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Electronic Circuits & Networks (4331101) - Winter 2023 Solution

15 mins· ·
Study-Material Solutions Electronic-Circuits Networks 4331101 2023 Winter
Milav Dabgar
Author
Milav Dabgar
Experienced lecturer in the electrical and electronic manufacturing industry. Skilled in Embedded Systems, Image Processing, Data Science, MATLAB, Python, STM32. Strong education professional with a Master’s degree in Communication Systems Engineering from L.D. College of Engineering - Ahmedabad.
Table of Contents

Question 1(a) [3 marks]
#

Explain Source transformation with appropriate diagram.

Answer: Source transformation is a technique to convert voltage source to current source or vice-versa without changing the external circuit behavior.

Diagram:

graph LR
    subgraph "Voltage Source Circuit"
    VS[V] --- RS[R]
    end
    subgraph "Current Source Circuit"
    IS[I] -.- RP[R]
    end

    VS --- IS
    
    class VS,IS fill:#f96
  • Voltage to Current Source: I = V/R, same R in parallel
  • Current to Voltage Source: V = I×R, same R in series

Mnemonic: “Value Stays, Resistance Shifts” (V=IR always applies)

Question 1(b) [4 marks]
#

Determine voltage, current and power relationship for two capacitor connected in series.

Answer:

Table: Capacitors in Series

ParameterFormulaExplanation
Total Capacitance1/CT = 1/C₁ + 1/C₂Reciprocal sum
Voltage DistributionV₁/V₂ = C₂/C₁Inverse to capacitance ratio
CurrentI = I₁ = I₂Same current flows through all
ChargeQ = Q₁ = Q₂Same charge on each capacitor
PowerP = VI = V²/XcWhere Xc = 1/2πfC
  • Voltage division: V₁ = V × C₂/(C₁+C₂)
  • Charge storage: Q = C₁C₂V/(C₁+C₂)

Mnemonic: “Capacitors in Series: Currents Same, Capacitance Shrinks”

Question 1(c) [7 marks]
#

State difference between Series and parallel connection of resistor and derive the equation of total resistance of parallel connection.

Answer:

Table: Series vs Parallel Resistors

ParameterSeries ConnectionParallel Connection
Total ResistanceIncreases (RT = R₁ + R₂ + …)Decreases (RT < smallest R)
CurrentSame through all (I)Divides (IT = I₁ + I₂ + …)
VoltageDivides (VT = V₁ + V₂ + …)Same across all (V)
PowerPT = P₁ + P₂ + …PT = P₁ + P₂ + …

Derivation for Parallel Resistance:

By Kirchhoff’s Current Law: IT = I₁ + I₂ + … + In

Substituting I = V/R: V/RT = V/R₁ + V/R₂ + … + V/Rn

Dividing by V: 1/RT = 1/R₁ + 1/R₂ + … + 1/Rn

For two resistors: 1/RT = 1/R₁ + 1/R₂, which gives RT = R₁R₂/(R₁+R₂)

Mnemonic: “In Parallel, Reciprocals Add”

Question 1(c) OR [7 marks]
#

1) Define unilateral, bilateral network, Mesh and Loop. 2) Draw voltage division circuit and write equation.

Answer:

Table: Network Definitions

TermDefinitionExample
Unilateral NetworkAllows current in one direction onlyDiode circuit
Bilateral NetworkAllows current in both directionsRLC circuit
MeshPlanar network path with no other path inside itSingle closed path
LoopAny closed path in a networkCan contain other elements

Voltage Division Circuit:

graph TD
    A[Input] --- R1[R₁] --- B[Output V₀] --- R2[R₂] --- C[Ground]

Voltage Division Equation: Vo = Vin × R₂/(R₁+R₂)

  • Proportional to: Resistance across which voltage is measured
  • Inversely proportional to: Total resistance

Mnemonic: “Voltage Output equals Input times Resistance Ratio”

Question 2(a) [3 marks]
#

Derive equations to convert T-type network into π-type network

Answer:

Diagram: T to π Conversion

AZCZBZ=>AZCZB

Conversion Equations:

  • Z₁₂ = (Z₁Z₂ + Z₂Z₃ + Z₃Z₁)/Z₃
  • Z₂₃ = (Z₁Z₂ + Z₂Z₃ + Z₃Z₁)/Z₁
  • Z₃₁ = (Z₁Z₂ + Z₂Z₃ + Z₃Z₁)/Z₂

Where Z₁, Z₂, Z₃ are T-network impedances and Z₁₂, Z₂₃, Z₃₁ are π-network impedances.

Mnemonic: “Sum of all products divided by the opposite”

Question 2(b) [4 marks]
#

Explain Open circuit Impedance Parameter (Z Parameter)

Answer:

Z-Parameters: Also called open-circuit impedance parameters because they’re measured with output ports open.

Table: Z-Parameter Equations

ParameterDefinitionCalculation
Z₁₁Input impedance with output openZ₁₁ = V₁/I₁ (when I₂=0)
Z₁₂Transfer impedance from port 2 to port 1Z₁₂ = V₁/I₂ (when I₁=0)
Z₂₁Transfer impedance from port 1 to port 2Z₂₁ = V₂/I₁ (when I₂=0)
Z₂₂Output impedance with input openZ₂₂ = V₂/I₂ (when I₁=0)

Matrix Form: [V₁] = [Z₁₁ Z₁₂] × [I₁] [V₂] [Z₂₁ Z₂₂] [I₂]

  • Symmetrical Network: Z₁₂ = Z₂₁
  • Units: Ohms (Ω)

Mnemonic: “Vs equal Zs times Is”

Question 2(c) [7 marks]
#

Derive the expressions for the characteristic impedance (Z₀ₜ) for Symmetrical T Network.

Answer:

Diagram: Symmetrical T-Network

ZZ/2ZZ2Z

Derivation:

  1. For symmetrical T-network, Z₁ is split equally across two arms (Z₁/2 each)
  2. For image impedance matching: Z₀ₜ = Z₀ₜ′

By voltage division: V₂/V₁ = Z₀ₜ/(Z₁/2 + Z₀ₜ + Z₂||Z₀ₜ)

For matched condition: Z₀ₜ² = (Z₁/2)(Z₁/2 + Z₂)

Therefore: Z₀ₜ = √[(Z₁/2)(Z₁/2 + Z₂)] Z₀ₜ = √[Z₁²/4 + Z₁Z₂/2] Z₀ₜ = √[Z₁(Z₁+2Z₂)/4]

Mnemonic: “The square root of Z₁ times what Z₁ meets”

Question 2(a) OR [3 marks]
#

Derive equations to convert π-type network into T-type network.

Answer:

Diagram: π to T Conversion

AZCZB=>AZCZBZ

Conversion Equations:

  • Z₁ = (Z₁₂Z₃₁)/(Z₁₂ + Z₂₃ + Z₃₁)
  • Z₂ = (Z₂₃Z₁₂)/(Z₁₂ + Z₂₃ + Z₃₁)
  • Z₃ = (Z₃₁Z₂₃)/(Z₁₂ + Z₂₃ + Z₃₁)

Where Z₁₂, Z₂₃, Z₃₁ are π-network impedances and Z₁, Z₂, Z₃ are T-network impedances.

Mnemonic: “Product of adjacent pairs divided by sum of all”

Question 2(b) OR [4 marks]
#

Explain Admittance Parameter (Y Parameter).

Answer:

Y-Parameters: Also called short-circuit admittance parameters because they’re measured with output ports shorted.

Table: Y-Parameter Equations

ParameterDefinitionCalculation
Y₁₁Input admittance with output shortedY₁₁ = I₁/V₁ (when V₂=0)
Y₁₂Transfer admittance from port 2 to port 1Y₁₂ = I₁/V₂ (when V₁=0)
Y₂₁Transfer admittance from port 1 to port 2Y₂₁ = I₂/V₁ (when V₂=0)
Y₂₂Output admittance with input shortedY₂₂ = I₂/V₂ (when V₁=0)

Matrix Form: [I₁] = [Y₁₁ Y₁₂] × [V₁] [I₂] [Y₂₁ Y₂₂] [V₂]

  • Symmetrical Network: Y₁₂ = Y₂₁
  • Units: Siemens (S)

Mnemonic: “Is equal Ys times Vs”

Question 2(c) OR [7 marks]
#

Derive the expressions for the characteristic impedance (Z₀π) for Symmetrical π Network.

Answer:

Diagram: Symmetrical π-Network

2Z-Zπ---Z--Zπ--2-Z

Derivation:

  1. For symmetrical π-network, admittance Y₁ in shunt arms is split into 2 equal parts (Y₃ = Y₁/2)
  2. For image impedance matching: Z₀π = Z₀π′

By current division: I₂/I₁ = Z₀π/(Z₀π + Z₁ + Z₀π||2Z₃)

For matched condition: Z₀π² = Z₁(2Z₃)/(Z₁ + 2Z₃)

Simplifying: Z₀π = √[Z₁(2Z₃)/(Z₁ + 2Z₃)] Z₀π = √[2Z₁Z₃/(Z₁ + 2Z₃)]

Mnemonic: “Pi’s impedance equals the geometric mean of what it sees”

Question 3(a) [3 marks]
#

Explain principal of duality.

Answer:

Principle of Duality: For every electrical network, there exists a dual network with similar behavior but with interchanged elements.

Table: Dual Element Pairs

Original CircuitDual Circuit
Voltage (V)Current (I)
Current (I)Voltage (V)
Resistance (R)Conductance (G)
Inductance (L)Capacitance (C)
Series ConnectionParallel Connection
KVLKCL
Mesh AnalysisNodal Analysis
  • Network Transformation: Replace each element with its dual
  • Topology Transformation: Replace each node with a loop and each loop with a node

Mnemonic: “Series to Parallel, Source turns dual, V becomes I and I becomes V”

Question 3(b) [4 marks]
#

State and Explain Thevenin’s Theorem.

Answer:

Thevenin’s Theorem: Any linear two-terminal network can be replaced by an equivalent circuit consisting of a voltage source (Vth) in series with a resistance (Rth).

Diagram:

graph LR
    subgraph "Original Network"
    A[Complex Network] --- R1[Load]
    end
    subgraph "Thevenin Equivalent"
    VTH[Vth] --- RTH[Rth] --- RL[Load]
    end

Finding Thevenin Equivalent:

  1. Remove the load resistance
  2. Calculate open-circuit voltage (Vth)
  3. Find Rth by:
    • Deactivating all sources (V=0, I=0)
    • Calculate resistance between terminals

Mnemonic: “Open for Voltage, Dead for Resistance”

Question 3(c) [7 marks]
#

State and explain KCL and KVL with example.

Answer:

Table: Kirchhoff’s Laws

LawStatementMathematical FormApplication
KCLSum of currents entering a node equals sum of currents leaving it∑Iin = ∑IoutNode Analysis
KVLSum of voltage drops around any closed loop equals zero∑V = 0Mesh Analysis

KCL Example:

AtnoIde:III=I+I

KVL Example:

AroVundloRop:VR-I×R-I×R=0

Mnemonic: “Currents at nodes sum to zero, Voltages round loops also do”

Question 3(a) OR [3 marks]
#

Explain the solution of a network by Mesh Analysis.

Answer:

Mesh Analysis: A circuit analysis method that uses mesh currents as variables to solve for unknown currents and voltages.

Diagram: Simple Two-Mesh Circuit

VMesRh1RMeRsh2V

Steps:

  1. Identify meshes (closed loops)
  2. Assign clockwise mesh currents (I₁, I₂)
  3. Apply KVL to each mesh
  4. Solve the resulting simultaneous equations

Example Equations:

  • Mesh 1: V₁ = I₁(R₁+R₂) - I₂R₂
  • Mesh 2: -V₂ = -I₁R₂ + I₂(R₂+R₃)

Mnemonic: “Assign, Apply KVL, Arrange, and Solve”

Question 3(b) OR [4 marks]
#

State and Explain Norton’s Theorem.

Answer:

Norton’s Theorem: Any linear two-terminal network can be replaced by an equivalent circuit consisting of a current source (IN) in parallel with a resistance (RN).

Diagram:

graph LR
    subgraph "Original Network"
    A[Complex Network] --- R1[Load]
    end
    subgraph "Norton Equivalent"
    IN[In] -.- RN[Rn] --- RL[Load]
    end

Finding Norton Equivalent:

  1. Remove the load resistance
  2. Calculate short-circuit current (IN)
  3. Find RN by:
    • Deactivating all sources (V=0, I=0)
    • Calculate resistance between terminals (RN = Rth)

Mnemonic: “Short for Current, Dead for Resistance”

Question 3(c) OR [7 marks]
#

State and explain Maximum power transfer theorem. Derive condition for maximum power transfer.

Answer:

Maximum Power Transfer Theorem: A load receives maximum power when its resistance equals the Thevenin equivalent resistance of the network.

Diagram:

graph LR
    A[Vth] --- B[Rth] --- C[RL]

Derivation:

  1. Power delivered to load: P = I²RL

  2. Current through circuit: I = Vth/(Rth + RL)

  3. Substituting: P = Vth²RL/(Rth + RL

  4. Differentiating with respect to RL and setting to zero: dP/dRL = 0

  5. This gives: RL = Rth

  6. Maximum power: Pmax = Vth²/(4Rth)

Mnemonic: “Match to maximize”

Question 4(a) [3 marks]
#

Derive equation of Q factor for coil.

Answer:

Q Factor (Quality Factor) for a coil represents the ratio of inductive reactance to resistance.

Diagram: Coil with Resistance

R-uuLuu----o

Derivation:

  1. For an inductor with resistance, impedance Z = R + jωL
  2. Q factor is defined as: Q = Reactive Power / Active Power
  3. Q = ωL/R

Where:

  • L = Inductance in Henries
  • R = Series resistance in Ohms
  • ω = 2πf, Angular frequency

Mnemonic: “Quality equals Reactance over Resistance”

Question 4(b) [4 marks]
#

Derive the formula for resonant frequency for a parallel RLC circuit.

Answer:

Diagram: Parallel RLC Circuit

RCL

Derivation:

  1. Admittance of parallel RLC: Y = 1/R + jωC + 1/jωL = 1/R + j(ωC - 1/ωL)
  2. At resonance, imaginary part is zero: ωC - 1/ωL = 0
  3. Solving for ω: ω² = 1/LC
  4. Therefore: ω = 1/√(LC)
  5. Resonance frequency: fr = 1/(2π√(LC))

Note: R affects bandwidth but not resonance frequency.

Mnemonic: “One over Two Pi times Square Root of LC”

Question 4(c) [7 marks]
#

Write types of coupled circuits with necessary diagram and explain iron core transformer.

Answer:

Table: Types of Coupled Circuits

TypeCoupling MediumApplication
Direct CouplingConductively connectedDC amplifiers
Capacitive CouplingCapacitorAC signal coupling
Inductive CouplingMagnetic fieldTransformers
Resistive CouplingResistorLow-frequency signals

Diagram: Iron Core Transformer

graph LR
    subgraph "Primary"
    V1[V₁] --- L1[uuuu]
    end

    subgraph "Iron Core"
    Core[" "]
    end
    
    subgraph "Secondary"
    L2[uuuu] --- V2[V₂]
    end
    
    L1 --- Core --- L2

Iron Core Transformer:

  • Principle: Mutual inductance through iron core
  • Function: Transfers energy between circuits by electromagnetic induction
  • Coupling Coefficient: k ≈ 1 (near perfect coupling)
  • Turns Ratio: V₂/V₁ = N₂/N₁
  • Advantages: High efficiency, good coupling

Mnemonic: “Primary excites, Core conducts, Secondary delivers”

Question 4(a) OR [3 marks]
#

Derive equation of Q factor for capacitor.

Answer:

Q Factor (Quality Factor) for a capacitor represents the ratio of capacitive reactance to resistance.

Diagram: Capacitor with Resistance

RC

Derivation:

  1. For a capacitor with series resistance, impedance Z = R - j/(ωC)
  2. Q factor is defined as: Q = Reactive Power / Active Power
  3. Q = 1/(ωCR)

Where:

  • C = Capacitance in Farads
  • R = Series resistance in Ohms
  • ω = 2πf, Angular frequency

Mnemonic: “Quality equals One over Resistance times Reactance”

Question 4(b) OR [4 marks]
#

Derive the equation of resonance frequency for a series resonance circuit.

Answer:

Diagram: Series RLC Circuit

R-uuLuu----||C----o

Derivation:

  1. Impedance of series RLC: Z = R + jωL - j/(ωC) = R + j(ωL - 1/ωC)
  2. At resonance, imaginary part is zero: ωL - 1/ωC = 0
  3. Solving for ω: ω² = 1/LC
  4. Therefore: ω = 1/√(LC)
  5. Resonance frequency: fr = 1/(2π√(LC))

Key Points:

  • At resonance, impedance is purely resistive: Z = R
  • Circuit appears as a resistor
  • Current is maximum at resonance

Mnemonic: “One over Two Pi times Square Root of LC”

Question 4(c) OR [7 marks]
#

Derive the Expression for coefficient coupling between pair of magnetically coupled coils.

Answer:

Diagram: Magnetically Coupled Coils

-uWLuWuWuW---k----uWuWLuWuW--o

Derivation:

  1. Mutual inductance (M) relates to individual inductances by: M = k√(L₁L₂)
  2. Solving for k: k = M/√(L₁L₂)

Where:

  • k = Coefficient of coupling (0 ≤ k ≤ 1)
  • M = Mutual inductance in Henries
  • L₁, L₂ = Self-inductances of coils in Henries

Table: Coupling Coefficient Values

Value of kCoupling TypeApplication
k = 0No couplingSeparate circuits
0 < k < 0.5Loose couplingRF transformers
0.5 < k < 1Tight couplingPower transformers
k = 1Perfect couplingIdeal transformer

Mnemonic: “Mutual over square root of product”

Question 5(a) [3 marks]
#

Define Neper and dB. Establish relationship between Neper and dB.

Answer:

Table: Neper and dB Definitions

UnitDefinitionFormulaUsage
Neper (Np)Natural logarithmic ratioN = ln(V₁/V₂) or ln(I₁/I₂)Power system analysis
Decibel (dB)Common logarithmic ratiodB = 20log₁₀(V₁/V₂) or 10log₁₀(P₁/P₂)Signal level measurement

Relationship:

  1. N = ln(V₁/V₂)
  2. dB = 20log₁₀(V₁/V₂)
  3. Since ln(x) = 2.303 × log₁₀(x)
  4. Therefore: N = 2.303 × dB/20 = 0.1152 × dB
  5. Conversely: dB = 8.686 × N

Mnemonic: “A Neper is 8.686 dB”

Question 5(b) [4 marks]
#

Classify various types of Attenuators.

Answer:

Table: Types of Attenuators

TypeStructureCharacteristicsApplications
T-typeThree resistors in T formationFixed impedance, good balanceSignal level control
π-type (Pi)Three resistors in π formationBetter isolation, more commonRF signal attenuation
L-typeTwo resistors in L formationSimple, unbalancedBasic level adjustment
Bridged TT with bridging resistorConstant impedanceAudio applications
BalancedSymmetrical designGood CMRRBalanced transmission
LatticeDiamond-shapedBalanced, symmetricalTelephone systems

Diagram: Basic Attenuator Types

graph TD
    subgraph "T-type"
    T1[o]---TR1[R₁]---T2[o]
    TR2[R₂]
    T2---TR2---T3[o]
    end

    subgraph "π-type"
    P1[o]---PR1[R₁]---P2[o]
    PR2[R₂]
    P1---PR2
    PR3[R₃]
    PR2---P2
    end

Mnemonic: “Tees, Pies and Ells attenuate the signals well”

Question 5(c) [7 marks]
#

Determine the cut-off frequency and the nominal impedance of each of the low-pass filter sections shown below.

Answer:

Diagram: Low-Pass Filter Sections

T-se-cLt/i2o-n-:-Co---L/2---oπC-/s2ec-tLi-o-n-:--o-----------Co/2

For T-section:

  • Cut-off frequency: fc = 1/(π√(LC))
  • Nominal impedance: R₀ = √(L/C)
  • Where L = 10 mH, C = 0.1 μF

Calculation: fc = 1/(π√(10×10⁻³ × 0.1×10⁻⁶)) = 1/(π√(10⁻⁹)) = 1/(π×10⁻⁴·⁵) = 3.18 kHz R₀ = √(10×10⁻³/0.1×10⁻⁶) = √(10⁵) = 316.23 Ω

For π-section:

  • Cut-off frequency: fc = 1/(π√(LC))
  • Nominal impedance: R₀ = √(L/C)
  • Same values as T-section

Mnemonic: “Cut-off frequency is inverse to the square root of LC”

Question 5(a) OR [3 marks]
#

Explain the limitation of constant k type filters.

Answer:

Table: Limitations of Constant-k Filters

LimitationDescriptionEffect
Impedance MatchingImpedance varies with frequencySignal reflection, power loss
Attenuation BandGradual transition at cut-offPoor frequency selectivity
Phase ResponseNon-linear phase characteristicSignal distortion
Passband RippleNon-uniform response in passbandSignal amplitude variation
Roll-off RateSlow roll-off (20 dB/decade)Poor stop-band rejection
  • Main issue: Poor transition from pass to stop band
  • Improvement: Using m-derived filters

Mnemonic: “Poor Matching And Transition Results In Distortion”

Question 5(b) OR [4 marks]
#

Derive equation of cut-off frequency for T-type Constant-k high Pass filter.

Answer:

Diagram: T-type Constant-k High Pass Filter

-C/2---L-o----C/2----o

Derivation:

  1. For high-pass filter, series elements are capacitors and shunt elements are inductors
  2. Transfer function: H(jω) = Z₂/(Z₁ + Z₂)
  3. Where Z₁ = 1/(jωC) and Z₂ = jωL
  4. Impedance condition for cut-off: Z₁/Z₂ = 4 or Z₁/4Z₂ = 1
  5. Substituting: 1/(jωC) = 4jωL
  6. Solving for ω: ω² = 1/(4LC)
  7. Cut-off frequency: fc = 1/(4π√(LC))

Mnemonic: “High Pass cuts frequencies below one over four pi L-C”

Question 5(c) OR [7 marks]
#

Give classification of filters using definitions and characteristics graphs for each.

Answer:

Table: Filter Classification

Filter TypePassesBlocksApplications
Low-PassFrequencies below fcFrequencies above fcAudio amplifiers, power supplies
High-PassFrequencies above fcFrequencies below fcNoise elimination, treble control
Band-PassRange between fL and fHFrequencies outside rangeRadio tuning, equalizers
Band-StopFrequencies outside rangeRange between fL and fHNoise elimination, notch filters
All-PassAll frequencies with unity gainNone (changes only phase)Phase correction, time delay

Characteristic Response Graphs:

graph LR
    subgraph "Low-Pass"
    LP[High

Gain

Low] --- LPf[Frequency →] style LP stroke-width:0, fill:#fff style LPf stroke-width:0, fill:#fff end subgraph "High-Pass" HP[High

Gain

Low] --- HPf[Frequency →] style HP stroke-width:0, fill:#fff style HPf stroke-width:0, fill:#fff end subgraph "Band-Pass" BP[High

Gain

Low] --- BPf[Frequency →] style BP stroke-width:0, fill:#fff style BPf stroke-width:0, fill:#fff end subgraph "Band-Stop" BS[High

Gain

Low] --- BSf[Frequency →] style BS stroke-width:0, fill:#fff style BSf stroke-width:0, fill:#fff end

Filter Implementations:

  • Passive: Uses R, L, C components
  • Active: Uses op-amps with RC networks
  • Digital: Uses DSP algorithms

Mnemonic: “Low-High-Band-Stop makes Signals Perfect”

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