GTU Basic Electrical Engineering (3110005) Semester 1 Summer 2026 Solved Paper
Detailed worked solutions for the GTU Basic Electrical Engineering (3110005) Semester 1 Summer 2026 exam paper. Includes circuit analysis, formulas, diagrams, and calculations.
Introduction
This is an AI-generated student-friendly worked solution for the Gujarat Technological University (GTU) Semester 1 examination in Basic Electrical Engineering (Subject Code: 3110005) held on July 7, 2026. These solutions provide detailed explanations, standard equations, and step-by-step mathematical calculations. Please verify these answers against standard textbook solutions and your own classroom notes.
Paper Information
- University
- Gujarat Technological University
- Department
- First Year Engineering (Common)
- Semester
- 1
- Subject
- Basic Electrical Engineering
- Subject Code
- 3110005
- Exam
- Summer
- Year
- 2026
Questions and Solutions
Q1 (a)
Question
Define ideal current and ideal voltage source. State the difference between an Ideal and practical voltage source.
Solution
Definition of Ideal Current Source
An ideal current source is an active circuit element that delivers a constant current to any load circuit connected across its terminals, completely independent of the voltage across its terminals.
- Its internal resistance (or source resistance) is infinite (R_S = infinity).
- Regardless of the load resistance connected, the output current remains constant.
Definition of Ideal Voltage Source
An ideal voltage source is an active circuit element that maintains a constant terminal voltage across its terminals, completely independent of the current drawn by the load circuit.
- Its internal resistance is zero (R_S = 0).
- Regardless of the load current, the terminal voltage remains constant.
Difference Between Ideal and Practical Voltage Source
- Internal Resistance:
- Ideal Voltage Source: Has zero internal resistance (R_in = 0).
- Practical Voltage Source: Has a small, non-zero internal resistance (R_in > 0) connected in series with the ideal voltage source.
- Terminal Voltage vs. Load Current:
- Ideal Voltage Source: The terminal voltage remains perfectly constant (Vt = Vs) at all load currents.
- Practical Voltage Source: The terminal voltage decreases as the load current increases due to the internal voltage drop across the internal resistance (Vt = Vs - IL * Rin).
- Efficiency and Real-world Application:
- Ideal Voltage Source: It is a theoretical concept used for circuit modeling. It has 100% efficiency and would theoretically supply infinite power under short-circuit conditions.
- Practical Voltage Source: It represents real-world sources like batteries or generators. It has internal energy losses and cannot supply infinite power.
Q1 (b)
Question
What is power factor? List different methods of power factor improvement.
Solution
What is Power Factor?
The power factor (PF) of an alternating current (AC) electrical power system is defined as the ratio of real power (active power) flowing to the load to the apparent power in the circuit.
- Mathematically:
Power Factor = Real Power (P) / Apparent Power (S) = kW / kVA - In terms of impedance and resistance:
Power Factor = Cosine of the phase angle (theta) between voltage and current = R / Z - A power factor ranges from 0 to 1 (or 0% to 100%). It can be lagging (for inductive loads where current lags voltage) or leading (for capacitive loads where current leads voltage). A low power factor indicates that a larger current is drawn for the same amount of real power delivered, leading to higher system losses.
Methods of Power Factor Improvement
To improve the power factor, devices that draw leading reactive power are connected in parallel with the inductive loads. The primary methods are:
- Static Capacitors:
- Connected in parallel across the inductive loads.
- They draw leading reactive power (VAR), which neutralizes or cancels out the lagging reactive power of the inductive load.
- Widely used in industries due to low cost, high reliability, and low maintenance.
- Synchronous Condensers:
- An over-excited synchronous motor running at no-load acts as a synchronous condenser.
- When over-excited, it behaves like a capacitor and draws a leading current from the supply.
- Typically used in large substation environments where continuous, smooth control of power factor is required.
- Phase Advancers:
- These are AC exciters used to improve the power factor of induction motors.
- By supplying exciting ampere-turns at slip frequency to the rotor circuit, the stator is relieved of drawing magnetizing current from the mains, thereby improving the motor's power factor.
Q1 (c)
Question
Define following: (1) Average value (2) Maximum value (3) Frequency (4) Resonance (5) Form factor (6) Time period (7) Phase sequence
Solution
(1) Average Value
The average value of an alternating current or voltage is the arithmetic average of all instantaneous values over one complete cycle. For a symmetrical sinusoidal wave, the average value over a full cycle is zero; hence, it is defined over a half-cycle as:
- Average Value = (2 / pi) Maximum Value approx. 0.637 Vmax (or Imax)
(2) Maximum Value
Also known as the peak value or amplitude, this is the maximum instantaneous value attained by an alternating quantity (voltage or current) in either positive or negative direction during one complete cycle.
(3) Frequency
Frequency is the number of complete cycles completed by an alternating quantity per second.
- Measured in Hertz (Hz).
- Formula: f = 1 / T, where T is the time period.
(4) Resonance
Resonance in an AC circuit containing inductance (L) and capacitance (C) is a state in which the inductive reactance (XL) becomes equal to the capacitive reactance (XC). At this condition, the net reactive impedance is zero, and the circuit behaves as a purely resistive circuit, where current is in phase with the applied voltage.
(5) Form Factor
Form factor is the ratio of the Root Mean Square (RMS) value to the Average value of an alternating quantity.
- Form Factor = RMS Value / Average Value
- For a purely sinusoidal wave, Form Factor = 1.11.
(6) Time Period
The time period is the duration in seconds taken by an alternating quantity to complete one full cycle of variation.
- Denoted by T.
- Formula: T = 1 / f.
(7) Phase Sequence
Phase sequence is the chronological order in which the three phase voltages in a three-phase system reach their respective maximum positive values.
- The standard phase sequence is represented as R-Y-B (Red-Yellow-Blue).
Q2 (a)
Question
A single-phase R–L circuit has R=10 Ω, L=0.1 H, supplied by 230 V, 50 Hz. Calculate current, inductive reactance and impedance.
Solution
Given Data:
- Resistance, R = 10 Ω
- Inductance, L = 0.1 H
- Supply Voltage, V = 230 V
- Frequency, f = 50 Hz
Step 1: Calculate Inductive Reactance (X_L)
The inductive reactance is given by the formula:
- X_L = 2 pi f * L
- X_L = 2 3.14159 50 * 0.1
- X_L = 31.416 Ω
Step 2: Calculate Impedance (Z)
For a series R-L circuit, impedance is calculated as:
- Z = Square root of (R² + X_L²)
- Z = Square root of (10² + 31.416²)
- Z = Square root of (100 + 986.96)
- Z = Square root of (1086.96)
- Z = 32.97 Ω
Step 3: Calculate Circuit Current (I)
Using Ohm's law for AC circuits:
- I = V / Z
- I = 230 / 32.97
- I = 6.976 A
Summary of Results:
- Inductive Reactance (X_L): 31.42 Ω
- Impedance (Z): 32.97 Ω
- Current (I): 6.98 A
Q2 (b)
Question
List the main parts of a single-phase transformer.
Solution
The main constructional parts of a single-phase transformer are:
- Magnetic Core:
- Made of laminated silicon steel (high permeability, low hysteresis loss).
- Provides a continuous low-reluctance path for the magnetic flux.
- Windings (Coils):
- Primary Winding: Connected to the input power source.
- Secondary Winding: Connected to the load circuit.
- These windings are usually made of copper and are electrically isolated from each other.
- Insulation:
- Synthetic varnishes, insulating papers, and pressboard are used to insulate the windings from each other and from the core to prevent short-circuits.
- Enclosure / Container:
- A protective sheet metal housing (or tank) that contains the core, winding, and insulating oil (if oil-cooled) to protect them from moisture and physical damage.
- Terminals and Bushings:
- Used to safely bring out the terminal connections of the primary and secondary windings through the metallic container without shorting.
Q2 (c)
Question
Explain the construction and working of a three-phase induction motor with neat diagram. Also state the role of slip in its operation.
Solution
Construction of a 3-Phase Induction Motor
A three-phase induction motor consists of two main parts:
- Stator (Stationary Part):
- Stator Core: Built up of high-grade silicon steel laminations to reduce eddy current and hysteresis losses. It contains slots on its inner periphery.
- Stator Winding: Three-phase distributed windings placed in the slots, wound for a specific number of poles, and connected in star or delta.
- Rotor (Rotating Part):
- Mounted on the shaft. It can be of two types:
- Squirrel Cage Rotor: Consists of heavy copper or aluminum bars inserted in the rotor slots and short-circuited at both ends by end-rings.
- Phase Wound / Slip Ring Rotor: Has a distributed three-phase winding similar to the stator, with terminals connected to three insulated slip rings mounted on the shaft.
`` +---------------------------------+ | STATOR CORE | | +-------------------------+ | | | Stator 3-Phase Winding | | | | (R, Y, B Phase) | | | | +-----------------+ | | | | | | | | | | | ROTOR BARS | | | | | | / / / / | | | | | | [ Shaft ] | | | | | | / / / / | | | | | | (Squirrel Cage)| | | | | +-----------------+ | | | +-------------------------+ | +---------------------------------+ ``
Working Principle
- When a 3-phase AC supply is connected to the stator winding, balanced currents flow in the three windings.
- These currents produce a Rotating Magnetic Field (RMF) that rotates at a constant synchronous speed, N_s = 120 * f / P.
- This rotating flux cuts across the stationary rotor conductors.
- According to Faraday's law of electromagnetic induction, an electromotive force (EMF) is induced in the rotor conductors.
- Since the rotor conductors form a closed circuit (via end-rings or slip rings), a rotor current flows.
- According to Lorenz force principle, a current-carrying conductor placed in a magnetic field experiences a mechanical force.
- The interaction between the stator's RMF and the rotor's current produces a torque that causes the rotor to rotate in the direction of the rotating magnetic field (Lenz's law).
Role of Slip
- Definition of Slip: Slip (s) is the fractional difference between the synchronous speed (N_s) of the stator magnetic field and the actual speed (N) of the rotor:
s = (Ns - N) / Ns - Role in Operation:
- Source of Rotor EMF: The induction motor runs because of the relative speed between the rotating magnetic field and the rotor. If the rotor were to run at synchronous speed (N = N_s), there would be no relative motion, zero magnetic flux cutting, zero induced EMF, zero rotor current, and thus zero electromagnetic torque.
- Therefore, the rotor must always run at a speed (N) slightly less than the synchronous speed (N_s) so that there is a non-zero slip to produce torque.
- Slip determines the frequency of rotor currents (f_r = s * f) and directly controls the torque and current characteristics under load.
OR Q2 (c)
Question
Explain the construction and working of a single-phase induction motor with neat diagram. Why is it not self-starting?
Solution
Construction of a Single-Phase Induction Motor
A single-phase induction motor consists of:
- Stator:
- A laminated core containing slots.
- Carries a main winding (running winding) excited by a single-phase AC supply.
- It also usually contains an auxiliary winding (starting winding) displaced by 90 electrical degrees in space.
- Rotor:
- Almost always of the squirrel cage type.
- Consists of uninsulated aluminum or copper bars placed in rotor slots, short-circuited at both ends by end-rings.
- Centrifugal Switch:
- Connected in series with the auxiliary winding to disconnect it once the motor reaches about 75% to 80% of its synchronous speed.
`` +----------------------------+ | STATOR CORE | | +------------------+ | | | Main Winding | | | | +------------+ | | | | | Rotor Bars | | | | | | [ Shaft ] | | | | | +------------+ | | | | Auxiliary Wind. | | | +------------------+ | +----------------------------+ ``
Working Principle (With Auxiliary Winding)
- Single-phase supply is applied to the stator winding.
- To make it self-starting, the auxiliary winding is connected in parallel with the main winding, usually with a capacitor in series. This produces a phase difference between the currents of the two windings.
- The two phase currents produce a rotating magnetic field in the air gap, similar to a 2-phase motor.
- This rotating field induces EMF in the rotor bars, creating rotor current and generating a starting torque that rotates the rotor.
Why is a Single-Phase Induction Motor Not Self-Starting?
- Double Revolving Field Theory:
- According to this theory, a single-phase alternating magnetic flux can be resolved into two rotating magnetic fields of equal magnitude, rotating in opposite directions at synchronous speed.
- Opposing Torques:
- One field rotates clockwise (forward field) and produces a forward torque (T_f).
- The other field rotates counter-clockwise (backward field) and produces a backward torque (T_b).
- Net Zero Torque at Start:
- At standstill (speed N = 0), the slip with respect to both fields is identical (s = 1).
- Thus, the forward torque and the backward torque are equal in magnitude but opposite in direction: Tf = Tb.
- The net starting torque is exactly zero.
- Consequently, the motor is not self-starting. If started manually in either direction, it will continue to run in that direction.
Q3 (a)
Question
Write short notes on plate earthing.
Solution
Short Notes on Plate Earthing
Plate earthing is one of the most reliable and efficient methods of grounding electrical installations to ensure safety against leakage currents.
- Materials used:
- A copper plate of size 60 cm x 60 cm x 3.18 mm, or a galvanized iron (GI) plate of size 60 cm x 60 cm x 6.3 mm is placed vertically in the earth.
- Installation Procedure:
- A pit of size about 2 to 3 meters deep is dug in the ground.
- The plate is embedded vertically at the bottom of the pit.
- The plate is surrounded by alternative layers of charcoal and salt to a thickness of about 15 cm. The charcoal-salt mixture absorbs and retains moisture, maintaining low soil resistance.
- A GI pipe with a funnel at the top is connected to the plate to facilitate pouring water periodically to keep the ground damp.
- Earthing Conductor:
- The earth lead wire (usually copper or GI) is securely bolted to the plate using washers and nuts and is brought out to the surface through a protective pipe.
Q3 (b)
Question
Compare mesh analysis with nodal analysis. Analyze which method is more suitable for circuits with more voltage sources.
Solution
Comparison Between Mesh and Nodal Analysis
| Parameter | Mesh Analysis | Nodal Analysis | | :--- | :--- | :--- | | Basic Law | Based on Kirchhoff's Voltage Law (KVL) and Ohm's Law. | Based on Kirchhoff's Current Law (KCL) and Ohm's Law. | | Variables | Uses loop/mesh currents as variables. | Uses node voltages as variables. | | Application | Only applicable to planar circuits. | Applicable to both planar and non-planar circuits. | | Number of Equations | Number of equations, e = b - n + 1 (where b = branches, n = nodes). | Number of equations, e = n - 1. |
Analysis: Suitability for Circuits with More Voltage Sources
If a circuit contains more voltage sources, the choice of method is influenced by how these sources are connected:
- When voltage sources are connected between nodes and reference node:
- Nodal Analysis becomes much easier because the node voltages at those nodes are directly known (no need to write KCL equations for those nodes). This reduces the number of simultaneous equations to solve.
- If a voltage source is connected between two non-reference nodes, a "Supernode" is formed, which reduces the number of equations by one.
- When there are many series voltage sources in the meshes:
- Mesh Analysis can be straightforward because the voltages directly add or subtract in the KVL loop equations. However, if there are current sources, they introduce "Supermesh" constraints.
Conclusion: For a circuit with numerous independent voltage sources, Nodal Analysis is generally more suitable and simpler because the presence of voltage sources reduces the number of independent node variables, thereby minimizing the mathematical complexity of the simultaneous linear equations.
Q3 (c)
Question
Explain the construction and working principle of ELCB with necessary diagram.
Solution
Construction of an Earth Leakage Circuit Breaker (ELCB)
An Earth Leakage Circuit Breaker (ELCB) is a safety device used to directly detect currents leaking to earth from an installation and interrupt the power supply. Modern ELCBs are generally current-operated and are also known as Residual Current Circuit Breakers (RCCB).
The primary parts of a current-operated ELCB are:
- Toroidal Iron Core (CBCT - Core Balance Current Transformer): A circular magnetic core through which both the Phase (Line) and Neutral wires pass.
- Sensing / Search Coil: A multi-turn secondary winding wound on the toroidal core, connected to a highly sensitive electromagnetic relay mechanism.
- Relay and Tripping Mechanism: A spring-loaded mechanical switch connected to the main contacts.
- Test Button and Resistor: Connected across one phase and neutral outside the CBCT to simulate a fault and test the device periodically.
`` Line o=======+=========+=================o To Load (Phase) | | +---------+ | +--+---| CBCT | | | | | Core | [R] | | +---------+ | (Test) | | Neutral o=====+======+==|===+=========+===o To Load (Neutral) | | | +--> [Sensing Coil] | | +-------> [Tripping Relay] ---> Opens Contacts ``
Working Principle
- Normal Condition (No Leakage):
- Under healthy conditions, the current flowing to the load through the Phase wire (IP) is exactly equal to the current returning through the Neutral wire (IN).
- The magnetic fluxes produced by IP and IN in the toroidal core are equal in magnitude but opposite in direction.
- Therefore, the net magnetic flux in the core is zero, and no EMF is induced in the search coil. The tripping relay remains inactive.
- Fault Condition (Leakage to Earth):
- When a fault occurs (e.g., a person touches a live wire, or insulation fails, causing current to leak to the earth), some current flows to the ground.
- Now, the current in the Phase wire is greater than the current in the Neutral wire (IP > IN).
- This difference (IP - IN = I_residual) creates a net alternating magnetic flux in the toroidal core.
- This changing magnetic flux cuts the search coil, inducing an EMF across its terminals.
- The induced EMF sends current through the sensing relay, energizing the electromagnet.
- The electromagnet releases the spring-loaded contacts, instantly tripping the circuit and isolating the faulty load from the supply.
OR Q3 (a)
Question
Differentiate between primary and secondary batteries.
Solution
Differences Between Primary and Secondary Batteries
| Parameter | Primary Batteries | Secondary Batteries | | :--- | :--- | :--- | | Reversibility | Non-rechargeable. The chemical reactions are irreversible. | Rechargeable. The chemical reactions are highly reversible. | | Life Cycle | Single-use. Once discharged, they must be discarded. | Multiple-use. Can be charged and discharged hundreds of times. | | Internal Resistance| Comparatively high. | Comparatively low. | | Initial Cost | Low and economical for one-time use. | High initial cost due to charging circuitry and design. | | Energy Density | High energy density, discharges slowly over a long period. | Moderate energy density, can deliver high current peaks. | | Examples | Zinc-carbon cells, Alkaline cells, Mercury cells. | Lead-acid batteries, Lithium-ion batteries, Ni-MH batteries. |
OR Q3 (b)
Question
Two RL circuits have the same inductance but different resistances: Circuit A: R=2 Ω, Circuit B: R=10 Ω. Compare their time constants. Analyze which circuit responds faster and justify.
Solution
Step 1: Definition of Time Constant for an R-L Circuit
The time constant (tau) of a series R-L circuit is defined as the ratio of its inductance (L) to its resistance (R):
- tau = L / R (seconds)
Step 2: Comparison of Time Constants
Let both circuits have the same inductance, L.
- For Circuit A:
R_A = 2 Ω
tau_A = L / 2 = 0.5 * L
- For Circuit B:
R_B = 10 Ω
tau_B = L / 10 = 0.1 * L
Comparing the two:
- tauA / tauB = (0.5 L) / (0.1 L) = 5
- This means the time constant of Circuit A is 5 times larger than the time constant of Circuit B (tauA = 5 * tauB).
Step 3: Analysis of Response Speed
- The time constant is a measure of the time taken by the current in an R-L circuit to reach 63.2% of its final steady-state value during transient growth, or to decay to 36.8% of its initial value.
- A smaller time constant means the circuit reaches its steady state much quicker.
- Since tauB = 0.1 * L is much smaller than tau
Justification
The resistance in Circuit B is five times larger than that of Circuit A. A higher resistance opposes the flow of current more strongly and dampens the transient inductive behavior faster, resulting in a quicker transition to steady-state operation. Hence, Circuit B responds faster.
OR Q3 (c)
Question
Explain the construction and working principle of MCB with necessary diagram.
Solution
Construction of a Miniature Circuit Breaker (MCB)
A Miniature Circuit Breaker (MCB) is an automatically operated electrical switch designed to protect an electrical circuit from damage caused by excess current from overload or short circuit.
Its main component parts are:
- Bimetallic Strip: Consists of two metals with different coefficients of thermal expansion bonded together. Used for overload (slow, thermal) protection.
- Solenoid / Magnetic Tripping Coil: An electromagnetic coil that produces a strong magnetic force under high current conditions. Used for short-circuit (instantaneous, electromagnetic) protection.
- Operating Mechanism & Contacts: Spring-loaded moving and fixed contacts that close or open the circuit.
- Arc Chute: A series of parallel metal plates designed to split, cool, and extinguish the electrical arc formed during contact separation.
- Incoming/Outgoing Terminals: For connection of line conductors.
`` Line/Inlet Terminal | [ Bimetallic Strip ] <--- (Overload Heating) | === Moving Contact (Spring Loaded) === Fixed Contact | [ Magnetic Tripping Coil ] <--- (Short-circuit Solenoid) | Load/Outlet Terminal ``
Working Principle
An MCB operates on two different principles to protect against two distinct fault conditions:
- Thermal Protection (For Overload Conditions):
- Under overload conditions, the current passing through the MCB is slightly above the rated limit for a sustained period.
- This continuous overcurrent heats up the bimetallic strip.
- Due to differing expansion coefficients, the strip bends significantly.
- The bending deflection mechanically releases the latch mechanism, allowing the spring-loaded contacts to open, thus cutting off the supply.
- Magnetic Protection (For Short-Circuit Conditions):
- During a short-circuit, a very high fault current flows through the circuit.
- This high current flows through the magnetic tripping coil (solenoid), generating a very strong magnetic field instantly.
- This magnetic force pulls a plunger inside the solenoid, which directly strikes the trip latch.
- The contacts are separated instantaneously (within milliseconds), preventing severe damage to the installation.
- The resulting electric arc is drawn into the arc chute where it is split and rapidly quenched.
Q4 (a)
Question
List the main parts of a separately excited DC motor.
Solution
The main parts of a separately excited DC motor are:
- Yoke (Frame): The outer protective cover that provides mechanical support to the poles and serves as a path for magnetic flux.
- Field Poles & Pole Shoes: Steel cores with laminated sheets that produce the magnetic field when energized by an external DC supply.
- Armature Core: A cylindrical drum made of laminated silicon steel slots to house the armature winding.
- Armature Winding: Copper conductors placed in armature slots that carry current and experience torque.
- Commutator: A cylindrical ring of copper segments separated by mica insulation that reverses the current direction in armature conductors to maintain unidirectional torque.
- Brushes and Brush Holders: Carbon or graphite blocks that make sliding contact with the commutator to feed current from the external source to the rotating armature.
Q4 (b)
Question
State the working principle and EMF equation of the transformer. Define Turns ratio.
Solution
Working Principle of a Transformer
A transformer is a static electromagnetic device that works on the principle of Faraday's Law of Electromagnetic Induction, specifically mutual induction between two or more windings.
- When an alternating voltage is applied to the primary winding, an alternating current flows through it, producing an alternating magnetic flux in the magnetic core.
- This alternating flux passes through the core and links with the secondary winding.
- According to Faraday's Law, this changing flux linkage induces an alternating EMF in the secondary winding. If the secondary circuit is closed, a current flows to the connected load.
EMF Equation of a Transformer
The RMS value of the induced EMF in the windings is given by:
- E1 = 4.44 f N1 * Phi_m (for primary winding)
- E2 = 4.44 f N2 * Phi_m (for secondary winding)
Where:
- E1 = RMS value of primary induced EMF (in Volts)
- E2 = RMS value of secondary induced EMF (in Volts)
- f = Frequency of the AC supply (in Hz)
- N1 = Number of turns in the primary winding
- N2 = Number of turns in the secondary winding
- Phim = Maximum magnetic flux in the core (in Webers, Wb) = B
Turns Ratio (K)
The Turns Ratio (often denoted by K) is defined as the ratio of the number of turns in the secondary winding (N2) to the number of turns in the primary winding (N1).
- Turns Ratio = N2 / N1
- In an ideal transformer, this is also equal to the ratio of induced voltages:
N2 / N1 = E2 / E1 = V2 / V1 = K
Q4 (c)
Question
Derive condition XL=XC in series RLC resonance. Explain why impedance is minimum. Draw and analyze: variation of current vs frequency, variation of impedance vs frequency, Identify resonance point.
Solution
Derivation of Resonance Condition (XL = XC)
In a series R-L-C circuit connected across an alternating voltage supply of variable frequency, the total impedance is given by:
- Z = Square root of [ R² + (XL - XC)² ]
Where:
- X_L = 2 pi f * L (Inductive Reactance)
- X_C = 1 / (2 pi f * C) (Capacitive Reactance)
The phase angle (theta) between voltage and current is:
- tan(theta) = (XL - XC) / R
Resonance is defined as the state in which the circuit current is in phase with the applied voltage (unity power factor). For current to be in phase with voltage, the phase angle must be zero:
- tan(theta) = 0
- (XL - XC) / R = 0
- XL - XC = 0
- XL = XC (Condition for Resonance)
This can be written in terms of frequency (f_r):
- 2 pi fr * L = 1 / (2 * pi * fr * C)
- (f_r)² = 1 / (4 pi² L * C)
- f_r = 1 / [ 2 pi Square root of (L * C) ] (Resonant Frequency)
Why Impedance is Minimum at Resonance
From the impedance formula:
- Z = Square root of [ R² + (XL - XC)² ]
The term (XL - XC)² is always positive or zero. To minimize Z, this term must be zero:
- At resonance, XL = XC, which means (XL - XC)² = 0.
- Therefore, the impedance reduces to:
Z_min = R
At resonance, the reactive components cancel each other out, making the impedance purely resistive and equal to the minimum possible value (R).
Variation of Current and Impedance vs Frequency
Below is a visual representation of how Impedance (Z) and Current (I) vary with frequency (f):
`` Impedance Z vs Frequency Current I vs Frequency Z ^ I ^ | \ / | .-"Imax"-. | \ / | ." | ". | \ / | / | \ | \ / | / | \ |
Analysis:
- Below Resonant Frequency (f < f_r):
- XC is larger than XL (since X_C is inversely proportional to f).
- The circuit behaves as a leading capacitive circuit (R-C nature).
- The impedance Z is high, so the current I is low.
- At Resonant Frequency (f = f_r):
- XL = XC.
- Impedance is at its absolute minimum value: Z = R.
- The current reaches its peak maximum value: I_max = V / R.
- The circuit acts as a purely resistive circuit.
- Above Resonant Frequency (f > f_r):
- XL becomes larger than XC (since X_L is directly proportional to f).
- The circuit behaves as a lagging inductive circuit (R-L nature).
- The impedance Z increases again, and consequently, the current I decreases.
OR Q4 (a)
Question
List the main parts of a synchronous generator.
Solution
The main parts of a synchronous generator (alternator) are:
- Stator (Stationary Armature):
- Stator Frame: Holds the stator core in place.
- Stator Core: Laminated silicon steel rings with slots on the inner periphery.
- Stator Winding: Three-phase distributed winding where AC voltage is induced.
- Rotor (Rotating Field):
- Carries the field winding excited by a DC source to produce magnetic poles. There are two types:
- Salient Pole Rotor: Projecting poles, used for low-speed applications (hydro power).
- Smooth Cylindrical Rotor: Non-projecting poles, used for high-speed applications (steam turbogenerators).
- Exciter:
- A small DC source (such as a DC generator or rectifier system) that supplies the magnetizing DC current to the rotor field windings.
- Slip Rings and Brushes:
- Conductive rings mounted on the rotor shaft to transfer the DC excitation current from the stationary exciter system to the rotating rotor coils.
OR Q4 (b)
Question
Identify the primary difference between a step-up and a step-down transformer in terms of their turn ratios. State which winding (primary or secondary) has thicker wire in a step-down transformer.
Solution
Difference in Terms of Turn Ratios
The primary difference lies in the turns ratio, K = N2 / N1, where N1 is primary turns and N2 is secondary turns:
- Step-Up Transformer:
- It increases the voltage from primary to secondary (V2 > V1).
- Therefore, the number of turns on the secondary winding is greater than on the primary winding (N2 > N1).
- The turns ratio K > 1.
- Step-Down Transformer:
- It decreases the voltage from primary to secondary (V2 < V1).
- Therefore, the number of turns on the secondary winding is less than on the primary winding (N2 < N1).
- The turns ratio K < 1.
Which Winding Has Thicker Wire in a Step-Down Transformer?
In a transformer, neglecting power losses, the apparent power rating is constant on both sides (V1 I1 = V2 I2).
- In a step-down transformer, the secondary voltage is lower than the primary voltage (V2 < V1).
- Consequently, the secondary current must be higher than the primary current (I2 > I1).
- To carry this higher current safely without overheating and to keep resistance losses low, the secondary winding must have a larger cross-sectional area.
- Thus, the secondary winding has thicker wire in a step-down transformer.
OR Q4 (c)
Question
A balanced 3-phase, 3-wire load is supplied with a line voltage of 400 V. The readings of two wattmeter connected by the two-wattmeter method are: W1=5 kW, W2=1 kW. Determine: Power factor of the load, Nature of power factor (lagging or leading), Phase angle of the load.
Solution
Given Data:
- Line Voltage, V_L = 400 V
- Wattmeter 1 Reading, W1 = 5 kW = 5000 W
- Wattmeter 2 Reading, W2 = 1 kW = 1000 W
Step 1: Calculate Total Active Power (P)
- P = W1 + W2
- P = 5 kW + 1 kW = 6 kW = 6000 W
Step 2: Calculate Phase Angle (theta)
In the two-wattmeter method, the phase angle theta of the load is calculated using the relation:
- tan(theta) = Square root of (3) * [ (W1 - W2) / (W1 + W2) ]
Assuming W1 is the larger reading:
- tan(theta) = 1.732 * [ (5 - 1) / (5 + 1) ]
- tan(theta) = 1.732 * [ 4 / 6 ]
- tan(theta) = 1.732 * 0.6667
- tan(theta) = 1.1547
Now, find the phase angle (theta):
- theta = arctan(1.1547)
- theta = 49.11 degrees
Step 3: Determine Power Factor (PF) of the Load
- PF = cos(theta)
- PF = cos(49.11 degrees)
- PF = 0.6546 (approx. 0.655)
Step 4: Determine the Nature of Power Factor
- For a standard balanced passive inductive load (such as motors), the current lags the voltage. Since the prompt specifies a balanced 3-phase load without adding capacitive components, the nature of the power factor is lagging.
Summary of Results:
- Phase Angle of the Load (theta): 49.11°
- Power Factor of the Load: 0.655
- Nature of Power Factor: Lagging
Q5 (a)
Question
Explain in brief construction of single phase transformer with neat diagram.
Solution
Construction of a Single-Phase Transformer
A single-phase transformer is structurally classified into two types: Core Type and Shell Type.
- Core Type:
- The windings surround the magnetic core limbs.
- It has a single magnetic circuit.
- High-voltage and low-voltage windings are wound concentrically on each limb (with low-voltage winding closer to the core to minimize insulation requirements).
- Shell Type:
- The magnetic core surrounds the windings.
- It has a double magnetic circuit with three limbs; the windings are wound on the central limb.
`` CORE TYPE TRANSFORMER SHELL TYPE TRANSFORMER +-------------------+ +---+-----------+---+ | Magnetic Core | | | Magnetic | | | +-------------+ | | | Core | | [W] | | [W] | +--+ +--+ | [I] | | [I] | | | [W] | | | [N] | | [N] | | | [I] | | | [D] | | [D] | | | [N] | | | [I] | | [I] | | | [D] | | | [N] | | [N] | | | [I] | | | [G] | | [G] | | | [G] | | | | +-------------+ | | +--+ +--+ | +-------------------+ +---+-----------+---+ ``
- Core Lamination: The core is made of thin silicon steel sheets (laminations) of 0.35 mm to 0.5 mm thickness, varnished and pressed together to minimize eddy current losses.
Q5 (b)
Question
A balanced load is connected first in star and then in delta across the same supply. Compare line current in both cases. Analyze power consumption in both connections.
Solution
Let the load have an impedance per phase of Zph and let it be connected across a 3-phase supply of line voltage VL.
Case 1: Star Connection (Y)
- Phase voltage, VphY = V_L / Square root of (3)
- Phase current, IphY = VphY / Zph = VL / [ Z_ph * Square root of (3) ]
- In star connection, line current (ILY) is equal to phase current:
ILY = VL / [ Zph * Square root of (3) ] - Total Power consumed, PY = 3 * (IphY)² * Rph = 3 [ V_L² / (3 Zph²) ] * Rph
PY = (VL² * Rph) / Zph²
Case 2: Delta Connection (Delta)
- Phase voltage, VphD = V_L
- Phase current, IphD = VphD / Zph = VL / Z_ph
- In delta connection, line current (ILD) is:
ILD = Square root of (3) * IphD
ILD = [ Square root of (3) * VL ] / Zph - Total Power consumed, PD = 3 * (IphD)² * Rph
PD = 3 * (VL² * Rph) / Zph²
Comparison and Analysis
- Comparison of Line Currents:
- Divide ILD by ILY:
ILD / ILY = { [ Square root of (3) V_L ] / Z_ph } / { V_L / [ Z_ph Square root of (3) ] }
ILD / ILY = 3 - Therefore:
ILD = 3 * ILY - The line current in a delta connection is three times the line current in a star connection for the same load and supply.
- Analysis of Power Consumption:
- Divide PD by PY:
PD / PY = [ 3 (V_L² Rph) / Zph² ] / [ (VL² * Rph) / Z_ph² ] = 3 - Therefore:
PD = 3 * PY - The power consumed by a balanced load connected in delta is three times the power consumed when connected in star across the same supply.
Q5 (c)
Question
Using the Superposition Theorem, find the current through the 6 Ω resistor in the given circuit.
Solution
Important Statement Regarding Missing Diagram
Note: The circuit diagram referred to as the "given circuit" is not present in the exam text. To show the step-by-step application of the Superposition Theorem, we will define a standard, typical GTU network containing a 6 Ω resistor, two sources, and apply the Superposition Theorem systematically.
Let's assume a typical test circuit:
- An active bilateral network containing two voltage sources:
- Source 1: V1 = 12 V (on the left)
- Source 2: V2 = 6 V (on the right)
- Resistors: R1 = 4 Ω (in series with V1), R2 = 2 Ω (in series with V2), and the load resistor R_L = 6 Ω connected in the middle branch.
Step-by-Step Solution using Superposition Theorem
Superposition states that the response (current) in any branch of a linear, bilateral network with multiple independent sources is equal to the algebraic sum of responses caused by each independent source acting alone, with all other independent sources turned off (voltage sources short-circuited and current sources open-circuited).
Case I: Activating the 12 V source alone (6 V source is short-circuited)
- The 6 V voltage source on the right is replaced by a short circuit.
- The 2 Ω resistor is now in parallel with the 6 Ω branch.
- Equivalent parallel resistance, R_p = (6 * 2) / (6 + 2) = 12 / 8 = 1.5 Ω.
- Total resistance seen by the 12 V source:
- Rtotal = R1 + Rp = 4 + 1.5 = 5.5 Ω.
- Total current from the 12 V source:
- I_total1 = 12 V / 5.5 Ω = 2.18 A.
- Current flowing through the 6 Ω resistor (I61) using the current division rule:
- I61 = I_total1 * [ 2 / (6 + 2) ]
- I61 = 2.18 * [ 2 / 8 ] = 0.545 A (downward direction).
Case II: Activating the 6 V source alone (12 V source is short-circuited)
- The 12 V voltage source on the left is replaced by a short circuit.
- The 4 Ω resistor is now in parallel with the 6 Ω branch.
- Equivalent parallel resistance, R_p2 = (6 * 4) / (6 + 4) = 24 / 10 = 2.4 Ω.
- Total resistance seen by the 6 V source:
- Rtotal2 = R2 + Rp2 = 2 + 2.4 = 4.4 Ω.
- Total current from the 6 V source:
- I_total2 = 6 V / 4.4 Ω = 1.364 A.
- Current flowing through the 6 Ω resistor (I62) using current division:
- I62 = I_total2 * [ 4 / (6 + 4) ]
- I62 = 1.364 * [ 4 / 10 ] = 0.545 A (downward direction).
Step 3: Total Superposition Current
Since both components of current (I61 and I62) flow in the same downward direction, the algebraic sum is:
- I6total = I61 + I62
- I6total = 0.545 A + 0.545 A = 1.09 A
(Note: In the actual exam, replace the steps with the respective values from your specific examination paper diagram.)
OR Q5 (a)
Question
Explain autotransformer in brief and describe the primary structural difference between the autotransformer and normal transformer.
Solution
What is an Autotransformer?
An autotransformer is a type of electrical transformer that has only one continuous winding wound on a laminated magnetic core. This single winding serves as both the primary and secondary windings.
- Part of the winding is common to both primary and secondary circuits.
- It works on the principle of self-induction as well as mutual induction.
- It is commonly used as a "Variac" to obtain variable AC voltage in laboratories.
Primary Structural Difference
The main structural differences between an autotransformer and a normal (two-winding) transformer are:
- Number of Windings:
- Normal Transformer: Has two separate, distinct windings (primary and secondary) wound on the core.
- Autotransformer: Has only a single, continuous winding with intermediate tapping points.
- Electrical Isolation:
- Normal Transformer: The primary and secondary windings are electrically completely isolated from each other. Energy transfer is purely magnetic.
- Autotransformer: The primary and secondary circuits are electrically connected. Energy is transferred both conductively (through the electrical connection) and inductively (through the magnetic field).
- Size and Weight:
- Due to the shared winding, an autotransformer requires significantly less copper and core material compared to a two-winding transformer of the same rating, making it more compact and less expensive.
OR Q5 (b)
Question
A balanced star-connected load has: VL=400 V, Zph=10+j5 Ω. Calculate phase voltage, phase and line current, power factor, total power.
Solution
Given Data:
- Star-connected load
- Line Voltage, V_L = 400 V
- Phase Impedance, Z_ph = 10 + j5 Ω
Step 1: Calculate Phase Voltage (V_ph)
For a balanced star (Y) connected system:
- Vph = VL / Square root of (3)
- V_ph = 400 / 1.7321
- V_ph = 230.94 V
Step 2: Calculate Phase Impedance Magnitude (|Z_ph|)
- |Z_ph| = Square root of (R² + X²)
- |Z_ph| = Square root of (10² + 5²)
- |Z_ph| = Square root of (100 + 25) = Square root of (125)
- |Z_ph| = 11.18 Ω
Step 3: Calculate Phase Current (Iph) and Line Current (IL)
- Iph = Vph / |Z_ph|
- I_ph = 230.94 / 11.18
- I_ph = 20.66 A
For a star connection, the line current is equal to the phase current:
- IL = Iph = 20.66 A
Step 4: Calculate Power Factor (PF)
- PF = Cos(theta) = R / |Z_ph|
- PF = 10 / 11.18
- PF = 0.894 (Lagging, because inductive reactance is positive (+j5))
Step 5: Calculate Total Power (P)
The total active power consumed by a balanced 3-phase load is:
- P = Square root of (3) V_L I_L * PF
- P = 1.7321 400 20.66 * 0.894
- P = 12792.8 Watts approx. 12.79 kW
Summary of Results:
- Phase Voltage (V_ph): 230.94 V
- Phase and Line Current (Iph = IL): 20.66 A
- Power Factor (PF): 0.894 (Lagging)
- Total Power (P): 12.79 kW
OR Q5 (c)
Question
Using Thevenin’s Theorem, find the current through the load resistor RL=3 Ω for the given circuit.
Solution
Important Statement Regarding Missing Diagram
Note: The circuit diagram for the "given circuit" is not present in the exam text. To illustrate the exact analytical steps, we will perform calculations based on a classic typical GTU circuit configuration containing a 3 Ω load resistor.
Let's assume a standard DC circuit network:
- A DC source V = 12 V
- Resistors forming a T-network: R1 = 2 Ω (series-in), R2 = 2 Ω (parallel-shunt), R3 = 1 Ω (series-out leading to load)
- Load Resistor: R_L = 3 Ω
Step-by-Step Solution using Thevenin’s Theorem
Step 1: Remove the Load Resistor and find Thevenin's Voltage (V_th)
- Disconnect R_L = 3 Ω from the output terminals A and B.
- The circuit becomes an open loop across the 2 Ω shunt resistor R2.
- Because no current flows through the series resistor R3 = 1 Ω under open-circuit conditions, the voltage across terminals A and B is simply the voltage drop across R2:
- V_th = V * [ R2 / (R1 + R2) ]
- V_th = 12 V [ 2 / (2 + 2) ] = 12 0.5 = 6 V
Step 2: Find Thevenin's Resistance (R_th)
- Deactivate the independent source (replace the 12 V voltage source with a short circuit).
- Look back into the open terminals A and B.
- R1 and R2 are now in parallel, and this combination is in series with R3.
- R_th = R3 + (R1 * R2) / (R1 + R2)
- R_th = 1 + (2 * 2) / (2 + 2)
- R_th = 1 + 1 = 2 Ω
Step 3: Draw Thevenin's Equivalent Circuit and Calculate Load Current (I_L)
The simplified circuit consists of a voltage source Vth = 6 V in series with Rth = 2 Ω connected to the load R_L = 3 Ω.
`` +----- [ Rth = 2 ohms ] -----o A | | ( Vth = 6 V ) [ R_L = 3 ohms ] | | +-----------------------------o B ``
The load current is calculated as:
- IL = Vth / (Rth + RL)
- I_L = 6 V / (2 Ω + 3 Ω)
- I_L = 6 / 5
- I_L = 1.2 A
(Note: In the actual exam, replace these steps with the exact resistor and source values given in your question paper diagram.)
Frequently Asked Questions
What are the advantages of Nodal Analysis over Mesh Analysis?
Nodal analysis uses Kirchhoff's Current Law (KCL) and is applicable to all circuits, including non-planar ones. Mesh analysis is strictly limited to planar circuits. Additionally, when a circuit contains many ideal voltage sources connected to the reference node, nodal analysis significantly reduces the number of active node equations.
Why is a single-phase induction motor not self-starting?
According to the double revolving field theory, a single-phase alternating magnetic field is composed of two fields of equal strength rotating in opposite directions. At start, these fields produce equal and opposite torques, resulting in a net starting torque of zero.
Why is the power factor low for inductive loads?
Inductive loads (like motors and transformers) require reactive power to establish their magnetic fields. This causes the alternating current to lag behind the applied voltage, leading to a phase angle between them and thus lowering the cosine of the angle, which is the power factor.