Skip to main content
  1. Resources/
  2. Study Materials/
  3. Electronics & Communication Engineering/
  4. ECE Semester 3/

Electronic Circuits & Networks (4331101) - Summer 2024 Solution

18 mins· ·
Study-Material Solutions Electronic-Circuits Networks 4331101 2024 Summer
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]
#

Define node, branch and loop with suitable diagram.

Answer:

Diagram:

graph TD
    A((Node A)) --- B{Branch 1}
    A --- C{Branch 2}
    A --- D{Branch 3}
    B --- E((Node B))
    C --- F((Node C))
    D --- G((Node D))
    E --- H{Branch 4}
    H --- F
    G --- I{Branch 5}
    I --- F

    subgraph Loop X
    A --> B --> E --> H --> F --> C --> A
    end

  • Node: A point where two or more circuit elements join together
  • Branch: A single element connecting two nodes
  • Loop: Any closed path in a circuit where no node is encountered more than once

Mnemonic: “NBA circuit” - Nodes are junctions, Branches are roads, Loops are Alternate paths

Question 1(b) [4 marks]
#

Explain “Tree” and “Graph” of a network.

Answer:

Diagram:

graph TD
    subgraph Network Graph
    A((A)) --- B((B))
    A --- C((C))
    B --- D((D))
    C --- D
    B --- C
    end

    subgraph Tree of Network
    E((A)) --- F((B))
    E --- G((C))
    F --- H((D))
    end

FeatureGraphTree
DefinitionComplete topological representation of networkConnected subgraph containing all nodes but no loops
ElementsContains all branches and nodesContains N-1 branches where N is number of nodes
LoopsContains loopsNo loops
ApplicationUsed for complete circuit analysisUsed for simplifying network calculations

Mnemonic: “GRAND Tree” - Graph has Routes And Nodes with Detours, Tree has only single Routes

Question 1(c) [7 marks]
#

Explain “Mesh current Method” using suitable diagram.

Answer:

Diagram:

graph LR
    subgraph Mesh 1
    A((+)) -- R1 --> B((+))
    B -- R3 --> C((+))
    C -- R5 --> A
    end

    subgraph Mesh 2
    B -- R2 --> D((+))
    D -- R4 --> C
    C -- R3 --> B
    end
    
    style Mesh 1 fill:#f9f,stroke:#333,stroke-width:2px
    style Mesh 2 fill:#bbf,stroke:#333,stroke-width:2px

StepDescription
1Identify independent meshes in the circuit
2Assign mesh currents (I₁, I₂, etc.) in clockwise direction
3Apply KVL to each mesh
4Form equations using: ΣR·I(own) - ΣR·I(adjacent) = ΣV
5Solve the simultaneous equations
  • Advantage: Fewer equations than branch current method
  • Application: Best for planar networks
  • Limitation: Less efficient for non-planar networks

Mnemonic: “MIAMI” - Meshes Identified, Assign currents, Make equations, Intersection currents calculated, Solve

Question 1(c OR) [7 marks]
#

Explain “Node pair voltage Method” using suitable diagram.

Answer:

Diagram:

graph TD
    A((Node 1)) -- I1 --> B((Node 2))
    A -- I2 --> C((Node 3))
    B -- I3 --> C
    B -- I4 --> D((Reference))
    C -- I5 --> D
    A -- I6 --> D

StepDescription
1Select a reference node (ground)
2Assign node voltages (V₁, V₂, etc.) to remaining nodes
3Apply KCL at each node (except reference)
4Express currents in terms of node voltages using Ohm’s Law
5Solve the simultaneous equations
  • Advantage: Fewer equations than mesh method for circuits with many meshes
  • Application: Efficient for non-planar circuits
  • Key equation: ΣG·V(own) - ΣG·V(adjacent) = ΣI

Mnemonic: “GRAND” - Ground node fixed, Remaining nodes numbered, Apply KCL, Note voltage differences, Derive solutions

Question 2(a) [3 marks]
#

Explain KCL with example.

Answer:

Diagram:

I2II14I3

Kirchhoff’s Current Law (KCL): The algebraic sum of all currents entering and leaving a node is zero.

Mathematical FormExample Application
ΣI = 0At node: I₁ - I₂ - I₃ + I₄ = 0
ΣIin = ΣIoutCurrents entering = Currents leaving

Mnemonic: “ZINC” - Zero Is Net Current at a node

Question 2(b) [4 marks]
#

Explain Z-parameter, Y-parameter, h-parameter and ABCD-parameter using suitable network.

Answer:

Diagram:

VI11P2ORTVI22
ParameterDefinitionEquationsUsage
ZImpedance parametersV₁ = Z₁₁I₁ + Z₁₂I₂, V₂ = Z₂₁I₁ + Z₂₂I₂High impedance circuits
YAdmittance parametersI₁ = Y₁₁V₁ + Y₁₂V₂, I₂ = Y₂₁V₁ + Y₂₂V₂Low impedance circuits
hHybrid parametersV₁ = h₁₁I₁ + h₁₂V₂, I₂ = h₂₁I₁ + h₂₂V₂Transistor circuits
ABCDTransmission parametersV₁ = AV₂ - BI₂, I₁ = CV₂ - DI₂Cascaded networks

Mnemonic: “ZANY HAB” - Z for high impedance, A for low, hy-brid for transistors, ABCD for Cascades

Question 2(c) [7 marks]
#

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

Answer:

Diagram:

graph TD
    subgraph T-Network
    A1((1)) -- Z1 --> O1((O))
    B1((2)) -- Z2 --> O1
    C1((3)) -- Z3 --> O1
    end

    subgraph π-Network
    A2((1)) -- Y1 --> B2((2))
    B2 -- Y2 --> C2((3))
    C2 -- Y3 --> A2
    end

ConversionFormulas
π to TZ₁ = (Z₁₂·Z₃₁)/(Z₁₂+Z₂₃+Z₃₁)
Z₂ = (Z₁₂·Z₂₃)/(Z₁₂+Z₂₃+Z₃₁)
Z₃ = (Z₂₃·Z₃₁)/(Z₁₂+Z₂₃+Z₃₁)
T to πZ₁₂ = (Z₁·Z₂+Z₂·Z₃+Z₃·Z₁)/Z₃
Z₂₃ = (Z₁·Z₂+Z₂·Z₃+Z₃·Z₁)/Z₁
Z₃₁ = (Z₁·Z₂+Z₂·Z₃+Z₃·Z₁)/Z₂
  • Application: Network simplification and analysis
  • Condition: Both networks must be equivalent at terminals
  • Limitation: Only applies for linear networks

Mnemonic: “TRIP” - T and π networks Relate Impedances through Products and sums

Question 2(a OR) [3 marks]
#

Explain KVL with example.

Answer:

Diagram:

V1--RR13----+R+2

Kirchhoff’s Voltage Law (KVL): The algebraic sum of all voltages around any closed loop is zero.

Mathematical FormExample Application
ΣV = 0In loop: V₁ - IR₁ - IR₂ - IR₃ = 0
ΣVrises = ΣVdropsVoltage rises = Voltage drops

Mnemonic: “ZERO” - Zero is Every voltage Round a loop’s Output

Question 2(b OR) [4 marks]
#

Classify and explain various Electronics network.

Answer:

Network TypeDescriptionExample
Linear vs Non-linearFollows/doesn’t follow proportionality principleResistors vs Diodes
Passive vs ActiveDon’t/do supply energyRC circuit vs Amplifier
Bilateral vs UnilateralSame/different properties in either directionResistors vs Diodes
Lumped vs DistributedParameters concentrated/spreadRC circuit vs Transmission line
Time variant vs InvariantParameters change/don’t change with timeElectronic switch vs Fixed resistor

Diagram:

graph TB
    A[Electronic Networks]
    A --> B[Based on Linearity]
    A --> C[Based on Energy]
    A --> D[Based on Directionality]
    A --> E[Based on Parameters]
    A --> F[Based on Time]

    B --> G[Linear]
    B --> H[Non-linear]
    C --> I[Active]
    C --> J[Passive]
    D --> K[Bilateral]
    D --> L[Unilateral]
    E --> M[Lumped]
    E --> N[Distributed]
    F --> O[Time-invariant]
    F --> P[Time-variant]

Mnemonic: “PLANT” - Proportionality for Linear, Lively for Active, All directions for bilateral, Near for lumped, Time-fixed for invariant

Question 2(c OR) [7 marks]
#

Derive the equation of characteristic impedance for T-network and π-network.

Answer:

Diagram:

graph LR
    subgraph T-Network
    A1((1)) -- Z1 --> O1((O))
    O1 -- Z3 --> C1((2))
    O1 -- Z2 --> B1
    end

    subgraph π-Network
    A2((1)) -- Y1 --> B2
    B2 -- Y2 --> C2((2))
    C2 -- Y3 --> A2
    end

NetworkCharacteristic Impedance EquationDerivation Steps
T-NetworkZ₀T = √[(Z₁+Z₂)(Z₂+Z₃)]1. Apply symmetrical load Z₀
2. Find input impedance
3. For impedance matching, Zin = Z₀
4. Solve for Z₀
π-NetworkZ₀π = 1/√[(Y₁+Y₃)(Y₂+Y₃)]1. Apply symmetrical load Z₀
2. Find input impedance
3. For impedance matching, Zin = Z₀
4. Solve for Z₀
  • Relation: Z₀T × Z₀π = Z₁·Z₃
  • Application: Impedance matching and filters
  • Limitation: Valid only for symmetrical networks

Mnemonic: “TIPSZ” - T-networks and π-networks Impedances are Products and Square roots of Z values

Question 3(a) [3 marks]
#

Explain the principle of duality with example.

Answer:

Diagram:

OriVg1ina--lRR13C--i--r-R-c2uit=>DuIa1lC--iGGr13c--u--i-G-t2

Principle of Duality: For every electrical network, there exists a dual network where:

OriginalDualExample
Voltage (V)Current (I)10V source → 10A source
Current (I)Voltage (V)5A → 5V
Resistance (R)Conductance (G)100Ω → 100S
Series connectionParallel connectionSeries resistors → Parallel conductors
KVLKCLΣV = 0 → ΣI = 0

Mnemonic: “VIGOR” - Voltage to current, Impedance to admittance, Graph remains, Open to closed, Resistors to conductors

Question 3(b) [4 marks]
#

Explain the steps to calculate the load current in the circuit using Thevenin’s Theorem.

Answer:

Diagram:

flowchart LR
    A[Original Circuit] --> B[Remove Load]
    B --> C[Find Voc]
    B --> D[Find Rth]
    C --> E[Thevenin Equivalent]
    D --> E
    E --> F[Reconnect Load]
    F --> G[Calculate IL = Vth/Rth+RL]

    style E fill:#bbf,stroke:#333

StepDescription
1Remove the load resistor from the circuit
2Find open-circuit voltage (Vth) across load terminals
3Calculate Thevenin resistance (Rth) looking back into circuit
4Draw Thevenin equivalent circuit (Vth in series with Rth)
5Reconnect load resistor (RL) to Thevenin circuit
6Calculate load current: IL = Vth/(Rth+RL)

Mnemonic: “REVOLT” - Remove load, Evaluate Voc, Obtain Rth, Look at Thevenin circuit, Use I = V/R formula

Question 3(c) [7 marks]
#

Find the current through load resistor using superposition theorem.

Answer:

Diagram:

12V4ΩIL6Ω10Ω12A

Table: Step-by-Step Solution:

StepDescriptionCalculation
1Consider 12V source only (replace 12A with open)I₁ = 12/(4+6+10) = 0.6A
I₁ through 6Ω = 0.6A
2Consider 12A source only (replace 12V with short)I₂ = -12×10/(4+10+6) = -6A
I₂ through 6Ω = -12×4/(4+10+6) = -2.4A
3Apply superpositionIL = I₁ + I₂ = 0.6 + (-2.4) = -1.8A

Answer: IL = -1.8A (current flowing upward through 6Ω load resistor)

Mnemonic: “SONAR” - Sources Only one at a time, Neutralize others, Add Results

Question 3(a OR) [3 marks]
#

Write Maximum Power Transfer Theorem statement. What are the conditions for maximum power transfer for AC and DC networks?

Answer:

Maximum Power Transfer Theorem: Maximum power is transferred from source to load when the load impedance is equal to the complex conjugate of the source internal impedance.

Network TypeCondition for Maximum Power Transfer
DC NetworksRL = Rth (Load resistance equals Thevenin resistance)
AC NetworksZL = Zth* (Load impedance equals complex conjugate of Thevenin impedance)
RL = Rth and XL = -Xth

Diagram:

VVttRhDRhtCtAhhC/N/\e\N/t/e\w\t/o/w\rX\oRktRrLhLkXXXL

Mnemonic: “MATCH” - Maximum power At Terminals when Conjugate impedances are Honored

Question 3(b OR) [4 marks]
#

Explain the steps to calculate the load current in the circuit using Norton’s Theorem.

Answer:

Diagram:

flowchart LR
    A[Original Circuit] --> B[Short Load Terminals]
    B --> C[Find Isc]
    B --> D[Find Rn=Rth]
    C --> E[Norton Equivalent]
    D --> E
    E --> F[Reconnect Load]
    F --> G[Calculate IL = In×Rn/Rn+RL]

    style E fill:#bbf,stroke:#333

StepDescription
1Remove the load resistor from the circuit
2Find short-circuit current (In) across load terminals
3Calculate Norton resistance (Rn) looking back into circuit
4Draw Norton equivalent circuit (In in parallel with Rn)
5Reconnect load resistor (RL) to Norton circuit
6Calculate load current: IL = In×Rn/(Rn+RL)

Mnemonic: “SENIOR” - Short terminals, Evaluate Isc, Notice Rn value, Implement Norton circuit, Obtain result

Question 3(c OR) [7 marks]
#

Demonstrate how the reciprocity theorem is applied to a given network.

Answer:

Diagram:

10V2Ω4Ω2Ω2Ω

Table: Applying Reciprocity Theorem:

StepCircuit 1Circuit 2Verification
110V source at left, Find I₁ at right10V source at right, Find I₂ at leftI₁ = I₂ confirms reciprocity
2Create mesh equations using KVLCreate new mesh equations for swapped sourceSolve both systems
3I₁ = 10×2/(2×4 + 2×2 + 4×2) = 0.625AI₂ = 10×2/(2×4 + 2×2 + 4×2) = 0.625AI₁ = I₂ = 0.625A ✓

Principle: In a passive network containing only bilateral elements, if voltage source E in branch 1 produces current I in branch 2, then the same voltage source E placed in branch 2 will produce the same current I in branch 1.

Mnemonic: “RESPECT” - Rewire sources, Exchange positions, See if currents Preserve Equality when Circuit Transformed

Question 4(a) [3 marks]
#

Explain coupled circuit.

Answer:

Diagram:

V1LP1rOiOmOMaOryLS2eOcOoOnOdRaLry

Coupled Circuit: A circuit where energy is transferred between inductors through mutual inductance.

ParameterDescription
Mutual Inductance (M)Measure of magnetic coupling between coils
Coupling Coefficient (k)k = M/√(L₁L₂), ranges from 0 (no coupling) to 1 (perfect coupling)
ApplicationsTransformers, filters, tuned circuits

Mnemonic: “MICE” - Mutual Inductance Creates Energy transfer

Question 4(b) [4 marks]
#

Derive the equation of co-efficient of coupling for coupled circuit.

Answer:

Diagram:

graph LR
    A[Magnetic Flux Linkage] --> B[Mutual Inductance]
    B --> C[Coupling Coefficient]

    subgraph Formula Derivation
    D["φ12 = Flux from coil 1 to 2"]
    E["M = N2·φ12/I1"]
    F["k = M/√(L1·L2)"]
    end

StepDescriptionEquation
1Define mutual inductanceM = N₂·φ₁₂/I₁
2Define self-inductancesL₁ = N₁·φ₁₁/I₁, L₂ = N₂·φ₂₂/I₂
3Maximum possible MMmax = √(L₁·L₂)
4Define coupling coefficientk = M/√(L₁·L₂)
  • Range: 0 ≤ k ≤ 1
  • Physical meaning: Fraction of flux from one coil linking with the other coil
  • Perfect coupling: k = 1, when all flux links both coils

Mnemonic: “MASK” - Mutual inductance And Self inductances create K

Question 4(c) [7 marks]
#

Derive equation of resonance frequency for series resonance. Calculate resonant frequency, Q factor and bandwidth of series RLC circuit with R=20Ω, L=1H, C=1μF.

Answer:

Diagram:

VR/\/\/\LOO|CO|O

Derivation:

StepDescriptionEquation
1Impedance of series RLCZ = R + j(ωL - 1/ωC)
2At resonance, Im(Z) = 0ωL - 1/ωC = 0
3Solve for resonant frequencyω₀ = 1/√(LC) or f₀ = 1/(2π√(LC))

Calculations:

ParameterFormulaCalculationResult
Resonant frequencyf₀ = 1/(2π√(LC))f₀ = 1/(2π√(1×10⁻⁶))159.15 Hz
Q factorQ = ω₀L/RQ = 2π×159.15×1/2050
BandwidthBW = f₀/QBW = 159.15/503.18 Hz

Mnemonic: “FQBR” - Frequency from reactances, Q from resistance ratio, Bandwidth from Resonance divided by Q

Question 4(a OR) [3 marks]
#

Explain Quality factor.

Answer:

Diagram:

graph LR
    A[Quality Factor] --> B[Energy Storage]
    A --> C[Power Loss]
    A --> D[Selectivity]
    A --> E[Bandwidth]

    style A fill:#bbf,stroke:#333

Quality Factor (Q): A dimensionless parameter that indicates how under-damped a resonator is, or alternatively, characterizes a resonator’s bandwidth relative to its center frequency.

DefinitionMathematical Expression
Energy perspectiveQ = 2π × Energy stored / Energy dissipated per cycle
Circuit perspectiveQ = X/R (where X is reactance, R is resistance)
Frequency perspectiveQ = f₀/BW (where f₀ is resonant frequency, BW is bandwidth)

Mnemonic: “QSEL” - Quality shows Energy vs. Loss and Selectivity

Question 4(b OR) [4 marks]
#

Derive the equation of quality factor for a capacitor.

Answer:

Diagram:

IRdeeaallcCapaciEtSRoRrmodel

Derivation:

StepDescriptionEquation
1Define energy storedEstored = CV²/2
2Define energy loss per cycleEloss = πCV²/ωCR = πV²/ωR
3Define Q factorQ = 2π × Estored / Eloss
4Substitute and simplifyQ = 2π × (CV²/2) ÷ (πV²/ωR) = ωCR

Final equation: Q = ωCR = 1/(ωRC) = 1/tanδ

Where:

  • ω = Angular frequency (2πf)
  • R = Equivalent series resistance (ESR)
  • C = Capacitance
  • tanδ = Dissipation factor

Mnemonic: “CORE” - Capacitors’ Quality equals One over Resistance times Capacitance

Question 4(c OR) [7 marks]
#

Derive equation of resonance frequency for parallel resonance. Calculate resonant frequency, Q factor and bandwidth of parallel RLC circuit with R=30Ω, L=1H, C=1μF.

Answer:

Diagram:

VROOLOOC

Derivation:

StepDescriptionEquation
1Admittance of parallel RLCY = 1/R + 1/jωL + jωC
2At resonance, Im(Y) = 01/jωL + jωC = 0
3Solve for resonant frequencyω₀ = 1/√(LC) or f₀ = 1/(2π√(LC))

Calculations:

ParameterFormulaCalculationResult
Resonant frequencyf₀ = 1/(2π√(LC))f₀ = 1/(2π√(1×10⁻⁶))159.15 Hz
Q factorQ = R/ω₀LQ = 30/(2π×159.15×1)0.03
BandwidthBW = f₀/QBW = 159.15/0.035305 Hz

Mnemonic: “FPQB” - Frequency from Parallel elements, Q from Resistance divided by reactance, Bandwidth from division

Question 5(a) [3 marks]
#

Explain the T type attenuator.

Answer:

Diagram:

InZ1//\\//Z\Z\2/3/\\/Out

T-type Attenuator: A passive network in T configuration used to reduce signal amplitude.

ComponentDescriptionFormula
Z1, Z2Series armsZ1 = Z2 = Z₀(N-1)/(N+1)
Z3Shunt armZ3 = 2Z₀/(N²-1)
NAttenuation ratioN = 10^(dB/20)
  • Characteristic: Symmetrical for matched source and load
  • Applications: Signal level control, impedance matching
  • Advantage: Maintains impedance matching with proper design

Mnemonic: “TSAR” - T-shape with Series Arms and Resistance in middle

Question 5(b) [4 marks]
#

Classify the various passive filter circuits.

Answer:

Diagram:

graph TD
    A[Passive Filters]
    A --> B[Based on Frequency Response]
    A --> C[Based on Configuration]

    B --> D[Low Pass]
    B --> E[High Pass]
    B --> F[Band Pass]
    B --> G[Band Stop]
    
    C --> H[T-section]
    C --> I[π-section]
    C --> J[L-section]
    C --> K[Lattice]

Filter TypeFunctionTypical CircuitApplications
Low PassPasses low frequenciesRC, RL circuitsAudio filters, Power supplies
High PassPasses high frequenciesCR, LR circuitsNoise filtering, Signal conditioning
Band PassPasses a band of frequenciesRLC circuitsRadio tuning, Signal selection
Band StopBlocks a band of frequenciesParallel RLCInterference rejection

Mnemonic: “LHBB” - Low High Band Band filters for Pass and Block

Question 5(c) [7 marks]
#

Design constant-k type low pass and High pass filter with T-section having cutoff frequency= 1000Hz & load of 500Ω.

Answer:

Diagram:

LowP-aLOs/Os2OOT---F-Ci-l-t-eLOr/O2OO--HighPCa/s2sOTLO-OFOiltCe/r2

Design Calculations:

For Constant-k T-type low pass filter:

ParameterFormulaCalculationValue
Cut-off frequencyfc = 1000 HzGiven1000 Hz
Load impedanceR₀ = 500 ΩGiven500 Ω
Series inductorL = R₀/πfcL = 500/(π×1000)159.15 mH
Half sectionsL/2159.15/279.58 mH
Shunt capacitorC = 1/(πfcR₀)C = 1/(π×1000×500)0.636 μF

For Constant-k T-type high pass filter:

ParameterFormulaCalculationValue
Series capacitorC = 1/(4πfcR₀)C = 1/(4π×1000×500)0.159 μF
Half sectionsC/20.159/20.0795 μF
Shunt inductorL = R₀/(4πfc)L = 500/(4π×1000)39.79 mH

Mnemonic: “FRED” - Frequency Ratio determines Element Dimensions

Question 5(a OR) [3 marks]
#

Explain the π type attenuator.

Answer:

Diagram:

InZ1Z2Z3Out

π-type Attenuator: A passive network in π configuration used to reduce signal amplitude.

ComponentDescriptionFormula
Z2Series armZ2 = 2Z₀/(N²-1)
Z1, Z3Shunt armsZ1 = Z3 = Z₀(N+1)/(N-1)
NAttenuation ratioN = 10^(dB/20)
  • Characteristic: Symmetrical for matched source and load
  • Applications: Signal level control, impedance matching
  • Advantage: Good isolation between input and output

Mnemonic: “PASS” - Pi-Attenuator has Series in middle and Shunt arms outside

Question 5(b OR) [4 marks]
#

Classify various types of attenuators.

Answer:

Diagram:

graph TD
    A[Attenuators]
    A --> B[Based on Structure]
    A --> C[Based on Function]

    B --> D[T-type]
    B --> E[π-type]
    B --> F[L-type]
    B --> G[Bridged-T]
    B --> H[Lattice]
    
    C --> I[Fixed]
    C --> J[Variable]
    C --> K[Stepped]
    C --> L[Programmable]

Attenuator TypeCharacteristicsApplicationsAdvantages
T-typeSeries-Shunt-SeriesAudio systemsSimple design
π-typeShunt-Series-ShuntRF circuitsBetter isolation
L-typeSeries-ShuntSimple matchingImpedance transformation
Bridged-TBalanced structureTest equipmentMinimal distortion
BalancedSymmetric dual pathsDifferential signalsCommon mode rejection

Mnemonic: “TPLBV” - T, Pi, L, Bridged-T, and Variable attenuators

Question 5(c OR) [7 marks]
#

Design a symmetrical T type attenuator and π type attenuator to give attenuation of 40dB and to work into the load of 500Ω.

Answer:

Diagram:

T-typeR1AttenRu2atRo1rπ-typRe1AttRe2nuRa1tor

Design Calculations:

StepFormulaCalculationValue
GivenAttenuation = 40 dB-40 dB
Step 1N = 10^(dB/20)10^(40/20)100
Step 2K = (N-1)/(N+1)(100-1)/(100+1)0.98

For T-type attenuator:

ComponentFormulaCalculationValue
R₁ (series)Z₀·K500 × 0.98490 Ω
R₂ (shunt)Z₀/(K·(N-K))500/(0.98×(100-0.98))5.15 Ω

For π-type attenuator:

ComponentFormulaCalculationValue
R₁ (shunt)Z₀/K500/0.98510.2 Ω
R₂ (series)Z₀·K·(N-K)500 × 0.98 × (100-0.98)48,541 Ω

Mnemonic: “DANK” - dB Attenuation is Number K, which determines resistor values

Related

Electronic Circuits & Networks (4331101) - Summer 2023 Solution
17 mins
Study-Material Solutions Electronic-Circuits Networks 4331101 2023 Summer
Electronic Circuits & Networks (4331101) - Winter 2024 Solution
18 mins
Study-Material Solutions Electronic-Circuits 4331101 2024 Winter
Electronic Circuits & Networks (4331101) - Winter 2022 Solution
18 mins
Study-Material Solutions Electronic-Circuits Networks 4331101 2022 Winter
Electronic Circuits & Networks (4331101) - Winter 2023 Solution
15 mins
Study-Material Solutions Electronic-Circuits Networks 4331101 2023 Winter
Communication Engineering (1333201) - Summer 2024 Solution
16 mins
Study-Material Solutions Communication-Engineering 1333201 2024 Summer
Microwave and Radar Communication (4351103) - Summer 2024 Solution
19 mins
Study-Material Solutions Microwave Radar 4351103 2024 Summer