Principles of Electrical Engineering and DC Circuit Analysis

Course Overview: Principles of Electrical Engineering and DC Circuits

  • Course Code: BAEEE101
  • Department: School of Electrical Engineering (SELECT) at Vellore Institute of Technology (VIT).

Module 1: Principles of Electrical Engineering: Circuits and Power Conversion Equipment

  • Topics Covered:
    • Electric circuit components.
    • Mesh current analysis and Node voltage analysis.
    • Thevenin's and Superposition theorems.
    • Single-phase AC circuits: RL, RC, RLC.
    • Power and Energy Calculations and Power Factor.
    • Basics of Electrical Safety and Earthing.
    • Introduction to electromechanical energy conversion.
    • Operation of Electrical Machines: DC Motor, Induction motors, BLDC Motor, and single-phase Transformers.
    • Concepts of Power Electronics and Industrial Applications of Electrical Drives (Qualitative Analysis).

Module 2: Foundations of Electronics and Communication Systems: Devices, Circuits, and Systems

  • Topics Covered:
    • Characteristics of PN Junction Diodes, Zener Diodes, BJT, and MOSFET.
    • Rectifiers and Voltage Regulators.
    • Introduction to Operational Amplifiers.
    • Electromagnetic Spectrum and Elements of Communication Systems.
    • Overview of cellular communication.
    • Fundamentals of Satellite Communication and Radar.

Advantages of Electricity in Daily Life

  • Why use Electricity?
    • Possibility of bulk production and transportability over long distances.
    • Operation is silent.
    • Ease of control.
    • Transfer is very fast.
    • Easily convertible to other forms of energy.
    • Possibility of storage.

Fundamental Electrical Quantities

  • Electric Charge (QQ or qq):
    • A property of subatomic particles like protons and electrons.
    • Measured in Coulombs (CC).
    • It forms the basis for electricity and explains the electrical behavior of materials.
    • It is the most elementary quantity in an electric circuit.
  • Electric Current (II or ii):
    • Defined as the directed flow of electric charge under the influence of an electric field.
  • Voltage (VV):
    • Also known as potential difference.
    • Defined as the electric pressure that makes charges flow in a conductor.
    • Technically, the work or energy required to move a unit charge from one point to another.
  • Electric Power (PP):
    • The time rate of expanding or absorbing energy in a circuit.
    • Equivalently, the rate of doing work in an electric circuit.

Classification of Electrical Networks

  • Electrical Network: An interconnection of electrical elements such as resistors (RR), inductors (LL), capacitors (CC), and sources.
  • Electric Circuit: An interconnection of elements that provides at least one closed path, allowing a return path for current. All circuits are networks, but not all networks are circuits.
  • Importance of Classification:
    • Simplifies analysis and problem-solving.
    • Assists in choosing appropriate methods like KCL/KVL, Thevenin/Norton, or Superposition.
    • Essential for modeling real systems in power, electronics, and control.
  • Categorization:
    • Active vs. Passive:
      • Active: Contains energy sources (independent or dependent) and can deliver power. Examples include batteries with resistors, transistors, and Operational Amplifiers.
      • Passive: Contains only RR, LL, and CC elements. These absorb or store energy but do not generate it. Example: an RLC network without sources.
    • Linear vs. Non-linear:
      • Linear: The Voltage-Current (VIV-I) relation is linear, and parameters remain constant regardless of applied voltage or current. Follows the principles of superposition and homogeneity. Examples: Ideal resistors, inductors, and capacitors.
      • Non-linear: The VIV-I relation is not linear; parameters vary with voltage, current, or temperature. Examples: Diodes, transistors, and filament lamps.
    • Bilateral vs. Unilateral:
      • Bilateral: Behavior and characteristics (impedance) remain the same regardless of the direction of current or voltage. Examples: RR, LL, and CC elements.
      • Unilateral: Behavior depends on the direction of current or voltage. Example: A diode circuit which conducts primarily in one direction.
    • Time-invariant vs. Time-variant:
      • Time-invariant: Element values do not change over time, making analysis easier.
      • Time-variant: Element values change over time. Examples: Resistance changing with a sensor (R(t)R(t)), switching circuits, or variable capacitors.

Fundamental Circuit Laws

  • Ohm's Law: States that the voltage VV across a resistor is directly proportional to the current II flowing through it.
    • Equation: V=IRV = IR
  • Kirchhoff’s Current Law (KCL): The algebraic sum of currents going away from or coming towards a node is zero.
    • Convention: Current coming toward a node is considered positive, and current leaving is negative (or vice-versa).
  • Kirchhoff’s Voltage Law (KVL): The algebraic sum of voltages equals zero for any closed path (loop) in an electrical circuit.

Circuit Topology Definitions

  • Node: An equipotential surface where two or more circuit elements are joined. Example nodes listed in a diagram: {1,2,3,4}\{1, 2, 3, 4\}.
  • Junction: A point in a network where three or more circuit elements are joined. Example junctions: {2,4}\{2, 4\}.
  • Loop: Any closed path of a network. Example loops: Loop 1 {1,2,4,1}\{1, 2, 4, 1\}, Loop 2 {2,3,4,2}\{2, 3, 4, 2\}, Loop 3 {1,2,3,4,1}\{1, 2, 3, 4, 1\}.
  • Mesh: The most elementary form of a loop; it cannot be divided into any other smaller loops. Example meshes: Mesh 1 {1,2,4,1}\{1, 2, 4, 1\}, Mesh 2 {2,3,4,2}\{2, 3, 4, 2\}.

Electrical Sources

  • Independent Sources: Provide a specified voltage or current that is completely independent of other circuit elements.
    • Representations: Time-varying voltage source symbols and continuous DC voltage source symbols.
  • Dependent (Controlled) Sources: The value depends on another voltage or current elsewhere in the circuit. These are used to model transistors, op-amps, and amplifiers.
Types of Dependent Sources
  1. VCVS (Voltage Controlled Voltage Source):
    • Output: Voltage Source.
    • Controlled by: Voltage.
    • Equation: V1=Av1V_1 = A v_1
    • Parameter: A=Voltage gainA = \text{Voltage gain} (unitless).
  2. VCCS (Voltage Controlled Current Source):
    • Output: Current Source.
    • Controlled by: Voltage.
    • Equation: i1=gv1i_1 = g v_1
    • Parameter: g=transconductanceg = \text{transconductance} (Unit: Siemens (SS) or Amperes/Volt (A/VA/V)).
  3. CCVS (Current Controlled Voltage Source):
    • Output: Voltage Source.
    • Controlled by: Current.
    • Equation: v0=ri1v_0 = r i_1
    • Parameter: r=trans-resistancer = \text{trans-resistance} (Unit: Ohms (Ω\Omega) or Volts/Ampere (V/AV/A)).
  4. CCCS (Current Controlled Current Source):
    • Output: Current Source.
    • Controlled by: Current.
    • Equation: ix=βi1i_x = \beta i_1
    • Parameter: β=Current Gain\beta = \text{Current Gain} (unitless).

Resistance Network Simplification

  • Series Resistance: The equivalent resistance (ReqR_{eq}) is the sum of individual resistances.
    • Req=R1+R2++RnR_{eq} = R_1 + R_2 + \dots + R_n
  • Parallel Resistance: The reciprocal of equivalent resistance is the sum of the reciprocals of individual resistances.
    • 1Req=1R1+1R2++1Rn\frac{1}{R_{eq}} = \frac{1}{R_1} + \frac{1}{R_2} + \dots + \frac{1}{R_n}
  • Equivalent Resistance Concept: A single resistance that can replace an entire circuit or network between two specific terminals.
Delta-Star (ΔY\Delta-Y) Transformations
  • Delta (Δ) to Star (Y) Conversion:

    • Used when three resistors (RABR_{AB}, RBCR_{BC}, RCAR_{CA}) form a closed mesh.
    • Formulas for star arms (RA,RB,RCR_A, R_B, R_C):
      • RA=RABRCARAB+RBC+RCAR_A = \frac{R_{AB} R_{CA}}{R_{AB} + R_{BC} + R_{CA}}
      • RB=RBCRABRAB+RBC+RCAR_B = \frac{R_{BC} R_{AB}}{R_{AB} + R_{BC} + R_{CA}}
      • RC=RCARBCRAB+RBC+RCAR_C = \frac{R_{CA} R_{BC}}{R_{AB} + R_{BC} + R_{CA}}
    • Memory Rule: Any arm of a star connection is equal to the product of two adjacent Δ arms divided by the sum of all Δ arms.
  • Star (Y) to Delta (Δ) Conversion:

    • Converts resistors RAR_A, RBR_B, and RCR_C connected to a common neutral node into a closed mesh.
    • Formulas for delta arms:
      • RAB=RA+RB+RARBRCR_{AB} = R_A + R_B + \frac{R_A R_B}{R_C}
      • RBC=RB+RC+RBRCRAR_{BC} = R_B + R_C + \frac{R_B R_C}{R_A}
      • RCA=RC+RA+RCRARBR_{CA} = R_C + R_A + \frac{R_C R_A}{R_B}
Numerical Examples for Resistance
  • Y to Δ conversion example:
    • Input Star: R1=7.5ΩR_1 = 7.5\,\Omega, R2=5ΩR_2 = 5\,\Omega, R3=3ΩR_3 = 3\,\Omega.
    • Calculations:
      • Ra=7.5+5+7.5×53=25ΩR_a = 7.5 + 5 + \frac{7.5 \times 5}{3} = 25\,\Omega
      • Rb=7.5+3+7.5×35=15ΩR_b = 7.5 + 3 + \frac{7.5 \times 3}{5} = 15\,\Omega
      • Rc=5+3+5×37.5=10ΩR_c = 5 + 3 + \frac{5 \times 3}{7.5} = 10\,\Omega
  • Δ to Y conversion example:
    • Input Delta: Ra=15ΩR_a = 15\,\Omega, Rb=10ΩR_b = 10\,\Omega, Rc=25ΩR_c = 25\,\Omega.
    • Calculations:
      • R1=10×2550=5ΩR_1 = \frac{10 \times 25}{50} = 5\,\Omega
      • R2=25×1550=7.5ΩR_2 = \frac{25 \times 15}{50} = 7.5\,\Omega
      • R3=15×1050=3ΩR_3 = \frac{15 \times 10}{50} = 3\,\Omega

Voltage and Current Division Rules

  • Voltage Division (Series Circuits):

    • The total applied voltage is distributed among resistors.
    • For two resistors R1R_1 and R2R_2 in series with voltage VV:
      • VR1=V×R1R1+R2V_{R1} = V \times \frac{R_1}{R_1 + R_2}
      • VR2=V×R2R1+R2V_{R2} = V \times \frac{R_2}{R_1 + R_2}
    • Example with 3 resistors (10Ω10\,\Omega, 20Ω20\,\Omega, 30Ω30\,\Omega) and 60V60\,V source:
      • V10Ω=60×1010+20+30=10VV_{10\Omega} = 60 \times \frac{10}{10 + 20 + 30} = 10\,V
      • V20Ω=60×2010+20+30=20VV_{20\Omega} = 60 \times \frac{20}{10 + 20 + 30} = 20\,V
      • V30Ω=60×3010+20+30=30VV_{30\Omega} = 60 \times \frac{30}{10 + 20 + 30} = 30\,V
  • Current Division (Parallel Circuits):

    • Total current (ITI_T) splits between parallel branches.
    • For two resistors R1R_1 and R2R_2 in parallel:
      • I1=IT×R2R1+R2I_1 = I_T \times \frac{R_2}{R_1 + R_2}
      • I2=IT×R1R1+R2I_2 = I_T \times \frac{R_1}{R_1 + R_2}
    • Relationship: IT=I1+I2I_T = I_1 + I_2
    • Example with R1=10ΩR_1=10\,\Omega, R2=20ΩR_2=20\,\Omega, and V=50VV=50\,V:
      • Req=10×2010+20=6.67ΩR_{eq} = \frac{10 \times 20}{10 + 20} = 6.67\,\Omega
      • IT=506.67=7.5AI_T = \frac{50}{6.67} = 7.5\,A
      • I1=7.5×2030=5AI_1 = 7.5 \times \frac{20}{30} = 5\,A
      • I2=2.5AI_2 = 2.5\,A

Source Transformation

  • Voltage to Current Source:
    • A voltage source VV with series resistance RseR_{se} converts to a current source I=VRseI = \frac{V}{R_{se}} with parallel internal resistance equal to RseR_{se}.
  • Current to Voltage Source:
    • A current source II with parallel resistance RshR_{sh} converts to a voltage source V=I×RshV = I \times R_{sh} with series internal resistance equal to RshR_{sh}.
  • Polarity Conventions:
    • The direction of equivalent current is from the negative to the positive terminal internal to the source.
    • When converting current to voltage, the positive terminal is at the head of the arrow and the negative at the tail.

Nodal Analysis

  • Definition: Nodal analysis focuses on identifying voltages at nodes where three or more branches are connected.
  • Procedure:
    1. Identify the total number of nodes (NN). The number of equations required is N1N-1.
    2. Mark branch currents.
    3. Write node equations using Kirchhoff’s Current Law (KCL).
    4. Arrange equations in matrix form.
    5. Solve the system using Cramer’s rule.
Nodal Analysis Example
  • Setup: 2-node circuit (N=2N=2, so 1 equation). Source voltage 10V10\,V, branches with resistors 4Ω4\,\Omega, 2Ω2\,\Omega, and 4Ω4\,\Omega.
  • Equation at Node 1:
    • I1=I2+I3I_1 = I_2 + I_3
    • 10V14=V12+V14\frac{10 - V_1}{4} = \frac{V_1}{2} + \frac{V_1}{4}
    • Result: V1=2.5VV_1 = 2.5\,V
  • Currents:
    • I1=102.54=1.875AI_1 = \frac{10 - 2.5}{4} = 1.875\,A
    • I2=2.52=1.25AI_2 = \frac{2.5}{2} = 1.25\,A
    • I3=2.54=0.625AI_3 = \frac{2.5}{4} = 0.625\,A

Mesh Analysis

  • Definition: Mesh analysis involves closed paths that do not contain any other loops within them.
  • Procedure:
    1. Identify the number of meshes.
    2. Mark each mesh current (usually in a clockwise direction).
    3. Apply Kirchhoff’s Voltage Law (KVL) to each mesh to write equations.
    4. Convert the equations into a matrix format.
    5. Use Cramer’s rule to solve for mesh currents.
Mesh Analysis Example
  • Setup: 3-mesh circuit to find power in an 18Ω18\,\Omega resistor.
    • Mesh 1: 12I16I2=12012 I_1 - 6 I_2 = 120
    • Mesh 2: 6I1+34.5I224I3=0-6 I_1 + 34.5 I_2 - 24 I_3 = 0
    • Mesh 3: 21I2+42I3=0-21 I_2 + 42 I_3 = 0
  • Solving:
    • Determinant (\Delta): 1058410584
    • Determinant for Mesh 3 (Δ3\Delta_3): 1512015120
    • I3=1512010584=1.428AI_3 = \frac{15120}{10584} = 1.428\,A
  • Power Calculation (P=I2RP = I^2 R):
    • P=1.42822×18=36.7WP = 1.4282^2 \times 18 = 36.7\,W

Network Theorems

  • Superposition Theorem:
    • In a linear network with two or more sources, the response in any element is the algebraic sum of responses caused by each source acting alone.
    • To act "alone," other ideal voltage sources are replaced by short circuits, and ideal current sources are replaced by open circuits.
    • Applicability: Only valid for linear systems. It does not apply to power calculations because power is a nonlinear function (PI2P \propto I^2).
  • Thevenin’s Theorem:
    • Any two-terminal linear network containing voltage/current sources and resistances can be replaced by an equivalent circuit.
    • The equivalent circuit consists of a single voltage source (VthV_{th}) in series with a single resistance (RthR_{th}).
    • VthV_{th} is the open-circuit voltage across the terminals.
    • RthR_{th} is the equivalent resistance measured between the terminals when all internal energy sources are replaced by their internal resistances (voltage sources shorted, current sources opened).