Question 1(a) [3 marks]#
Define following terms. (i) Active elements (ii) Bilateral elements (iii) Linear elements
Answer:
Term | Definition |
---|---|
Active elements | Electronic components that can supply energy or power to a circuit (like batteries, generators, op-amps) |
Bilateral elements | Components that allow current flow equally in both directions with same characteristics (like resistors, capacitors, inductors) |
Linear elements | Components whose current-voltage relationship follows a straight line and obeys the principle of superposition (like resistors following Ohm’s law) |
Mnemonic: “ABL: Active powers Batteries, Bilateral flows Both ways, Linear stays Lawful”
Question 1(b) [4 marks]#
Capacitors of 10µF, 20µF and 30µF are connected in series and supply of 200V DC is given. Find voltage across each capacitor.
Answer:
For series-connected capacitors:
- Find equivalent capacitance: 1/Ceq = 1/C₁ + 1/C₂ + 1/C₃
- Voltage division: VC = (C₁/C) × V
Calculation: 1/Ceq = 1/10 + 1/20 + 1/30 = 0.1 + 0.05 + 0.033 = 0.183 Ceq = 5.46 μF
Capacitor | Formula | Calculation | Voltage |
---|---|---|---|
C₁ = 10μF | V₁ = (Ceq/C₁) × V | (5.46/10) × 200 = 109.2V | 109.2V |
C₂ = 20μF | V₂ = (Ceq/C₂) × V | (5.46/20) × 200 = 54.6V | 54.6V |
C₃ = 30μF | V₃ = (Ceq/C₃) × V | (5.46/30) × 200 = 36.4V | 36.4V |
Mnemonic: “Smaller Capacitors get Larger Voltages”
Question 1(c) [7 marks]#
Explain Node pair voltage method for graph theory.
Answer:
Node pair voltage method is a systematic approach to analyze electrical networks.
Procedure:
- Select a reference node (ground)
- Identify the node voltages (N-1 unknowns for N nodes)
- Apply KCL at each non-reference node
- Express branch currents in terms of node voltages
- Solve the equations for node voltages
Diagram:
graph TD
A[1. Select reference node] --> B[2. Identify node voltages]
B --> C[3. Apply KCL at each node]
C --> D[4. Express branch currents using node voltages]
D --> E[5. Solve equations for node voltages]
E --> F[6. Calculate branch currents]
Key advantages:
- Fewer equations: Only (n-1) equations for n nodes
- Computational efficiency: Reduces system complexity
- Direct voltage solutions: Provides node voltages directly
- Systematic approach: Works for any network topology
Mnemonic: “GARCS: Ground, Assign voltages, Relate with KCL, Calculate currents, Solve equations”
Question 1(c) OR [7 marks]#
Explain voltage division method with necessary equations.
Answer:
Voltage division is a method to calculate how voltage distributes across series components.
Principle: In a series circuit, voltage divides proportionally to component resistances/impedances.
Formula: For a resistor R₁ in a series circuit with total resistance RT: V₁ = (R₁/RT) × VS
Diagram:
Mathematical explanation:
- For resistors: V₁ = (R₁/RT) × VS
- For capacitors: V₁ = (1/C₁)/(1/CT) × VS = (CT/C₁) × VS
- For inductors: V₁ = (L₁/LT) × VS
- For complex impedances: V₁ = (Z₁/ZT) × VS
Examples:
- Voltage across a 1kΩ resistor in series with 4kΩ with 5V source = (1/5)×5V = 1V
- Voltage across a 10μF capacitor in series with 40μF with 10V source = (1/10)/(1/8)×10V = 8V
Mnemonic: “The BIGGER the RESISTANCE, the BIGGER the VOLTAGE drop”
Question 2(a) [3 marks]#
Write open circuit impedance parameters of Two port network.
Answer:
Open Circuit Impedance Parameters:
Parameter | Equation | Physical Meaning |
---|---|---|
Z₁₁ | Z₁₁ = V₁/I₁ (when I₂=0) | Input impedance with output open-circuited |
Z₁₂ | Z₁₂ = V₁/I₂ (when I₁=0) | Transfer impedance from port 2 to port 1 |
Z₂₁ | Z₂₁ = V₂/I₁ (when I₂=0) | Transfer impedance from port 1 to port 2 |
Z₂₂ | Z₂₂ = V₂/I₂ (when I₁=0) | Output impedance with input open-circuited |
Mnemonic: “ZIPO: Z-parameters with Inputs and outputs, Ports Open where needed”
Question 2(b) [4 marks]#
Derive conversion from T-type network to ∏-type network.
Answer:
T to ∏ Network Conversion:
Diagram:
Conversion Equations:
∏-Parameter | Formula | Based on T-Parameters |
---|---|---|
Y₁ = 1/Z₁ | Y₁ = Z₂/(Z₁Z₂+Z₂Z₃+Z₃Z₁) | Reciprocal of Z₁ modified by network |
Y₂ = 1/Z₂ | Y₂ = Z₁/(Z₁Z₂+Z₂Z₃+Z₃Z₁) | Reciprocal of Z₂ modified by network |
Y₃ = 1/Z₃ | Y₃ = Z₃/(Z₁Z₂+Z₂Z₃+Z₃Z₁) | Reciprocal of Z₃ modified by network |
Derivation Steps:
- Define determinant Δ = Z₁Z₂+Z₂Z₃+Z₃Z₁
- Use network theory to derive Y₁ = Z₂/Δ
- Similarly, Y₂ = Z₁/Δ
- And Y₃ = Z₃/Δ
Mnemonic: “Delta Divides: Y₁ gets Z₂, Y₂ gets Z₁, Y₃ gets Z₃”
Question 2(c) [7 marks]#
Three resistances of 1, 1 and 1 ohms are connected in Delta. Find equivalent resistances in star connection.
Answer:
Delta to Star Conversion:
Diagram:
Conversion Formulas:
- ra = (R₁×R₃)/(R₁+R₂+R₃)
- rb = (R₁×R₂)/(R₁+R₂+R₃)
- rc = (R₂×R₃)/(R₁+R₂+R₃)
Calculation: Given: R₁ = R₂ = R₃ = 1Ω Sum of resistances: R₁+R₂+R₃ = 3Ω
Star Resistor | Formula | Calculation | Result |
---|---|---|---|
ra | (R₁×R₃)/(R₁+R₂+R₃) | (1×1)/3 | 0.333Ω |
rb | (R₁×R₂)/(R₁+R₂+R₃) | (1×1)/3 | 0.333Ω |
rc | (R₂×R₃)/(R₁+R₂+R₃) | (1×1)/3 | 0.333Ω |
Mnemonic: “Product Over Sum: Each star arm gets the product of adjacent delta sides divided by the sum of all”
Question 2(a) OR [3 marks]#
Define. (i) Transfer Impedance (ii) Image Impedance (iii) Driving point Impedance
Answer:
Term | Definition |
---|---|
Transfer Impedance | Ratio of output voltage at one port to input current at another port when all other ports are open-circuited (Z₂₁ = V₂/I₁ when I₂=0) |
Image Impedance | Input impedance at port when the output port is terminated with its own image impedance, creating infinite chain with same impedance at all points |
Driving point Impedance | Input impedance seen when looking into a specified port or terminal pair (Z₁₁ = V₁/I₁ for port 1) |
Mnemonic: “TID: Transfer relates ports, Image creates reflections, Driving point looks inward”
Question 2(b) OR [4 marks]#
Get the equation for characteristics impedance Z for a standard ‘T’ network.
Answer:
Characteristic Impedance of ‘T’ network:
Diagram:
Derivation: For a symmetrical T-network with series impedance Z₁ (split as Z₁/2 on each side) and shunt impedance Z₂:
Z₀ = √(Z₁Z₂ + Z₁²/4)
Steps:
- ABCD parameters for T-network:
- A = 1 + Z₁/2Z₂
- B = Z₁ + Z₁²/4Z₂
- C = 1/Z₂
- D = 1 + Z₁/2Z₂
- From transmission line theory, Z₀ = √(B/C)
- Substituting: Z₀ = √((Z₁ + Z₁²/4Z₂)/(1/Z₂))
- Simplifying: Z₀ = √(Z₁Z₂ + Z₁²/4)
Mnemonic: “Square root of Z-products plus quarter-square”
Question 2(c) OR [7 marks]#
Three resistances of 6, 15 and 10 ohms are connected in star. Find equivalent resistances in delta connection.
Answer:
Star to Delta Conversion:
Diagram:
Conversion Formulas:
- R₁ = (ra×rb + rb×rc + rc×ra)/ra
- R₂ = (ra×rb + rb×rc + rc×ra)/rb
- R₃ = (ra×rb + rb×rc + rc×ra)/rc
Calculation: Given: ra = 6Ω, rb = 15Ω, rc = 10Ω Sum of products = (6×15) + (15×10) + (10×6) = 90 + 150 + 60 = 300
Delta Resistor | Formula | Calculation | Result |
---|---|---|---|
R₁ | (ra×rb + rb×rc + rc×ra)/ra | 300/6 | 50Ω |
R₂ | (ra×rb + rb×rc + rc×ra)/rb | 300/15 | 20Ω |
R₃ | (ra×rb + rb×rc + rc×ra)/rc | 300/10 | 30Ω |
Mnemonic: “Sum of Products Over Each: Delta side gets all products divided by opposite star arm”
Question 3(a) [3 marks]#
Analyze the circuit (R1, R2 and R3 Connected in series with dc supply) to calculate loop current using KVL.
Answer:
KVL for Series Circuit:
Diagram:
KVL Equation: VS - IR₁ - IR₂ - IR₃ = 0 Loop Current: I = VS/(R₁ + R₂ + R₃)
Steps:
- Identify all elements in the loop: VS, R₁, R₂, R₃
- Apply KVL: Sum of voltage rises = Sum of voltage drops
- Solve for I: I = VS/RT where RT = R₁ + R₂ + R₃
Mnemonic: “KVL: Kirchhoff’s Voltage Loop requires total resistance”
Question 3(b) [4 marks]#
State Norton’s theorem
Answer:
Norton’s Theorem:
Any linear electrical network consisting of voltage sources, current sources, and resistances can be replaced by an equivalent circuit consisting of a current source IN in parallel with a resistance RN.
Diagram:
How to find Norton equivalent:
- Norton Current (IN): Short-circuit current flowing through the load terminals
- Norton Resistance (RN): Input resistance seen at the terminals with all sources replaced by their internal resistances
Mnemonic: “SCIP: Short-Circuit current In Parallel with equivalent resistance”
Question 3(c) [7 marks]#
Explain the steps to calculate the current in any branch of the ckt using superposition theorem
Answer:
Superposition Theorem Application:
Principle: In a linear circuit with multiple sources, the response in any element equals the sum of responses caused by each source acting alone.
Steps:
- Consider only one source at a time
- Replace other voltage sources with short circuits
- Replace other current sources with open circuits
- Calculate partial current for each source
- Add all partial currents (algebraically) for final current
Diagram:
flowchart TD
A[1. Select one source] --> B[2. Replace other sources]
B --> C[3. Calculate partial current]
C --> D[4. Repeat for all sources]
D --> E[5. Sum partial currents]
Mathematical Expression: I = I₁ + I₂ + I₃ + … + In where I₁, I₂, etc. are partial currents due to individual sources
Example calculation: For a branch with current contributions: I₁ = 2A (from source 1) I₂ = -1A (from source 2) I₃ = 0.5A (from source 3) Total current = 2A + (-1A) + 0.5A = 1.5A
Mnemonic: “OSACI: One Source Active, Calculate and Integrate”
Question 3(a) OR [3 marks]#
Analyze the circuit (R1, R2 and R3 Connected in parallel with dc supply) to calculate node voltage using KCL.
Answer:
KCL for Parallel Circuit:
Diagram:
KCL Equation: I₁ + I₂ + I₃ = 0 Node Voltage: V = VS (because parallel elements have same voltage)
Steps:
- Identify node voltage V
- Express branch currents: I₁ = V/R₁, I₂ = V/R₂, I₃ = V/R₃
- Apply KCL: V/R₁ + V/R₂ + V/R₃ = VS/RT where 1/RT = 1/R₁ + 1/R₂ + 1/R₃
Mnemonic: “KCL: Kirchhoff’s Current Law means parallel voltage equals source”
Question 3(b) OR [4 marks]#
State Maximum power transfer theorem.
Answer:
Maximum Power Transfer Theorem:
For a source with internal resistance, maximum power is transferred to the load when the load resistance equals the source’s internal resistance.
Diagram:
Mathematical expression:
- Maximum power transfer occurs when RL = Rsource
- Maximum power: Pmax = V²/(4×Rsource)
Key points:
- Efficiency: Only 50% at maximum power transfer
- AC Circuits: Load impedance must be complex conjugate of source impedance
- Applications: Signal transmission, audio systems, RF circuits
Mnemonic: “MEET: Maximum Efficiency Equals when Thevenin-matched”
Question 3(c) OR [7 marks]#
Explain the steps to calculate Vth, Rth and load current in the ckt using Thevenin’s theorem
Answer:
Thevenin’s Theorem Application:
Principle: Any linear electrical network with voltage and current sources can be replaced by an equivalent circuit with a single voltage source Vth and a series resistance Rth.
Steps:
- Remove the load resistance from the circuit
- Calculate open-circuit voltage (Vth) across the load terminals
- Replace all sources with their internal resistances (voltage sources as short circuits, current sources as open circuits)
- Calculate equivalent resistance (Rth) seen from the load terminals
- Draw the Thevenin equivalent circuit with Vth and Rth
- Reconnect the load and calculate load current: IL = Vth/(Rth + RL)
Diagram:
flowchart TD
A[1. Remove load] --> B[2. Find Vth]
B --> C[3. Replace sources with internal resistances]
C --> D[4. Calculate Rth]
D --> E[5. Draw Thevenin equivalent]
E --> F[6. Reconnect load and calculate IL]
Example calculation:
- If Vth = 12V
- Rth = 3Ω
- RL = 6Ω
- Then IL = 12V/(3Ω + 6Ω) = 12V/9Ω = 1.33A
Mnemonic: “VORTE: Voltage Open, Resistance with sources Transformed, Equivalent circuit”
Question 4(a) [3 marks]#
Define resonance.
Answer:
Resonance:
Resonance is a phenomenon in which a circuit responds with maximum amplitude to an applied signal at a specific frequency called the resonant frequency.
Key characteristics:
- Impedance becomes purely resistive
- Inductive reactance equals capacitive reactance (XL = XC)
- Voltage and current are in phase
- Circuit stores and releases energy between L and C components
Applications:
- Tuning circuits
- Filters
- Oscillators
- Wireless communications
Mnemonic: “MAX-IN-PHASE: Maximum response when Inductive and capacitive reactances are equal and PHASEs cancel”
Question 4(b) [4 marks]#
Derive an equation for Quality factor of coil.
Answer:
Quality Factor (Q) of a Coil:
Definition: Q-factor is the ratio of energy stored to energy dissipated per cycle in a resonant circuit.
Derivation: For a coil with inductance L and resistance R:
- Energy stored in inductor: WL = ½LI²
- Power dissipated in resistance: P = I²R
- Time period: T = 1/f = 2π/ω
- Energy dissipated per cycle: Wd = P×T = I²R×(2π/ω)
- Q = 2π(Energy stored/Energy dissipated per cycle)
- Q = 2π(½LI²)/(I²R×2π/ω) = ωL/R
Final Equation: Q = ωL/R = 2πfL/R
Significance:
- Higher Q indicates lower energy loss
- Q increases with frequency
- Q decreases with resistance
Mnemonic: “Omega-L over R gives Quality”
Question 4(c) [7 marks]#
An RLC series circuit has R=1 KΩ, L=100 mH and C=10µF. If a voltage of 100 V is applied across series combination, determine: (i) Resonance frequency (ii) ‘Q’ factor
Answer:
RLC Series Circuit Analysis:
Diagram:
Calculations:
(i) Resonance frequency:
- Formula: fr = 1/(2π√(LC))
- fr = 1/(2π√(100×10⁻³ × 10×10⁻⁶))
- fr = 1/(2π√(1×10⁻⁶))
- fr = 1/(2π × 1×10⁻³)
- fr = 159.15 Hz
(ii) Quality factor (Q):
- Formula: Q = (1/R)√(L/C)
- Q = (1/1000)√(100×10⁻³/10×10⁻⁶)
- Q = (1/1000)√(10⁴)
- Q = (1/1000) × 100
- Q = 0.1
Parameter | Formula | Calculation | Result |
---|---|---|---|
Resonant frequency (fr) | 1/(2π√(LC)) | 1/(2π√(1×10⁻⁶)) | 159.15 Hz |
Quality factor (Q) | (1/R)√(L/C) | (1/1000)√(10⁴) | 0.1 |
Mnemonic: “Frequency from LC, Quality from LCR”
Question 4(a) OR [3 marks]#
Define Mutual Inductance.
Answer:
Mutual Inductance:
Mutual inductance is the property of a circuit whereby a change in current in one coil induces a voltage in another coil due to the magnetic coupling between them.
Mathematical expression:
- Voltage induced in coil 2: V₂ = -M(dI₁/dt)
- M = k√(L₁L₂) where k is the coupling coefficient (0≤k≤1)
- Unit: Henry (H)
Key properties:
- Depends on coil geometry, distance and orientation
- Proportional to both inductances
- Basis for transformers and coupled circuits
- Can be positive or negative based on mutual flux direction
Mnemonic: “MICK: Mutual Inductance links Coils through K-coupling”
Question 4(b) OR [4 marks]#
Derive equation of coefficient of coupling
Answer:
Coefficient of Coupling (k):
Definition: The coefficient of coupling (k) is a measure of the magnetic coupling between two coils, ranging from 0 (no coupling) to 1 (perfect coupling).
Derivation:
- Define mutual inductance: M = magnetic flux linkage / current
- For two coils with self-inductances L₁ and L₂:
- Flux linkage in coil 1 due to current in coil 1: λ₁₁ = L₁I₁
- Flux linkage in coil 2 due to current in coil 2: λ₂₂ = L₂I₂
- Flux linkage in coil 2 due to current in coil 1: λ₂₁ = MI₁
- The coupling coefficient k represents the fraction of flux from coil 1 that links with coil 2
- From electromagnetic theory: M = k√(L₁L₂)
- Rearranging: k = M/√(L₁L₂)
Final Equation: k = M/√(L₁L₂)
Key points:
- k = 0: No magnetic coupling
- 0 < k < 1: Partial coupling
- k = 1: Perfect coupling (all flux links both coils)
Mnemonic: “M divided by Geometric Mean of Ls”
Question 4(c) OR [7 marks]#
Derive resonance frequency of parallel resonance circuit.
Answer:
Parallel Resonance Frequency Derivation:
Diagram:
Derivation steps:
For a parallel RLC circuit, the admittance is: Y = 1/Z = 1/R + 1/jωL + jωC
At resonance, the imaginary part becomes zero: Im(Y) = 0 1/jωL + jωC = 0 -j/ωL + jωC = 0 1/ωL = ωC ω²LC = 1
For the ideal case (with infinite resistance): ω₀ = 1/√(LC) f₀ = 1/(2π√(LC))
For the real case (with resistance R): If R is in series with L, the resonant frequency becomes: f₀ = (1/2π)√(1/LC - R²/L²)
Final Equation:
- Ideal case: f₀ = 1/(2π√(LC))
- Real case (R in series with L): f₀ = (1/2π)√(1/LC - R²/L²)
Key characteristics of parallel resonance:
- Maximum impedance at resonance
- Minimum current drawn from source
- Current circulates between L and C
- Also called “anti-resonance” or “rejector circuit”
Mnemonic: “ONE over LC SQRT: The frequency where parallel paths balance”
Question 5(a) [3 marks]#
Classify various types of attenuators.
Answer:
Types of Attenuators:
Type | Structure | Characteristics |
---|---|---|
T-type | Series-shunt-series | Symmetric, good for matching, widely used |
∏-type | Shunt-series-shunt | Symmetric, alternative to T-type |
Lattice | Balanced bridge | Symmetrical, used in balanced lines |
L-type | Series-shunt | Asymmetric, simpler design |
Bridged-T | T with bridged shunt | Better frequency response, complex |
O-type | Series-shunt-series-shunt | Improved rejection characteristics |
Mnemonic: “TL∏BO: Top attenuators Let ∏ signals Balance Output”
Question 5(b) [4 marks]#
Derive relation between Decibel and Neper
Answer:
Decibel to Neper Conversion:
Definitions:
- Decibel (dB): Power ratio logarithm using base 10 (common logarithm)
- Neper (Np): Voltage/current ratio logarithm using base e (natural logarithm)
Derivation:
- Power ratio in dB: Loss(dB) = 10 log₁₀(P₁/P₂)
- Voltage ratio in dB: Loss(dB) = 20 log₁₀(V₁/V₂)
- Voltage ratio in Nepers: Loss(Np) = ln(V₁/V₂)
- Converting between logarithm bases: log₁₀(x) = ln(x)/ln(10)
- Substitute: Loss(dB) = 20 ln(V₁/V₂)/ln(10) = 20 Loss(Np)/ln(10)
Final Relation:
- 1 Neper = ln(10)/20 × 10 dB = 8.686 dB
- 1 dB = 0.115 Neper
Table:
Conversion | Formula | Value |
---|---|---|
Neper to dB | 1 Np = (20/ln10) dB | 1 Np = 8.686 dB |
dB to Neper | 1 dB = (ln10/20) Np | 1 dB = 0.115 Np |
Mnemonic: “8.686: Eight Point Six Nepers Buy Ten decibels”
Question 5(c) [7 marks]#
Design T type attenuator which provides 20 dB attenuation and having characteristics Impedance of 600 ohm.
Answer:
T-Type Attenuator Design:
Diagram:
Design Steps:
Calculate attenuation ratio N from dB: N = 10^(dB/20) = 10^(20/20) = 10
Calculate R₁ and R₂ using formulas:
- R₁ = R₀ × [(N² - 1)/(N² + 1)]
- R₂ = R₀ × [2N/(N² - 1)]
Calculation:
Given:
- Attenuation = 20 dB
- Characteristic impedance = 600 Ω
Parameter | Formula | Calculation | Result |
---|---|---|---|
N | 10^(dB/20) | 10^(20/20) | 10 |
R₁ | R₀[(N² - 1)/(N² + 1)] | 600[(10² - 1)/(10² + 1)] | 588.2 Ω |
Z₁/2 | R₁/2 | 588.2/2 | 294.1 Ω |
R₂ | R₀[2N/(N² - 1)] | 600[2×10/(10² - 1)] | 121.2 Ω |
Final T-network values:
- Each series arm (Z₁/2): 294.1 Ω
- Shunt arm (Z₂): 121.2 Ω
Mnemonic: “N-squared minus ONE over N-squared plus ONE for series resistance”
Question 5(a) OR [3 marks]#
State limitations of constant K low pass filters
Answer:
Limitations of Constant-K Low Pass Filters:
Limitation | Description |
---|---|
Poor cutoff transition | Gradual transition from pass band to stop band instead of sharp cutoff |
Uneven impedance | Impedance varies with frequency, causing matching problems |
Attenuation ripple | Non-uniform attenuation in both pass band and stop band |
Phase distortion | Non-linear phase response causing signal distortion |
Fixed termination | Designed for specific load impedance; performance deteriorates with other loads |
Limited selectivity | Poor selectivity compared to modern filter designs |
Mnemonic: “PUAPFL: Poor transition, Uneven impedance, Attenuation ripple, Phase distortion, Fixed termination, Limited selectivity”
Question 5(b) OR [4 marks]#
Give classification of filters showing frequency response curves For each of them
Answer:
Classification of Filters:
Filter Type | Frequency Response Curve | Characteristics |
---|---|---|
Low Pass | ```goat |
|\\
| \\
| \\________
|
+---------------
fc
``` | Passes frequencies below cutoff fc, blocks higher frequencies |
| High Pass | goat | _______ | / | / | / |/ +--------------- fc
| Blocks frequencies below cutoff fc, passes higher frequencies |
| Band Pass | goat | /\ | / \ | / \ | / \ |__/ \___ +--------------- f1 f2
| Passes frequencies between f1 and f2, blocks others |
| Band Stop | goat |___ ___ | \ / | \ / | \ / | \/ +--------------- f1 f2
| Blocks frequencies between f1 and f2, passes others |
Mnemonic: “LHBS: Low lets low tones, High lets high tones, Band-pass selects middle, Band-Stop rejects middle”
Question 5(c) OR [7 marks]#
Derive equation for designing a constant K low pass filters.
Answer:
Constant-K Low Pass Filter Design:
Diagram:
Design Theory: A constant-K filter has impedance product Z₁Z₂ = k² (constant) at all frequencies.
Derivation Steps:
For a T-section low-pass filter:
- Series impedance Z₁ = jωL
- Shunt impedance Z₂ = 1/jωC
Product Z₁Z₂ must be constant:
- Z₁Z₂ = jωL × 1/jωC = L/C = k²
Characteristic impedance at zero frequency:
- R₀ = √(L/C)
Cut-off frequency occurs when:
- Z₁ = 2Z₀ at ω = ωc
- jωcL = 2R₀ = 2√(L/C)
- ωc² = 4/LC
- ωc = 2/√(LC)
- fc = 1/π√(LC)
Design equations:
- L = R₀/πfc
- C = 1/(πfcR₀)
Final Equations:
- Cut-off frequency: fc = 1/π√(LC)
- Inductance: L = R₀/πfc
- Capacitance: C = 1/(πfcR₀)
T-section values:
- Series inductance: L/2 each arm
- Shunt capacitance: C
π-section values:
- Series inductance: L
- Shunt capacitance: C/2 each arm
Mnemonic: “One over Pi-Root-LC: The frequency where we Cut”