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
Parameter | Formula | Explanation |
---|---|---|
Total Capacitance | 1/CT = 1/C₁ + 1/C₂ | Reciprocal sum |
Voltage Distribution | V₁/V₂ = C₂/C₁ | Inverse to capacitance ratio |
Current | I = I₁ = I₂ | Same current flows through all |
Charge | Q = Q₁ = Q₂ | Same charge on each capacitor |
Power | P = VI = V²/Xc | Where 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
Parameter | Series Connection | Parallel Connection |
---|---|---|
Total Resistance | Increases (RT = R₁ + R₂ + …) | Decreases (RT < smallest R) |
Current | Same through all (I) | Divides (IT = I₁ + I₂ + …) |
Voltage | Divides (VT = V₁ + V₂ + …) | Same across all (V) |
Power | PT = 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
Term | Definition | Example |
---|---|---|
Unilateral Network | Allows current in one direction only | Diode circuit |
Bilateral Network | Allows current in both directions | RLC circuit |
Mesh | Planar network path with no other path inside it | Single closed path |
Loop | Any closed path in a network | Can 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
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
Parameter | Definition | Calculation |
---|---|---|
Z₁₁ | Input impedance with output open | Z₁₁ = V₁/I₁ (when I₂=0) |
Z₁₂ | Transfer impedance from port 2 to port 1 | Z₁₂ = V₁/I₂ (when I₁=0) |
Z₂₁ | Transfer impedance from port 1 to port 2 | Z₂₁ = V₂/I₁ (when I₂=0) |
Z₂₂ | Output impedance with input open | Z₂₂ = 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
Derivation:
- For symmetrical T-network, Z₁ is split equally across two arms (Z₁/2 each)
- 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
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
Parameter | Definition | Calculation |
---|---|---|
Y₁₁ | Input admittance with output shorted | Y₁₁ = I₁/V₁ (when V₂=0) |
Y₁₂ | Transfer admittance from port 2 to port 1 | Y₁₂ = I₁/V₂ (when V₁=0) |
Y₂₁ | Transfer admittance from port 1 to port 2 | Y₂₁ = I₂/V₁ (when V₂=0) |
Y₂₂ | Output admittance with input shorted | Y₂₂ = 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
Derivation:
- For symmetrical π-network, admittance Y₁ in shunt arms is split into 2 equal parts (Y₃ = Y₁/2)
- 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 Circuit | Dual Circuit |
---|---|
Voltage (V) | Current (I) |
Current (I) | Voltage (V) |
Resistance (R) | Conductance (G) |
Inductance (L) | Capacitance (C) |
Series Connection | Parallel Connection |
KVL | KCL |
Mesh Analysis | Nodal 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:
- Remove the load resistance
- Calculate open-circuit voltage (Vth)
- 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
Law | Statement | Mathematical Form | Application |
---|---|---|---|
KCL | Sum of currents entering a node equals sum of currents leaving it | ∑Iin = ∑Iout | Node Analysis |
KVL | Sum of voltage drops around any closed loop equals zero | ∑V = 0 | Mesh Analysis |
KCL Example:
KVL Example:
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
Steps:
- Identify meshes (closed loops)
- Assign clockwise mesh currents (I₁, I₂)
- Apply KVL to each mesh
- 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:
- Remove the load resistance
- Calculate short-circuit current (IN)
- 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:
Power delivered to load: P = I²RL
Current through circuit: I = Vth/(Rth + RL)
Substituting: P = Vth²RL/(Rth + RL)²
Differentiating with respect to RL and setting to zero: dP/dRL = 0
This gives: RL = Rth
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
Derivation:
- For an inductor with resistance, impedance Z = R + jωL
- Q factor is defined as: Q = Reactive Power / Active Power
- 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
Derivation:
- Admittance of parallel RLC: Y = 1/R + jωC + 1/jωL = 1/R + j(ωC - 1/ωL)
- At resonance, imaginary part is zero: ωC - 1/ωL = 0
- Solving for ω: ω² = 1/LC
- Therefore: ω = 1/√(LC)
- 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
Type | Coupling Medium | Application |
---|---|---|
Direct Coupling | Conductively connected | DC amplifiers |
Capacitive Coupling | Capacitor | AC signal coupling |
Inductive Coupling | Magnetic field | Transformers |
Resistive Coupling | Resistor | Low-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
Derivation:
- For a capacitor with series resistance, impedance Z = R - j/(ωC)
- Q factor is defined as: Q = Reactive Power / Active Power
- 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
Derivation:
- Impedance of series RLC: Z = R + jωL - j/(ωC) = R + j(ωL - 1/ωC)
- At resonance, imaginary part is zero: ωL - 1/ωC = 0
- Solving for ω: ω² = 1/LC
- Therefore: ω = 1/√(LC)
- 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
Derivation:
- Mutual inductance (M) relates to individual inductances by: M = k√(L₁L₂)
- 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 k | Coupling Type | Application |
---|---|---|
k = 0 | No coupling | Separate circuits |
0 < k < 0.5 | Loose coupling | RF transformers |
0.5 < k < 1 | Tight coupling | Power transformers |
k = 1 | Perfect coupling | Ideal 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
Unit | Definition | Formula | Usage |
---|---|---|---|
Neper (Np) | Natural logarithmic ratio | N = ln(V₁/V₂) or ln(I₁/I₂) | Power system analysis |
Decibel (dB) | Common logarithmic ratio | dB = 20log₁₀(V₁/V₂) or 10log₁₀(P₁/P₂) | Signal level measurement |
Relationship:
- N = ln(V₁/V₂)
- dB = 20log₁₀(V₁/V₂)
- Since ln(x) = 2.303 × log₁₀(x)
- Therefore: N = 2.303 × dB/20 = 0.1152 × dB
- 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
Type | Structure | Characteristics | Applications |
---|---|---|---|
T-type | Three resistors in T formation | Fixed impedance, good balance | Signal level control |
π-type (Pi) | Three resistors in π formation | Better isolation, more common | RF signal attenuation |
L-type | Two resistors in L formation | Simple, unbalanced | Basic level adjustment |
Bridged T | T with bridging resistor | Constant impedance | Audio applications |
Balanced | Symmetrical design | Good CMRR | Balanced transmission |
Lattice | Diamond-shaped | Balanced, symmetrical | Telephone 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
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
Limitation | Description | Effect |
---|---|---|
Impedance Matching | Impedance varies with frequency | Signal reflection, power loss |
Attenuation Band | Gradual transition at cut-off | Poor frequency selectivity |
Phase Response | Non-linear phase characteristic | Signal distortion |
Passband Ripple | Non-uniform response in passband | Signal amplitude variation |
Roll-off Rate | Slow 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
Derivation:
- For high-pass filter, series elements are capacitors and shunt elements are inductors
- Transfer function: H(jω) = Z₂/(Z₁ + Z₂)
- Where Z₁ = 1/(jωC) and Z₂ = jωL
- Impedance condition for cut-off: Z₁/Z₂ = 4 or Z₁/4Z₂ = 1
- Substituting: 1/(jωC) = 4jωL
- Solving for ω: ω² = 1/(4LC)
- 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 Type | Passes | Blocks | Applications |
---|---|---|---|
Low-Pass | Frequencies below fc | Frequencies above fc | Audio amplifiers, power supplies |
High-Pass | Frequencies above fc | Frequencies below fc | Noise elimination, treble control |
Band-Pass | Range between fL and fH | Frequencies outside range | Radio tuning, equalizers |
Band-Stop | Frequencies outside range | Range between fL and fH | Noise elimination, notch filters |
All-Pass | All frequencies with unity gain | None (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”