Note that because the two
voltage sources do not have a common terminal, it is not possible to choose a ground
node that is the negative terminal of both. As a result, one of the voltage sources
will be “floating.” Therefore, you will have to use the “supernode” method discussed
in recitation. The basic idea is to add the two node equations for the “floating”
voltage source. Each node equation has one term for the unknown current through
the voltage source. By adding the two equations together, the current terms cancel.
In essence, you are applying conservation of charge to the whole dashed region, rather
than just to a node.
Note: Feel free to use the loop method to check your answer, but use the node
method for your final answer.
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Unified Engineering I Fall 2003

Problem S5 (Signals and Systems)

Consider the circuit below:

R

R

R

R

R

V

V

v o

Supernode

where

R

3

= 2 Ω, R

4

= 1 Ω, R

4

= 2 Ω, R

6

= 2 Ω, R

7

V

1

= 10 V, V

2

= 5 V

Find the output voltage, v 0 , using the node method. Note that because the two

voltage sources do not have a common terminal, it is not possible to choose a ground

node that is the negative terminal of both. As a result, one of the voltage sources

will be “floating.” Therefore, you will have to use the “supernode” method discussed

in recitation. The basic idea is to add the two node equations for the “floating”

voltage source. Each node equation has one term for the unknown current through

the voltage source. By adding the two equations together, the current terms cancel.

In essence, you are applying conservation of charge to the whole dashed region, rather

than just to a node.

Note: Feel free to use the loop method to check your answer, but use the node

method for your final answer.

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