UNIT 5: Network Analysis - Short Notes
1. Basic Circuit Laws, Theorems, and Analysis Techniques
Kirchhoff's Laws
- KCL (Current Law): At any node, the algebraic sum of currents leaving the node is zero.
$$\sum_{k=1}^{n} i_k = 0$$
> [!TIP] Assign consistent current directions (e.g., all leaving).
- KVL (Voltage Law): Around any closed loop, the algebraic sum of voltages is zero.
$$\sum_{k=1}^{n} v_k = 0$$
> [!TIP] Traverse loop in one direction, assign + to voltage if entering + terminal of an element.
Mesh Analysis (Planar Circuits)
-
Identify independent meshes (windows).
-
Apply KVL to each mesh, expressing voltages in terms of mesh currents.
-
Solve simultaneous equations.
- Supermesh: Formed when a current source lies on a common branch of two meshes. The supermesh excludes the current source and its branch. Use KVL on supermesh and the current source constraint equation.
Nodal Analysis
-
Select a reference node (ground).
-
Assign node voltages to remaining (n-1) nodes.
-
Apply KCL at each non-reference node, expressing currents in terms of node voltages.
-
Solve equations.
- Supernode: Formed when a voltage source connects two non-reference nodes. Enclose the source and connected nodes. Apply KCL to the supernode and use the voltage source constraint.
Superposition Theorem
For a linear circuit with multiple independent sources:
-
The response (voltage/current) in any element = Algebraic sum of responses caused by each independent source acting alone.
-
Procedure: Kill all other independent sources (voltage sources → short, current sources → open). Repeat for each source and sum results.
Pitfall: Does NOT apply to power calculations directly.
Thevenin's Theorem
Any linear two-terminal network can be replaced by an equivalent circuit of:
-
V<sub>TH</sub>: Open-circuit voltage across terminals.
-
R<sub>TH</sub> (DC) / Z<sub>TH</sub> (AC): Equivalent impedance seen from terminals with all independent sources killed.
-
For AC: Z<sub>TH</sub> = R<sub>TH</sub> + jX<sub>TH</sub>
-
With dependent sources, apply test source.
-
Norton's Theorem
Equivalent circuit: I<sub>N</sub> (short-circuit current) in parallel with R<sub>N</sub> / Y<sub>N</sub>.
-
R<sub>N</sub> = R<sub>TH</sub>, Y<sub>N</sub> = 1/Z<sub>TH</sub>
-
I<sub>N</sub> = V<sub>TH</sub> / Z<sub>TH</sub>
Maximum Power Transfer Theorem
- Condition: Load impedance Z<sub>L</sub> = Z<sub>TH</sub>** (complex conjugate for AC).
$$Z_L = R_{TH} + jX_{TH} \quad \text{(For max power)}$$
- Maximum Power:
$$P_{max} = \frac{|V_{TH}|^2}{4R_{TH}}$$
- Efficiency at max power:
$$\eta = \frac{P_{load}}{P_{total}} = \frac{P_{max}}{P_{max} + P_{loss\,in\,R_{TH}}} = 50\%$$
Millman's Theorem
For parallel voltage sources (V<sub>1</sub>...V<sub>n</sub>) each with series resistance (R<sub>1</sub>...R<sub>n</sub>):
\boxed{V = \frac{\sum_{k=1}^{n} \frac{V_k}{R_k}}{\sum_{k=1}^{n} \frac{1}{R_k}}}
The equivalent resistance:
$$R_{eq} = \frac{1}{\sum_{k=1}^{n} \frac{1}{R_k}}$$
Tellegen's Theorem
For any network (linear/nonlinear, passive/active, time-variant/invariant):
\boxed{\sum_{m=1}^{b} v_m i_m = 0}
Where the sum is over all b branches, v<sub>m</sub> and i<sub>m</sub> are branch voltage and current satisfying KVL & KCL.
Interpretation: Total instantaneous power in any network is zero (power absorbed = power delivered).
Compensation Theorem
If a branch impedance Z in a network is changed by ΔZ, the change in any branch current/voltage is the same as that produced by injecting a compensating source (V = -IΔZ or I = -VΔZ) in series/parallel with the changed branch, with all other sources killed.
Use: Sensitivity analysis.
Substitution Theorem
If the voltage across and current through any branch of a network are known, that branch can be replaced by any combination of elements that maintains the same v-i relationship (e.g., ideal voltage source of that voltage, or ideal current source of that current), without altering the currents/voltages elsewhere.
2. Network Topology
Graph & Oriented Graph
-
Graph: Set of nodes (junctions) and branches (elements) showing connectivity, ignoring element sizes.
-
Oriented Graph: Graph with arrows on branches indicating reference direction for current.
Tree & Co-Tree
-
Tree (T): A connected subgraph containing all nodes and no loops. Has (n-1) branches for n nodes.
-
Twigs: Branches of the tree.
-
Links (or Chords): Branches not in the tree. Number of links = b - (n-1) = l.
-
Co-Tree: Set of all links. Each link, when added to the tree, forms a fundamental loop.
Tie Set & Basic Tie Set Matrix
-
Tie Set (Fundamental Loop): A loop containing exactly one link and the tree branches connecting its end nodes.
-
Basic Tie Set Matrix (B<sub>f</sub>): (l x b) matrix. Rows = fundamental loops (links). Columns = all branches.
-
Entry: +1 if branch reference direction aligns with loop direction, -1 if opposite, 0 if not in loop.
-
Property: B<sub>f</sub> · A = 0 (A = incidence matrix).
-
Cut Set & Basic Cut Set Matrix
-
Cut Set: A set of branches whose removal disconnects the graph into two parts, with exactly one branch from the tree connecting each part.
-
Fundamental Cut Set: A cut containing exactly one twig.
-
Basic Cut Set Matrix (Q<sub>f</sub>): ((n-1) x b) matrix. Rows = fundamental cuts (twigs). Columns = all branches.
- Property: Q<sub>f</sub> · A = I (identity matrix).
Incidence Matrix
-
Complete Incidence Matrix (A): (n x b) matrix.
-
a<sub>ij</sub> = +1 if branch j leaves node i.
-
a<sub>ij</sub> = -1 if branch j enters node i.
-
a<sub>ij</sub> = 0 otherwise.
-
Property: Sum of any column = 0. Sum of any row = number of branches incident.
-
-
Reduced Incidence Matrix (A<sub>red</sub>): Formed by deleting the row corresponding to the reference node. Size: ((n-1) x b). Used in nodal analysis: A<sub>red</sub> · V = E (source vector).
Matrix Relationships
\boxed{A_{red}^T \cdot Q_f^T = I} \quad \text{and} \quad \boxed{B_f \cdot A = 0}
Where I is identity matrix.
3. Mutual Inductance and Coupled Circuits
Self & Mutual Inductance
- Self Inductance (L): Flux linking a coil due to its own current:
$$v = L \frac{di}{dt}$$
- Mutual Inductance (M): Flux in one coil due to current in another:
$$v_2 = M \frac{di_1}{dt}$$
-
Dot Convention: Dots indicate polarity of induced voltage. If currents enter dotted terminals simultaneously, mutual voltage is positive.
- Equation:
$$v_1 = L_1 \frac{di_1}{dt} \pm M \frac{di_2}{dt}$$
* Sign: **+** if i<sub>2</sub> enters dotted terminal, **-** if enters undotted.
Coefficient of Coupling (k)
\boxed{k = \frac{M}{\sqrt{L_1 L_2}}}, \quad 0 \le k \le 1
-
k = 1: Perfect coupling (all flux links).
-
k = 0: No coupling (M = 0).
Equivalent Inductance
-
Series Aiding: L<sub>eq</sub> = L<sub>1</sub> + L<sub>2</sub> + 2M
-
Series Opposing: L<sub>eq</sub> = L<sub>1</sub> + L<sub>2</sub> - 2M
-
Parallel Aiding:
$$L_{eq} = \frac{L_1 L_2 - M^2}{L_1 + L_2 + 2M}$$
- Parallel Opposing:
$$L_{eq} = \frac{L_1 L_2 - M^2}{L_1 + L_2 - 2M}$$
Analysis of Coupled Circuits
-
Write KVL for each mesh, including mutual terms using dot convention.
-
Solve simultaneous differential equations.
- Example (two coils, dots on left):
$$v_1 = L_1 \frac{di_1}{dt} + M \frac{di_2}{dt}$$
$$v_2 = M \frac{di_1}{dt} + L_2 \frac{di_2}{dt}$$
4. Resonance
Series Resonance (RLC Series)
- Resonant Frequency (ω<sub>0</sub>): When X<sub>L</sub> = X<sub>C</sub>.
$$\omega_0 = \frac{1}{\sqrt{LC}} \quad \text{or} \quad f_0 = \frac{1}{2\pi\sqrt{LC}}$$
-
Impedance: Z = R (minimum, purely resistive).
-
Current: I = V/R (maximum).
-
Voltage Magnification: Voltage across L or C = Q × V, where Q-factor =
$$\frac{\omega_0 L}{R} = \frac{1}{\omega_0 C R}$$
- Bandwidth (BW):
$$\text{BW} = \frac{\omega_0}{Q} = \frac{R}{L} \text{ (rad/s)}$$
Parallel Resonance
-
Ideal Case (R=0): ω<sub>0</sub> = 1/√(LC), admittance Y = 0 (infinite impedance).
-
Practical (with R in series with L):
-
Admittance minimum → Impedance maximum.
-
Resonant frequency:
-
$$\omega_0 = \sqrt{\frac{1}{LC} - \frac{R^2}{L^2}} \approx \frac{1}{\sqrt{LC}} \text{ (if R small)}$$
* At ω<sub>0</sub>, current from source is minimum, and currents in L and C branches are large (Q × I<sub>source</sub>).
5. Fourier Series
Trigonometric Fourier Series
For a periodic function f(t) with period T=2π/ω₀:
\boxed{f(t) = a_0 + \sum_{n=1}^{\infty} (a_n \cos n\omega_0 t + b_n \sin n\omega_0 t)}
- Coefficients:
$$a_0 = \frac{1}{T} \int_{0}^{T} f(t) dt \quad (\text{DC component})$$
$$a_n = \frac{2}{T} \int_{0}^{T} f(t) \cos n\omega_0 t \, dt$$
$$b_n = \frac{2}{T} \int_{0}^{T} f(t) \sin n\omega_0 t \, dt$$
-
Symmetry Properties:
-
Even function: b<sub>n</sub> = 0 (only cosine terms).
-
Odd function: a<sub>0</sub> = a<sub>n</sub> = 0 (only sine terms).
-
Half-wave symmetry: f(t+T/2) = -f(t) → only odd harmonics (n=1,3,5...).
-
Exponential Fourier Series
\boxed{f(t) = \sum_{n=-\infty}^{\infty} c_n e^{jn\omega_0 t}}
- Complex Coefficients:
$$c_n = \frac{1}{T} \int_{0}^{T} f(t) e^{-jn\omega_0 t} dt$$
- Relationship:
$$c_0 = a_0, \quad c_n = \frac{a_n - jb_n}{2}, \quad c_{-n} = \frac{a_n + jb_n}{2}$$
- |c<sub>n</sub>| gives amplitude of nth harmonic, ∠c<sub>n</sub> gives phase.
Waveform Analysis (Common Examples)
- Square Wave (odd, ±A, 50% duty): Only odd harmonics.
$$a_0=0, \quad a_n=0, \quad b_n = \frac{4A}{n\pi} \text{ for n odd}$$
- Triangular Wave (odd, even harmonics only):
$$b_n = \frac{8A}{n^2\pi^2} \text{ for n odd}$$
- Sawtooth Wave (odd):
$$a_0 = 0, \quad a_n = 0, \quad b_n = -\frac{2A}{n\pi}$$
6. Laplace Transform in Network Analysis
Laplace Transform (LT) Properties
-
Linearity: L{af(t) + bg(t)} = aF(s) + bG(s)
-
Time-shift: L{f(t-a)u(t-a)} = e<sup>-as</sup>F(s)
-
Differentiation: L{f'(t)} = sF(s) - f(0⁻)
-
Integration: L{∫₀ᵗ f(τ)dτ} = F(s)/s
-
Convolution: L{f(t)*g(t)} = F(s)G(s)
s-Domain Circuit Elements
| Element | Time Domain | s-Domain Impedance (with IC) |
|---|---|---|
| Resistor (R) | v = Ri | Z(s) = R |
| Inductor (L) | v = L di/dt | Z(s) = Ls + Li(0⁻) |
| Capacitor (C) | i = C dv/dt | Z(s) = 1/(Cs) + 1/(sC) v(0⁻) |
| Voltage Source | v(t) | V(s) |
| Current Source | i(t) | I(s) |
- Initial conditions (IC) appear as additional sources in s-domain.
Initial & Final Value Theorems
-
Initial Value Theorem (if F(s) has no poles in Re(s)>0):
\boxed{f(0^+) = \lim_{s \to \infty} sF(s)}
-
Final Value Theorem (if sF(s) has no poles in Re(s)≥0):
\boxed{f(\infty) = \lim_{s \to 0} sF(s)}
Pitfall: Do not apply final value theorem if poles on imaginary axis (e.g., undamped oscillation).
Transient Analysis (Steps)
-
Draw s-domain circuit. Replace L, C with their impedances including IC sources.
-
Apply circuit laws (KVL/KCL) to find desired variable (I(s), V(s)).
-
Simplify F(s) using partial fractions.
-
Apply inverse LT (using tables or pole-zero) to get f(t).
-
For t>0, use final value theorem to check steady-state.
Pole-Zero Analysis
-
Poles: Roots of denominator of F(s). → System stability: All poles must have negative real parts for causal, stable system.
-
Zeros: Roots of numerator.
-
Pole-Zero Plot: s-plane with poles (X) and zeros (O). Shape of |F(jω)| determined by pole-zero locations.
Transfer Functions
-
Driving Point Impedance: Z(s) = V(s)/I(s) at a port with all other ports terminated.
-
Transfer Function (Gain): Ratio of output phasor to input phasor in s-domain, e.g., Voltage Gain = V<sub>2</sub>(s)/V<sub>1</sub>(s).
7. Two-Port Networks
Z-Parameters (Open-Circuit Impedance)
\boxed{
\begin{bmatrix}
V_1 \ V_2
\end{bmatrix}
= \begin{bmatrix}
Z_{11} & Z_{12} \
Z_{21} & Z_{22}
\end{bmatrix}
\begin{bmatrix}
I_1 \ I_2
\end{bmatrix}
}
-
Z<sub>11</sub> = V<sub>1</sub>/I<sub>1</sub> | I<sub>2</sub>=0 (input impedance with output open)
-
Z<sub>12</sub> = V<sub>1</sub>/I<sub>2</sub> | I<sub>1</sub>=0 (reverse transfer impedance)
-
Z<sub>21</sub> = V<sub>2</sub>/I<sub>1</sub> | I<sub>2</sub>=0 (forward transfer impedance)
-
Z<sub>22</sub> = V<sub>2</sub>/I<sub>2</sub> | I<sub>1</sub>=0 (output impedance with input open)
For reciprocal networks: Z<sub>12</sub> = Z<sub>21</sub>
Y-Parameters (Short-Circuit Admittance)
\boxed{
\begin{bmatrix}
I_1 \ I_2
\end{bmatrix}
= \begin{bmatrix}
Y_{11} & Y_{12} \
Y_{21} & Y_{22}
\end{bmatrix}
\begin{bmatrix}
V_1 \ V_2
\end{bmatrix}
}
-
Y<sub>ij</sub> = I<sub>i</sub>/V<sub>j</sub> with other port shorted.
-
Y = Z<sup>-1</sup>
h-Parameters (Hybrid)
\boxed{
\begin{bmatrix}
V_1 \ I_2
\end{bmatrix}
= \begin{bmatrix}
h_{11} & h_{12} \
h_{21} & h_{22}
\end{bmatrix}
\begin{bmatrix}
I_1 \ V_2
\end{bmatrix}
}
-
h<sub>11</sub> = Input impedance with output shorted (Ω).
-
h<sub>12</sub> = Reverse voltage gain with input shorted (dimensionless).
-
h<sub>21</sub> = Forward current gain with output shorted (dimensionless).
-
h<sub>22</sub> = Output admittance with input open (S).
ABCD Parameters (Transmission)
\boxed{
\begin{bmatrix}
V_1 \ I_1
\end{bmatrix}
= \begin{bmatrix}
A & B \
C & D
\end{bmatrix}
\begin{bmatrix}
V_2 \ -I_2
\end{bmatrix}
}
-
A = V<sub>1</sub>/V<sub>2</sub> | I<sub>2</sub>=0 (Open-circuit voltage ratio)
-
B = -V<sub>1</sub>/I<sub>2</sub> | V<sub>2</sub>=0 (Negative transfer impedance)
-
C = I<sub>1</sub>/V<sub>2</sub> | I<sub>2</sub>=0 (Transfer admittance)
-
D = I<sub>1</sub>/(-I<sub>2</sub>) | V<sub>2</sub>=0 (Short-circuit current ratio)
Cascade: Overall [A] = [A]<sub>1</sub>[A]<sub>2</sub> (matrix multiplication).
Parameter Conversions (Key Relationships)
| From \ To | Z | Y | h | ABCD |
|---|---|---|---|---|
| Z | - | Z = Y<sup>-1</sup> | h<sub>11</sub>=Z<sub>11</sub>, h<sub>12</sub>=ΔZ/Z<sub>22</sub>, h<sub>21</sub>=1/Z<sub>22</sub>, h<sub>22</sub>=Z<sub>22</sub>/ΔZ | A=Z<sub>11</sub>/Z<sub>21</sub>, B=ΔZ/Z<sub>21</sub>, C=1/Z<sub>21</sub>, D=Z<sub>22</sub>/Z<sub>21</sub> |
| Y | Y<sup>-1</sup> | - | h<sub>11</sub>=1/Y<sub>11</sub>, h<sub>12</sub>=-Y<sub>12</sub>/Y<sub>11</sub>, h<sub>21</sub>=Y<sub>21</sub>/Y<sub>11</sub>, h<sub>22</sub>=ΔY/Y<sub>11</sub> | A=Y<sub>22</sub>/Y<sub>12</sub>, B=1/Y<sub>12</sub>, C=ΔY/Y<sub>12</sub>, D=Y<sub>11</sub>/Y<sub>12</sub> |
| h | See Z column | See Y column | - | A = h<sub>11</sub>/(h<sub>21</sub>Δh), B = Δh/h<sub>21</sub>, C = h<sub>21</sub>/Δh, D = h<sub>22</sub>/h<sub>21</sub> |
| ABCD | A = D - BC? | - |
- ΔZ = Z<sub>11</sub>Z<sub>22</sub> - Z<sub>12</sub>Z<sub>21</sub>, similarly for ΔY, Δh.
Terminated Two-Port Network
- Input Impedance with Load Z<sub>L</sub>:
$$Z_{in} = \frac{AV_2 + B(-I_2)}{CV_2 + D(-I_2)} = \frac{AZ_L + B}{CZ_L + D} \quad (\text{using } V_2 = -I_2 Z_L)$$
- Voltage Gain:
$$A_v = \frac{V_2}{V_1} = \frac{1}{A + B/Z_L} \quad (\text{if } I_1=0)$$
- Current Gain:
$$A_i = \frac{I_2}{I_1} = \frac{1}{C Z_L + D} \quad (\text{if } V_2=0)$$
8. Special Topics for Short Notes
Controlled Sources (Dependent Sources)
| Type | Symbol | Controlling Variable | Output Variable |
|---|---|---|---|
| VCVS | ⊛⏚ | Voltage | Voltage |
| VCCS | ⊛⏚⏚ | Voltage | Current |
| CCVS | ⊛⏚ | Current | Voltage |
| CCCS | ⊛⏚⏚ | Current | Current |
Used to model transistors and amplifiers.
Dual Networks
-
Principle: Every theorem/equation in a network has a dual obtained by replacing:
-
Voltage ↔ Current
-
Series ↔ Parallel
-
Resistance ↔ Conductance
-
Inductance ↔ Capacitance
-
Open circuit ↔ Short circuit
-
KVL ↔ KCL
-
-
Dual Circuit: Topologically identical graph, but with dual elements.
Network Topology Summary
-
Graph: Connectivity only.
-
Tree: Loopless, connects all nodes. (n-1) twigs.
-
Link: Branch not in tree. (b-n+1) links.
-
Fundamental Loop: One link + tree branches.
-
Fundamental Cut: One twig + links.
-
Matrices: Incidence (A), Tie Set (B<sub>f</sub>), Cut Set (Q<sub>f</sub>). Relationships: B<sub>f</sub>A=0, Q<sub>f</sub>A=I.
S-Domain Theorems
-
Initial/Final Value Theorems: As above.
-
Convolution Theorem: Time-domain convolution ↔ s-domain multiplication.
-
Superposition: Holds in s-domain for linear circuits.
-
Thevenin/Norton: Valid with s-domain equivalents (Z<sub>TH</sub>(s), V<sub>TH</sub>(s)).