Circuit Analysis Techniques
Ohm's Law states the voltage across a resistor, R
(or impedance, Z) is directly proportional to the current passing
through it (the resistance/impedance is the proportionality constant)
Kirchhoff's Voltage Law (KVL): the algebraic sum of the voltages
around any loop of N elements is zero (like pressure drops through
a closed pipe loop)
Kirchhoff's Current Law (KCL): the algebraic sum of the currents
entering any node is zero, i.e., sum of currents entering equals
sum of currents leaving (like mass flow at a junction in a pipe)
Nodal analysis is generally best in the case of several voltage sources.
In nodal analysis, the variables (unknowns) are the "node voltages."
Nodal Analysis Procedure:
 Label the N node voltages. The node voltages are defined positive
with respect to a common point (i.e., the reference node) in the circuit
generally designated as the ground (V = 0).
 Apply KCL at each node in terms of node voltages.
 Use KCL to write a current balance at N1 of the N nodes
of the circuit using assumed current directions, as necessary. This will create
N1 linearly independent equations.
 Take advantage of supernodes, which create constraint equations.
For circuits containing independent voltage sources, a supernode is generally
used when two nodes of interest are separated by a voltage source instead of a
resistor or current source. Since the current (i) is unknown through the
voltage source, this extra constraint equation is needed.
 Compute the currents based on voltage differences between nodes.
Each resistive element in the circuit is connected between two nodes;
the current in this branch is obtained via Ohm's Law
where V_{m} is the positive side and current flows from node
m to n (that is, I is m > n).
 Determine the unknown node voltages; that is, solve the N1
simultaneous equations for the unknowns, for example using Gaussian elimination
or matrix solution methods.
Nodal Analysis Example

 Label the nodal voltages.
 Apply KCL.
 KCL at top node gives I_{S} = I_{L} + I_{C}
 Supernode constraint eq. of V_{L} = V_{S}

 Solve for V_{T} for instance.

Mesh (loop) analysis is generally best in the case of several current sources.
In loop analysis, the unknowns are the loop currents. Mesh analysis means that we
choose loops that have no loops inside them.
Loop Analysis Procedure:
 Label each of the loop/mesh currents.
 Apply KVL to loops/meshes to form equations with current variables.
 For N independent loops, we may write N total equations
using KVL around each loop. Loop currents are those currents flowing in a loop;
they are used to define branch currents.
 Current sources provide constraint equations.
 Solve the equations to determine the user defined loop currents.
Mesh Analysis Example:

 Label mesh currents.
 Apply KVL.
 Left loop KVL:
 V_{S} = R_{1}I_{1} + R_{2}(I_{1}I_{2})
 Constraint equation I_{2} = I_{S}.
 Solve for I_{1} and I_{2}.
Note: Branch current from mesh currents: I_{M} = I_{1}  I_{2}

In any linear circuit containing multiple independent sources,
the current or voltage at any point in the network may be calculated as the
algebraic sum of the individual contributions of each source acting alone.
Procedure:
 For each independent voltage and current source (repeat the following):
 Replace the other independent voltage sources with a short circuit
(i.e., v = 0).
 Replace the other independent current sources with an open circuit
(i.e., i = 0).
 Note: Dependent sources are not changed!
 Calculate the contribution of this particular voltage or current
source to the desired output parameter.
 Algebraically sum the individual contributions (current and/or voltage)
from each independent source.
An ac voltage source V in series with an impedance Z can be
replaced with an ac current source of value I=V/Z in parallel
with the impedance Z.
An ac current source I in parallel with an impedance Z can be
replaced with an ac voltage source of value V=IZ in series with the
impedance Z.
Likewise, a dc voltage source V in series with a resistor R can be
replaced with a dc current source of value i = v/R in parallel
with the resistor R; and vice versa.
Thévenin's Theorem states that we can replace entire network,
exclusive of the load, by an equivalent circuit that contains only an
independent voltage source in series with an impedance (resistance) such
that the currentvoltage relationship at the load is unchanged.
Norton's Thereom is identical to Thévenin's Theorem except
that the equivalent circuit is an independent current source in parallel
with an impedance (resistor). Hence, the Norton equivalent circuit is a
source transformation of the Thévenin
equivalent circuit.
Thévenin Equivalent Circuit 
Norton Equivalent Circuit 


Procedure:
 Pick a good breaking point in the circuit (cannot split a dependent
source and its control variable).
 Thevenin: Compute the open circuit voltage, V_{OC}.
Norton: Compute the short circuit current, I_{SC}.
 Compute the Thevenin equivalent resistance, R_{Th}
(or impedance, Z_{Th}).
 If there are only independent sources, then short circuit all the voltage
sources and open circuit the current sources (just like superposition).
 If there are only dependent sources, then must use a test voltage or current
source in order to calculate R_{Th}= v_{Test}/i_{Test}
(or Z_{Th}=V_{Test}/I_{Test}).
 If there are both independent and dependent sources, then compute
R_{Th} (or Z_{Th}) from
R_{Th}= v_{OC}/i_{SC}
(or Z_{Th}=V_{OC}/I_{SC}).
 Replace circuit with Thevenin/Norton equivalent.
Thevenin: V_{OC} in series with R_{Th}
(or Z_{Th}).
Norton: I_{SC} in parallel with R_{Th}
(or Z_{Th}).
 Note: for 3(b) the equivalent network is merely R_{Th}
(or Z_{Th}), that is, no current or voltage sources.
Last updated: June 10, 1998
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