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
Feature | Graph | Tree |
---|---|---|
Definition | Complete topological representation of network | Connected subgraph containing all nodes but no loops |
Elements | Contains all branches and nodes | Contains N-1 branches where N is number of nodes |
Loops | Contains loops | No loops |
Application | Used for complete circuit analysis | Used 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
Step | Description |
---|---|
1 | Identify independent meshes in the circuit |
2 | Assign mesh currents (I₁, I₂, etc.) in clockwise direction |
3 | Apply KVL to each mesh |
4 | Form equations using: ΣR·I(own) - ΣR·I(adjacent) = ΣV |
5 | Solve 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
Step | Description |
---|---|
1 | Select a reference node (ground) |
2 | Assign node voltages (V₁, V₂, etc.) to remaining nodes |
3 | Apply KCL at each node (except reference) |
4 | Express currents in terms of node voltages using Ohm’s Law |
5 | Solve 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:
Kirchhoff’s Current Law (KCL): The algebraic sum of all currents entering and leaving a node is zero.
Mathematical Form | Example Application |
---|---|
ΣI = 0 | At node: I₁ - I₂ - I₃ + I₄ = 0 |
ΣIin = ΣIout | Currents 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:
Parameter | Definition | Equations | Usage |
---|---|---|---|
Z | Impedance parameters | V₁ = Z₁₁I₁ + Z₁₂I₂, V₂ = Z₂₁I₁ + Z₂₂I₂ | High impedance circuits |
Y | Admittance parameters | I₁ = Y₁₁V₁ + Y₁₂V₂, I₂ = Y₂₁V₁ + Y₂₂V₂ | Low impedance circuits |
h | Hybrid parameters | V₁ = h₁₁I₁ + h₁₂V₂, I₂ = h₂₁I₁ + h₂₂V₂ | Transistor circuits |
ABCD | Transmission parameters | V₁ = AV₂ - BI₂, I₁ = CV₂ - DI₂ | Cascaded 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
Conversion | Formulas |
---|---|
π to T | Z₁ = (Z₁₂·Z₃₁)/(Z₁₂+Z₂₃+Z₃₁) Z₂ = (Z₁₂·Z₂₃)/(Z₁₂+Z₂₃+Z₃₁) Z₃ = (Z₂₃·Z₃₁)/(Z₁₂+Z₂₃+Z₃₁) |
T to π | Z₁₂ = (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:
Kirchhoff’s Voltage Law (KVL): The algebraic sum of all voltages around any closed loop is zero.
Mathematical Form | Example Application |
---|---|
ΣV = 0 | In loop: V₁ - IR₁ - IR₂ - IR₃ = 0 |
ΣVrises = ΣVdrops | Voltage 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 Type | Description | Example |
---|---|---|
Linear vs Non-linear | Follows/doesn’t follow proportionality principle | Resistors vs Diodes |
Passive vs Active | Don’t/do supply energy | RC circuit vs Amplifier |
Bilateral vs Unilateral | Same/different properties in either direction | Resistors vs Diodes |
Lumped vs Distributed | Parameters concentrated/spread | RC circuit vs Transmission line |
Time variant vs Invariant | Parameters change/don’t change with time | Electronic 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
Network | Characteristic Impedance Equation | Derivation Steps |
---|---|---|
T-Network | Z₀T = √[(Z₁+Z₂)(Z₂+Z₃)] | 1. Apply symmetrical load Z₀ 2. Find input impedance 3. For impedance matching, Zin = Z₀ 4. Solve for Z₀ |
π-Network | Z₀π = 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:
Principle of Duality: For every electrical network, there exists a dual network where:
Original | Dual | Example |
---|---|---|
Voltage (V) | Current (I) | 10V source → 10A source |
Current (I) | Voltage (V) | 5A → 5V |
Resistance (R) | Conductance (G) | 100Ω → 100S |
Series connection | Parallel connection | Series resistors → Parallel conductors |
KVL | KCL | ΣV = 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
Step | Description |
---|---|
1 | Remove the load resistor from the circuit |
2 | Find open-circuit voltage (Vth) across load terminals |
3 | Calculate Thevenin resistance (Rth) looking back into circuit |
4 | Draw Thevenin equivalent circuit (Vth in series with Rth) |
5 | Reconnect load resistor (RL) to Thevenin circuit |
6 | Calculate 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:
Table: Step-by-Step Solution:
Step | Description | Calculation |
---|---|---|
1 | Consider 12V source only (replace 12A with open) | I₁ = 12/(4+6+10) = 0.6A I₁ through 6Ω = 0.6A |
2 | Consider 12A source only (replace 12V with short) | I₂ = -12×10/(4+10+6) = -6A I₂ through 6Ω = -12×4/(4+10+6) = -2.4A |
3 | Apply superposition | IL = 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 Type | Condition for Maximum Power Transfer |
---|---|
DC Networks | RL = Rth (Load resistance equals Thevenin resistance) |
AC Networks | ZL = Zth* (Load impedance equals complex conjugate of Thevenin impedance) RL = Rth and XL = -Xth |
Diagram:
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
Step | Description |
---|---|
1 | Remove the load resistor from the circuit |
2 | Find short-circuit current (In) across load terminals |
3 | Calculate Norton resistance (Rn) looking back into circuit |
4 | Draw Norton equivalent circuit (In in parallel with Rn) |
5 | Reconnect load resistor (RL) to Norton circuit |
6 | Calculate 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:
Table: Applying Reciprocity Theorem:
Step | Circuit 1 | Circuit 2 | Verification |
---|---|---|---|
1 | 10V source at left, Find I₁ at right | 10V source at right, Find I₂ at left | I₁ = I₂ confirms reciprocity |
2 | Create mesh equations using KVL | Create new mesh equations for swapped source | Solve both systems |
3 | I₁ = 10×2/(2×4 + 2×2 + 4×2) = 0.625A | I₂ = 10×2/(2×4 + 2×2 + 4×2) = 0.625A | I₁ = 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:
Coupled Circuit: A circuit where energy is transferred between inductors through mutual inductance.
Parameter | Description |
---|---|
Mutual Inductance (M) | Measure of magnetic coupling between coils |
Coupling Coefficient (k) | k = M/√(L₁L₂), ranges from 0 (no coupling) to 1 (perfect coupling) |
Applications | Transformers, 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
Step | Description | Equation |
---|---|---|
1 | Define mutual inductance | M = N₂·φ₁₂/I₁ |
2 | Define self-inductances | L₁ = N₁·φ₁₁/I₁, L₂ = N₂·φ₂₂/I₂ |
3 | Maximum possible M | Mmax = √(L₁·L₂) |
4 | Define coupling coefficient | k = 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:
Derivation:
Step | Description | Equation |
---|---|---|
1 | Impedance of series RLC | Z = R + j(ωL - 1/ωC) |
2 | At resonance, Im(Z) = 0 | ωL - 1/ωC = 0 |
3 | Solve for resonant frequency | ω₀ = 1/√(LC) or f₀ = 1/(2π√(LC)) |
Calculations:
Parameter | Formula | Calculation | Result |
---|---|---|---|
Resonant frequency | f₀ = 1/(2π√(LC)) | f₀ = 1/(2π√(1×10⁻⁶)) | 159.15 Hz |
Q factor | Q = ω₀L/R | Q = 2π×159.15×1/20 | 50 |
Bandwidth | BW = f₀/Q | BW = 159.15/50 | 3.18 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.
Definition | Mathematical Expression |
---|---|
Energy perspective | Q = 2π × Energy stored / Energy dissipated per cycle |
Circuit perspective | Q = X/R (where X is reactance, R is resistance) |
Frequency perspective | Q = 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:
Derivation:
Step | Description | Equation |
---|---|---|
1 | Define energy stored | Estored = CV²/2 |
2 | Define energy loss per cycle | Eloss = πCV²/ωCR = πV²/ωR |
3 | Define Q factor | Q = 2π × Estored / Eloss |
4 | Substitute and simplify | Q = 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:
Derivation:
Step | Description | Equation |
---|---|---|
1 | Admittance of parallel RLC | Y = 1/R + 1/jωL + jωC |
2 | At resonance, Im(Y) = 0 | 1/jωL + jωC = 0 |
3 | Solve for resonant frequency | ω₀ = 1/√(LC) or f₀ = 1/(2π√(LC)) |
Calculations:
Parameter | Formula | Calculation | Result |
---|---|---|---|
Resonant frequency | f₀ = 1/(2π√(LC)) | f₀ = 1/(2π√(1×10⁻⁶)) | 159.15 Hz |
Q factor | Q = R/ω₀L | Q = 30/(2π×159.15×1) | 0.03 |
Bandwidth | BW = f₀/Q | BW = 159.15/0.03 | 5305 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:
T-type Attenuator: A passive network in T configuration used to reduce signal amplitude.
Component | Description | Formula |
---|---|---|
Z1, Z2 | Series arms | Z1 = Z2 = Z₀(N-1)/(N+1) |
Z3 | Shunt arm | Z3 = 2Z₀/(N²-1) |
N | Attenuation ratio | N = 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 Type | Function | Typical Circuit | Applications |
---|---|---|---|
Low Pass | Passes low frequencies | RC, RL circuits | Audio filters, Power supplies |
High Pass | Passes high frequencies | CR, LR circuits | Noise filtering, Signal conditioning |
Band Pass | Passes a band of frequencies | RLC circuits | Radio tuning, Signal selection |
Band Stop | Blocks a band of frequencies | Parallel RLC | Interference 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:
Design Calculations:
For Constant-k T-type low pass filter:
Parameter | Formula | Calculation | Value |
---|---|---|---|
Cut-off frequency | fc = 1000 Hz | Given | 1000 Hz |
Load impedance | R₀ = 500 Ω | Given | 500 Ω |
Series inductor | L = R₀/πfc | L = 500/(π×1000) | 159.15 mH |
Half sections | L/2 | 159.15/2 | 79.58 mH |
Shunt capacitor | C = 1/(πfcR₀) | C = 1/(π×1000×500) | 0.636 μF |
For Constant-k T-type high pass filter:
Parameter | Formula | Calculation | Value |
---|---|---|---|
Series capacitor | C = 1/(4πfcR₀) | C = 1/(4π×1000×500) | 0.159 μF |
Half sections | C/2 | 0.159/2 | 0.0795 μF |
Shunt inductor | L = 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:
π-type Attenuator: A passive network in π configuration used to reduce signal amplitude.
Component | Description | Formula |
---|---|---|
Z2 | Series arm | Z2 = 2Z₀/(N²-1) |
Z1, Z3 | Shunt arms | Z1 = Z3 = Z₀(N+1)/(N-1) |
N | Attenuation ratio | N = 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 Type | Characteristics | Applications | Advantages |
---|---|---|---|
T-type | Series-Shunt-Series | Audio systems | Simple design |
π-type | Shunt-Series-Shunt | RF circuits | Better isolation |
L-type | Series-Shunt | Simple matching | Impedance transformation |
Bridged-T | Balanced structure | Test equipment | Minimal distortion |
Balanced | Symmetric dual paths | Differential signals | Common 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:
Design Calculations:
Step | Formula | Calculation | Value |
---|---|---|---|
Given | Attenuation = 40 dB | - | 40 dB |
Step 1 | N = 10^(dB/20) | 10^(40/20) | 100 |
Step 2 | K = (N-1)/(N+1) | (100-1)/(100+1) | 0.98 |
For T-type attenuator:
Component | Formula | Calculation | Value |
---|---|---|---|
R₁ (series) | Z₀·K | 500 × 0.98 | 490 Ω |
R₂ (shunt) | Z₀/(K·(N-K)) | 500/(0.98×(100-0.98)) | 5.15 Ω |
For π-type attenuator:
Component | Formula | Calculation | Value |
---|---|---|---|
R₁ (shunt) | Z₀/K | 500/0.98 | 510.2 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