UNIT 4: Network Analysis - Short Notes
I. Fundamental Laws and Basic Concepts
Kirchhoff's Current Law (KCL)
Statement: The algebraic sum of currents meeting at any node (junction) in a network is zero.
$$ \sum_{k=1}^{n} I_k = 0 $$
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Explanation: Based on conservation of charge. Currents entering a node are positive; currents leaving are negative (or vice-versa, but consistency is key).
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Example: For a node with three branches, if $$\displaystyle I_1 $$ enters and $$\displaystyle I_2 $$, $$\displaystyle I_3 $$ leave, then $$\displaystyle I_1 - I_2 - I_3 = 0 $$ or $$\displaystyle I_1 = I_2 + I_3 $$.
Kirchhoff's Voltage Law (KVL)
Statement: The algebraic sum of voltages around any closed loop in a network is zero.
$$ \sum_{k=1}^{m} V_k = 0 $$
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Explanation: Based on conservation of energy. Assign polarity signs to voltage drops; traverse the loop in one direction.
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Example: For a loop with a voltage source $$\displaystyle V_s $$ and two resistors with drops $$\displaystyle V_1 $$, $$\displaystyle V_2 $$, traversing from - to + across $$\displaystyle V_s $$ gives $$\displaystyle +V_s - V_1 - V_2 = 0 $$.
II. Graph Theory and Network Topology
Graph and Oriented Graph
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Graph: A representation of a circuit where branches (circuit elements) are shown as lines and nodes (connection points) as dots. It ignores physical layout.
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Oriented Graph: A graph with directions (arrows) assigned to all branches. Used for analysis (e.g., KCL/KVL equations).
Tree and Co-Tree
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Tree: A connected subgraph of a graph that includes all nodes but no closed loops. Number of twigs (tree branches) = $b - n + 1$, where $b$ = total branches, $n$ = total nodes.
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Co-Tree: The set of branches not in the tree. Each branch in the co-tree is a link or chord. Links = $n - 1$.
Twigs and Links
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Twigs: Branches that form the tree.
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Links (Chords): Branches that form the co-tree.
Cut Set and Basic Cut Set Matrix
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Cut Set: A minimal set of branches whose removal disconnects the graph into exactly two parts, with one branch from each remaining tree branch.
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Basic Cut Set Matrix ($Q$): A matrix where rows represent fundamental cut sets (one twig removed, rest are links). Entries: $+1$ if branch leaves the isolated part, $-1$ if it enters, $0$ otherwise. For a graph with $n$ nodes, there are $(n-1)$ fundamental cut sets.
Tie Set and Basic Tie Set Matrix
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Tie Set (Loop): A minimal set of branches forming a closed loop with exactly one link and the remaining twigs.
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Basic Tie Set Matrix ($B$): Rows represent fundamental tie sets. Entries: $+1$ if branch direction matches loop direction, $-1$ if opposite, $0$ if not in loop. Number of fundamental tie sets = $b - n + 1$ (links).
Incidence Matrix (Complete Incidence Matrix $A$)
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Definition: A matrix representing the connection between branches and nodes.
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Construction: Rows = nodes ($n$), Columns = branches ($b$). For branch $k$ connecting node $i$ to $j$:
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$$\displaystyle A_{ik} = +1 $$ (branch leaves node $i$)
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$$\displaystyle A_{jk} = -1 $$ (branch enters node $j$)
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All other entries = 0.
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Property: Sum of elements in any column = 0 (KCL). Rank = $n-1$ for a connected graph.
Network Topology
- Significance: Provides a systematic, algebraic method (via matrices $A$, $B$, $Q$) to write KCL/KVL equations without drawing loops/nodes repeatedly. Essential for computer-aided circuit analysis.
III. Circuit Theorems
Thevenin's Theorem (DC & AC)
Statement: Any linear bilateral network can be replaced by an equivalent circuit consisting of a voltage source $$\displaystyle V_{th} $$ in series with an impedance $$\displaystyle Z_{th} $$.
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Procedure:
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Remove load. Find $$\displaystyle V_{th} $$ = open-circuit voltage across terminals.
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Find $$\displaystyle Z_{th} $$:
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DC: $$\displaystyle Z_{th} = R_{th} $$ = (V_oc / I_sc) or deactivate independent sources.
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AC: $$\displaystyle Z_{th} $$ = (V_oc / I_sc) with phasors; deactivate independent sources.
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Connect load $$\displaystyle Z_L $$ to $$\displaystyle V_{th} $$ and $$\displaystyle Z_{th} $$.
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Key: $$\displaystyle V_{th} $$ is the open-circuit voltage; $$\displaystyle Z_{th} $$ is the impedance seen into the network with sources killed.
Norton's Theorem (DC & AC)
Statement: Any linear bilateral network can be replaced by an equivalent circuit consisting of a current source $$\displaystyle I_N $$ in parallel with an impedance $$\displaystyle Z_N $$.
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Procedure:
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Remove load. Find $$\displaystyle I_N $$ = short-circuit current across terminals.
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Find $$\displaystyle Z_N $$ = $$\displaystyle Z_{th} $$ (same as Thevenin).
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Connect load $$\displaystyle Z_L $$ to $$\displaystyle I_N $$ and $$\displaystyle Z_N $$.
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Relation: $$\displaystyle I_N = V_{th} / Z_{th} $$, $$\displaystyle Z_N = Z_{th} $$.
Superposition Theorem
Statement: In a linear circuit with multiple independent sources, the response (voltage/current) in any branch is the algebraic sum of the responses caused by each independent source acting alone, with all other independent sources deactivated (voltage sources shorted, current sources opened).
- Application: Useful for circuits with one source at a time. Not applicable for power calculations (non-linear).
Maximum Power Transfer Theorem (DC)
Condition: Maximum power is delivered to the load when load resistance $$\displaystyle R_L $$ equals Thevenin resistance $$\displaystyle R_{th} $$ seen from the load terminals.
$$ R_L = R_{th} $$
- Maximum Power:
$$ P_{max} = \frac{V_{th}^2}{4 R_{th}} $$
- Efficiency Proof: Efficiency $$\displaystyle \eta = \frac{P_L}{P_{total}} $$. At max power, $$\displaystyle P_L = V_{th}^2/(4R_{th}) $$, $$\displaystyle P_{total} = V_{th}^2/R_{th} $$. Thus $$\displaystyle \eta = 0.5 $$ or 50%.
[!TIP] Efficiency is 50% only at maximum power condition. For higher efficiency, $$\displaystyle R_L > R_{th} $$.
Tellegen's Theorem
Statement: For any two networks (not necessarily the same) that have the same topology (same incidence matrix), the following holds:
$$ \sum_{k=1}^{b} v_k i_k = 0 $$
where $$\displaystyle v_k $$ and $$\displaystyle i_k $$ are branch voltages and currents of the two networks respectively.
- Significance: A topological theorem independent of element characteristics. Used to verify network solutions and derive other theorems.
Millman's Theorem
Statement: For a circuit with several parallel branches, each containing a voltage source $$\displaystyle V_k $$ in series with impedance $$\displaystyle Z_k $$, the equivalent voltage $$\displaystyle V_{eq} $$ and impedance $$\displaystyle Z_{eq} $$ across the parallel combination are:
$$ V_{eq} = \frac{\sum_{k=1}^{n} \frac{V_k}{Z_k}}{\sum_{k=1}^{n} \frac{1}{Z_k}}, \quad Z_{eq} = \frac{1}{\sum_{k=1}^{n} \frac{1}{Z_k}} $$
- Application: Directly finds the common voltage in parallel voltage sources. For current sources, use dual form.
Substitution Theorem
Statement: 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 voltage and current, without affecting the rest of the network.
- Conditions: The replacing network must have identical $v$ and $i$ for the given branch. Useful for simplifying networks during analysis.
Compensation Theorem
Statement: If a branch with impedance $Z$ has a current $I$, and a voltage $$\displaystyle V = IZ $$ is injected in series opposition to $V$, the effect on the rest of the network is the same as replacing that branch with a voltage source of value $V$.
- Application: Network modification. Useful in sensitivity analysis and fault studies.
IV. Resonance
Series Resonant Circuit
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Circuit: $R$, $L$, $C$ in series with voltage source $V$.
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Resonance Condition: Impedance is purely resistive and minimum.
$$ X_L = X_C \implies \omega_0 L = \frac{1}{\omega_0 C} \implies \omega_0 = \frac{1}{\sqrt{LC}} $$
$$ f_0 = \frac{1}{2\pi\sqrt{LC}} $$
- Quality Factor (Q): Measure of sharpness.
$$ Q = \frac{\omega_0 L}{R} = \frac{1}{\omega_0 C R} = \frac{1}{R} \sqrt{\frac{L}{C}} $$
- Voltage Magnification: At resonance, voltage across $L$ or $C$ is $Q$ times the input voltage.
$$ |V_L| = |V_C| = Q \cdot V $$
Parallel Resonant Circuit
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Circuit: $R$, $L$, $C$ in parallel (often $R$ represents inductor resistance).
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Resonance Condition: Admittance is purely conductive and minimum (impedance maximum).
$$ B_L = B_C \implies \frac{1}{\omega_0 L} = \omega_0 C \quad \text{(if } R \text{ large)} \implies \omega_0 = \frac{1}{\sqrt{LC}} $$
- Admittance at Resonance: $$\displaystyle Y_{res} = 1/R_{eq} $$ (purely real). For ideal parallel RLC, $$\displaystyle Y_{res} = 1/R $$.
V. Laplace Transform Analysis
Laplace Transform of Standard Waveforms
| Waveform $f(t)$ | Laplace Transform $F(s)$ |
|---|---|
| Unit Step $u(t)$ | $$\displaystyle \frac{1}{s} $$ |
| Unit Impulse $\delta(t)$ | $1$ |
| Ramp $t \cdot u(t)$ | $$\displaystyle \frac{1}{s^2} $$ |
| Exponential $$\displaystyle e^{-at} u(t) $$ | $$\displaystyle \frac{1}{s+a} $$ |
| Sinusoid $\sin \omega t \cdot u(t)$ | $$\displaystyle \frac{\omega}{s^2 + \omega^2} $$ |
| Cosinusoid $\cos \omega t \cdot u(t)$ | $$\displaystyle \frac{s}{s^2 + \omega^2} $$ |
Application to RLC Circuits (Transient Analysis)
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Model circuit in s-domain:
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$$\displaystyle R \rightarrow R $$
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$$\displaystyle L \rightarrow sL + L i(0^-) $$ (voltage source in series)
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$$\displaystyle C \rightarrow \frac{1}{sC} + \frac{v_C(0^-)}{s} $$ (current source in parallel)
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Write KVL/KCL equations in s-domain.
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Solve for desired variable (e.g., $I(s)$).
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Apply Inverse Laplace to get $i(t)$.
Initial Value Theorem (IVT)
Statement: If $F(s)$ is the Laplace transform of $f(t)$, and $sF(s)$ has no poles in the right-half plane (RHP) and possibly a simple pole at $$\displaystyle s=0 $$, then:
$$ f(0^+) = \lim_{s \to \infty} s F(s) $$
- Application: Find initial value of $i(t)$ or $v(t)$ directly from $I(s)$ or $V(s)$.
Final Value Theorem (FVT)
Statement: If $sF(s)$ has no poles in the RHP and possibly a simple pole at $$\displaystyle s=0 $$, then:
$$ f(\infty) = \lim_{s \to 0} s F(s) $$
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Verification: Check poles of $sF(s)$. Fails if poles on imaginary axis (except origin) or in RHP.
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Example: For $$\displaystyle I(s) = \frac{2s+3}{(s+1)(s+3)} $$, poles at $$\displaystyle s=-1,-3 $$ (LHP). FVT applicable.
Transfer Function, Pole-Zero Plot, Inverse Laplace
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Driving Point Impedance: $$\displaystyle Z(s) = \frac{V(s)}{I(s)} $$ (ratio at same port).
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Transfer Function: $$\displaystyle H(s) = \frac{Output(s)}{Input(s)} $$ (e.g., $$\displaystyle V_2(s)/V_1(s) $$).
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Pole-Zero Plot: Plot poles ($\times$) and zeros ($\circ$) on s-plane. Determines stability and response shape.
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Inverse Laplace: Use partial fraction expansion and transform tables to obtain $i(t)$ or $v(t)$.
VI. Fourier Series Analysis
Trigonometric Fourier Series
For a periodic function $f(t)$ with period $T$ ($$\displaystyle \omega_0 = 2\pi/T $$):
$$ f(t) = a_0 + \sum_{n=1}^{\infty} \left( a_n \cos n\omega_0 t + b_n \sin n\omega_0 t \right) $$
Coefficients:
$$ a_0 = \frac{1}{T} \int_{0}^{T} f(t) dt \quad (\text{DC component}) $$
$$ a_n = \frac{2}{T} \int_{0}^{T} f(t) \cos n\omega_0 t \, dt $$
$$ b_n = \frac{2}{T} \int_{0}^{T} f(t) \sin n\omega_0 t \, dt $$
Exponential Fourier Series
$$ f(t) = \sum_{n=-\infty}^{\infty} c_n e^{j n \omega_0 t} $$
Coefficient:
$$ c_n = \frac{1}{T} \int_{0}^{T} f(t) e^{-j n \omega_0 t} dt $$
Relation to Trigonometric:
$$ c_n = \frac{1}{2} (a_n - j b_n), \quad c_{-n} = c_n^* $$
$$ a_0 = c_0, \quad a_n = c_n + c_{-n}, \quad b_n = j(c_n - c_{-n}) $$
VII. Two-Port Network Parameters
Z-Parameters (Impedance Parameters)
Definition: Open-circuit impedance parameters.
$$ V_1 = Z_{11} I_1 + Z_{12} I_2 $$
$$ V_2 = Z_{21} I_1 + Z_{22} I_2 $$
- Calculation: $$\displaystyle Z_{11} = \left. \frac{V_1}{I_1} \right|_{I_2=0} $$, $$\displaystyle Z_{12} = \left. \frac{V_1}{I_2} \right|_{I_1=0} $$, etc.
Y-Parameters (Admittance Parameters)
Definition: Short-circuit admittance parameters.
$$ I_1 = Y_{11} V_1 + Y_{12} V_2 $$
$$ I_2 = Y_{21} V_1 + Y_{22} V_2 $$
- Relation to Z: $$\displaystyle [Y] = [Z]^{-1} $$.
h-Parameters (Hybrid Parameters)
Definition: Mix of voltage and current.
$$ V_1 = h_{11} I_1 + h_{12} V_2 $$
$$ I_2 = h_{21} I_1 + h_{22} V_2 $$
- Common in transistor circuits. $$\displaystyle h_{11} $$: input impedance (V/I), $$\displaystyle h_{12} $$: reverse voltage gain, $$\displaystyle h_{21} $$: forward current gain, $$\displaystyle h_{22} $$: output admittance.
ABCD Parameters (Transmission Parameters)
Definition: Cascadable parameters.
$$ V_1 = A V_2 + B I_2 $$
$$ I_1 = C V_2 + D I_2 $$
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Cascade Property: For two networks in cascade, $$\displaystyle [ABCD]_{total} = [ABCD]_1 \cdot [ABCD]_2 $$.
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Relation to Z: $$\displaystyle A = \frac{Z_{11}}{Z_{21}} $$, $$\displaystyle B = \frac{Z_{11}Z_{22} - Z_{12}Z_{21}}{Z_{21}} $$, etc.
Conversions between Parameters (Key Relations)
| From \ To | Z | Y | h | ABCD |
|---|---|---|---|---|
| Z | - | $$\displaystyle [Z]=[Y]^{-1} $$ | $$\displaystyle h_{11}=Z_{11} $$, $$\displaystyle h_{12}=\frac{Z_{12}}{Z_{22}} $$... | $$\displaystyle A=\frac{Z_{11}}{Z_{21}} $$... |
| Y | $$\displaystyle [Y]=[Z]^{-1} $$ | - | $$\displaystyle h_{11}=\frac{Y_{22}}{Y_{12}Y_{21}} $$... | $$\displaystyle A=-\frac{Y_{22}}{Y_{21}} $$... |
| h | $$\displaystyle Z_{11}=h_{11} $$, $$\displaystyle Z_{12}=\frac{h_{12}}{h_{22}} $$... | $$\displaystyle Y_{11}=\frac{h_{22}}{\Delta_h} $$... | - | $$\displaystyle A=\frac{h_{11}}{h_{21}} $$, $$\displaystyle B=\frac{\Delta_h}{h_{21}} $$... |
| ABCD | $$\displaystyle Z_{11}=\frac{A}{C} $$, $$\displaystyle Z_{12}=\frac{AD-BC}{C} $$... | $$\displaystyle Y_{11}=\frac{D}{B} $$, $$\displaystyle Y_{12}=-\frac{1}{B} $$... | $$\displaystyle h_{11}=\frac{A}{C} $$, $$\displaystyle h_{12}=\frac{AD-BC}{C} $$... | - |
- $$\displaystyle \Delta_h = h_{11}h_{22} - h_{12}h_{21} $$, $$\displaystyle \Delta = AD - BC $$.
Terminated Two-Port Network
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Concept: A two-port network with a load $$\displaystyle Z_L $$ connected at output port 2.
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Analysis: Use two-port equations (e.g., Z-parameters) with $$\displaystyle V_2 = -Z_L I_2 $$ (assuming port 2 reference direction into network).
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Gain Calculations:
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Voltage Gain: $$\displaystyle A_v = \frac{V_2}{V_1} = \frac{-Z_L}{Z_{22} + Z_L} $$ (for Z-params).
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Current Gain: $$\displaystyle A_i = \frac{I_2}{I_1} $$.
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Power Gain: $$\displaystyle A_p = \frac{P_L}{P_{in}} $$.
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VIII. Additional Topics
Controlled Sources
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Types:
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VCVS: Voltage-Controlled Voltage Source ($$\displaystyle v_o = \mu v_c $$)
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VCCS: Voltage-Controlled Current Source ($$\displaystyle i_o = g v_c $$)
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CCVS: Current-Controlled Voltage Source ($$\displaystyle v_o = r i_c $$)
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CCCS: Current-Controlled Current Source ($$\displaystyle i_o = \beta i_c $$)
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Symbol: Diamond shape for controlled source. Controlling variable ($$\displaystyle v_c $$ or $$\displaystyle i_c $$) shown separately.
Mutual Inductance and Coefficient of Coupling
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Mutual Inductance ($M$): Voltage induced in one coil due to current change in another: $$\displaystyle v_1 = M \frac{di_2}{dt} $$.
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Coefficient of Coupling ($k$): Measures magnetic coupling between two coils.
$$ k = \frac{M}{\sqrt{L_1 L_2}}, \quad 0 \le k \le 1 $$
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Calculation from Inductance Measurements:
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Series aiding: $$\displaystyle L_{eq} = L_1 + L_2 + 2M $$
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Series opposing: $$\displaystyle L_{eq} = L_1 + L_2 - 2M $$
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Solve for $M$, then $k$.
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Dual Networks
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Concept: Two networks are duals if their equations are identical when dual quantities are exchanged.
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Duality Principle: Replace:
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Voltage $$\displaystyle \leftrightarrow $$ Current
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Resistance $$\displaystyle R \leftrightarrow $$ Conductance $G$
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Inductance $$\displaystyle L \leftrightarrow $$ Capacitance $C$
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Series $$\displaystyle \leftrightarrow $$ Parallel
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Open circuit $$\displaystyle \leftrightarrow $$ Short circuit
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Node $$\displaystyle \leftrightarrow $$ Mesh (Loop)
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Example: Series RLC circuit $$\displaystyle \leftrightarrow $$ Parallel GLC circuit.
s-Domain Superposition Theorem
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Clarification: In s-domain, Superposition Theorem still applies to linear circuits with independent sources (voltage/current sources in s-domain). Deactivate all but one independent source at a time (set to zero). Dependent sources remain active.
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Application: Simplifies solving circuits with multiple independent sources in transient analysis.
Exam Tips from Past Papers:
- KCL/KVL (Dec 24, Jun 23): Always draw a clear circuit, label currents/voltages with assumed directions/polarities. Write equations systematically.
- Graph Theory (Dec 24, Jun 23): Practice drawing trees, identifying twigs/links, and constructing $A$, $B$, $Q$ matrices for small graphs (3-4 nodes).
- Thevenin/Norton (Dec 24, Jun 24, Dec 23): Very frequent. Master finding $$\displaystyle V_{th}/I_N $$ and $$\displaystyle Z_{th} $$. For AC, use phasors.
- Superposition (Dec 24, Jun 23): Kill sources correctly (voltage source โ short, current source โ open). Remember: Do not kill dependent sources.
- Max Power (Jun 24, Dec 23): State condition $$\displaystyle R_L = R_{th} $$ clearly. Derive/state efficiency = 50%.
- Laplace (Jun 24, Dec 23, Nov 22): Be flawless in s-domain modeling (initial conditions as sources). Practice IVT/FVT with pole analysis.
- Fourier Series (Dec 24, Jun 23, Nov 22): Know both forms. For given waveform, write expression first, then compute $$\displaystyle a_0, a_n, b_n $$ or $$\displaystyle c_n $$.
- Two-Port (Dec 24, Jun 24, Dec 23): Be able to calculate Z/Y/h/ABCD from a given circuit. Conversions are crucial. For terminated networks, use correct two-port equation with load condition.
- Short Notes (Dec 24, Jun 24): Topics like Cut Set, Compensation, Incidence Matrix, Dual Networks, Terminated Two-Port are often asked for 7m. Prepare 3-4 bullet points with a key formula or example.