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EC-305 · Network Analysis/Quick Revision Short Notes

Network Analysis (EC-305) - Unit 5 Short Notes

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)

  1. Identify independent meshes (windows).

  2. Apply KVL to each mesh, expressing voltages in terms of mesh currents.

  3. 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

  1. Select a reference node (ground).

  2. Assign node voltages to remaining (n-1) nodes.

  3. Apply KCL at each non-reference node, expressing currents in terms of node voltages.

  4. 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

  1. Write KVL for each mesh, including mutual terms using dot convention.

  2. 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)

  1. Draw s-domain circuit. Replace L, C with their impedances including IC sources.

  2. Apply circuit laws (KVL/KCL) to find desired variable (I(s), V(s)).

  3. Simplify F(s) using partial fractions.

  4. Apply inverse LT (using tables or pole-zero) to get f(t).

  5. 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)).

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