Comprehensive Circuit Analysis Study Guide

Fundamental DC Circuit Rules and Node Analysis

  • Node Labeling Procedure:

    • Node labeling is the mandatory first step when analyzing any electric circuit.
    • A node is defined as the point of intersection or connection boundary between two or more circuit elements.
    • Example Node Identification: In a single-loop series circuit connected to a DC power supply, Node 1 is the boundary between the power supply terminal and one end of resistor R1R_1; Node 2 is the connection point between R1R_1 and R2R_2; Node 3 is the connection point between R2R_2 and R3R_3.
    • Visual arrangement can be deceptive: elements that appear visually parallel in a schematic drawing may actually be connected sequentially in series if each element shares only one single node with an adjacent element.
  • Series Circuit Properties:

    • Current Consistency: Components connected in series share the exact same nodes sequentially, meaning the same total current (ItotalI_{\text{total}}) flows continuously through every series element.
    • Total Resistance Formula:Rtotal=R1+R2+R3+⋯+RnR_{\text{total}} = R_1 + R_2 + R_3 + \dots + R_n
    • Voltage Drop Across a Resistor (Ohm's Law):VRn=Itotal×RnV_{R_n} = I_{\text{total}} \times R_n
    • Kirchhoff's Voltage Law (KVL) Constraint: The sum of all individual resistor voltage drops across a closed series loop must equal the source voltage (VsourceV_{\text{source}}). For a 10 V10\,V source:         VR1+VR2+VR3=10 VV_{R_1} + V_{R_2} + V_{R_3} = 10\,V
  • Mandatory Engineering Metric Prefixes:

    • Prefix values are required knowledge for all calculations and are not provided on formula reference sheets:
      • Kilo (kk) = 10310^3 (1 kΩ=1000 Ω1\,k\Omega = 1000\,\Omega)
      • Milli (mm) = 10−310^{-3} (1 mA=1×10−3 A1\,mA = 1 \times 10^{-3}\,A)

Parallel DC Circuits Analysis

  • Parallel Circuit Rules and Node Structure:

    • In a purely parallel circuit, all parallel branches are connected directly between the same two primary nodes.
    • Branch Voltage: The voltage drop across every individual branch in a parallel circuit is constant and directly equals the total supply voltage (Vbranch=VsourceV_{\text{branch}} = V_{\text{source}}).
  • Ohm's Law Applied to Individual Parallel Branches:

    • For a parallel circuit powered by a 20 V20\,V DC source connected across three parallel resistors (R1=1 kΩR_1 = 1\,k\Omega, R2=2 kΩR_2 = 2\,k\Omega, R3=4 kΩR_3 = 4\,k\Omega):
      • Branch 1 Current (I1I_1):             I1=VsourceR1=20 V1 kΩ=20 mAI_1 = \frac{V_{\text{source}}}{R_1} = \frac{20\,V}{1\,k\Omega} = 20\,mA
      • Branch 2 Current (I2I_2):             I2=VsourceR2=20 V2 kΩ=10 mAI_2 = \frac{V_{\text{source}}}{R_2} = \frac{20\,V}{2\,k\Omega} = 10\,mA
      • Branch 3 Current (I3I_3):             I3=VsourceR3=20 V4 kΩ=5 mAI_3 = \frac{V_{\text{source}}}{R_3} = \frac{20\,V}{4\,k\Omega} = 5\,mA
  • Total Parallel Current Calculation:

    • By Kirchhoff's Current Law (KCL), the total current entering the parallel network equals the sum of all individual branch currents:         Itotal=I1+I2+I3I_{\text{total}} = I_1 + I_2 + I_3Itotal=20 mA+10 mA+5 mA=35 mAI_{\text{total}} = 20\,mA + 10\,mA + 5\,mA = 35\,mA
  • Equivalent Parallel Resistance (RtotalR_{\text{total}}) Calculations:

    • Reciprocal Method using Least Common Multiple (LCM):1Rtotal=1R1+1R2+1R3\frac{1}{R_{\text{total}}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3}1Rtotal=11000+12000+14000\frac{1}{R_{\text{total}}} = \frac{1}{1000} + \frac{1}{2000} + \frac{1}{4000}
    • Finding the LCM (40004000):         1Rtotal=4+2+14000=74000\frac{1}{R_{\text{total}}} = \frac{4 + 2 + 1}{4000} = \frac{7}{4000}Rtotal=40007 ΩR_{\text{total}} = \frac{4000}{7}\,\Omega
    • Decimal Precision Requirement: Convert fractions to standard decimal format rounded to exactly two decimal places:         Rtotal≈571.43 ΩR_{\text{total}} \approx 571.43\,\Omega

Series-Parallel Combination Circuit Analysis

  • Circuit Parameters and Specifications:

    • Source Voltage (VsV_s) = 10 V10\,V
    • Resistor Values:
      • R1=1 kΩR_1 = 1\,k\Omega (1000 Ω1000\,\Omega)
      • R2=500 ΩR_2 = 500\,\Omega
      • R3=2 kΩR_3 = 2\,k\Omega (2000 Ω2000\,\Omega)
      • R4=1 kΩR_4 = 1\,k\Omega (1000 Ω1000\,\Omega)
      • R5=2 kΩR_5 = 2\,k\Omega (2000 Ω2000\,\Omega)
      • R6=2 kΩR_6 = 2\,k\Omega (2000 Ω2000\,\Omega)
  • Step 1: Complete Node Labeling:

    • Label all unique nodes in the circuit (5 total nodes):
      • Node 1: Positive terminal of VsV_s to R1R_1.
      • Node 2: Junction of R1R_1, R3R_3, and R4R_4
      • Node 3: Junction of R4R_4, R5R_5, and R6R_6
      • Node 4: Common return rail connecting R3R_3, R5R_5, and R6R_6
      • Node 5: Return from R2R_2 to negative terminal of VsV_s
  • Step 2: Circuit Reduction from Right-Hand Side (RHS):

    • Always reduce complex networks from the side furthest from the source (the right-hand side) back toward the power source to reduce the network to a single equivalent resistance across one voltage source.
    • First Reduction (Req1R_{\text{eq1}}): Resistors R5R_5 and R6R_6 are in parallel between Nodes 3 and 4.         Req1=R5∥R6=R5×R6R5+R6R_{\text{eq1}} = R_5 \parallel R_6 = \frac{R_5 \times R_6}{R_5 + R_6}Req1=2000×20002000+2000=40000004000=1000 Ω=1 kΩR_{\text{eq1}} = \frac{2000 \times 2000}{2000 + 2000} = \frac{4000000}{4000} = 1000\,\Omega = 1\,k\Omega
    • Second Reduction (Req2R_{\text{eq2}}): Req1R_{\text{eq1}} (located between Nodes 3 and 4) is in series with R4R_4.         Req2=Req1+R4R_{\text{eq2}} = R_{\text{eq1}} + R_4Req2=1 kΩ+1 kΩ=2 kΩ=2000 ΩR_{\text{eq2}} = 1\,k\Omega + 1\,k\Omega = 2\,k\Omega = 2000\,\Omega
    • Third Reduction (Req3R_{\text{eq3}}): Req2R_{\text{eq2}} (between Nodes 2 and 4) is in parallel with R3R_3 (between Nodes 2 and 4).         Req3=R3∥Req2=2000×20002000+2000=1000 Ω=1 kΩR_{\text{eq3}} = R_3 \parallel R_{\text{eq2}} = \frac{2000 \times 2000}{2000 + 2000} = 1000\,\Omega = 1\,k\Omega
    • Final Resistance (RtotalR_{\text{total}}): R1R_1, Req3R_{\text{eq3}}, and R2R_2 are all connected in series across the supply terminals.         Rtotal=R1+Req3+R2R_{\text{total}} = R_1 + R_{\text{eq3}} + R_2Rtotal=1 kΩ+1 kΩ+0.5 kΩ=2.5 kΩ=2500 ΩR_{\text{total}} = 1\,k\Omega + 1\,k\Omega + 0.5\,k\Omega = 2.5\,k\Omega = 2500\,\Omega
  • Step 3: Calculating Total Source Current (ItotalI_{\text{total}}):Itotal=VsRtotal=10 V2500 Ω=0.004 A=4 mAI_{\text{total}} = \frac{V_s}{R_{\text{total}}} = \frac{10\,V}{2500\,\Omega} = 0.004\,A = 4\,mA

Voltage Drops and Branch Currents in Combination Circuits

  • Tracing Total Current Flow:

    • By conventional current flow analysis, ItotalI_{\text{total}} (4 mA4\,mA) leaves the source and passes entirely through R1R_1 before reaching Node 2.
    • After passing through the internal network, the total recombined current (4 mA4\,mA) passes entirely through R2R_2 before returning to the source.
  • Outer Series Resistor Voltage Drops:

    • Voltage drop across R1R_1 (VR1V_{R1}):         VR1=Itotal×R1=4 mA×1 kΩ=4 VV_{R1} = I_{\text{total}} \times R_1 = 4\,mA \times 1\,k\Omega = 4\,V
    • Voltage drop across R2R_2 (VR2V_{R2}):         VR2=Itotal×R2=4 mA×0.5 kΩ=2 VV_{R2} = I_{\text{total}} \times R_2 = 4\,mA \times 0.5\,k\Omega = 2\,V
  • Intermediate Loop Voltage Drop Calculation:

    • Applying Kirchhoff's Voltage Law to the main loop containing VsV_s, R1R_1, R3R_3, and R2R_2:         Vs=VR1+VR2+VR3V_s = V_{R1} + V_{R2} + V_{R3}10 V=4 V+2 V+VR310\,V = 4\,V + 2\,V + V_{R3}VR3=10 V−6 V=4 VV_{R3} = 10\,V - 6\,V = 4\,V
    • The voltage drop across R3R_3 (4 V4\,V) acts as a secondary effective source voltage for all remaining parallel downstream network components connected between Nodes 2 and 4.
  • Branch Currents and Downstream Drops:

    • Current through R3R_3 (I1I_1):         I1=VR3R3=4 V2 kΩ=2 mAI_1 = \frac{V_{R3}}{R_3} = \frac{4\,V}{2\,k\Omega} = 2\,mA
    • Current entering the R4R_4 branch (I2I_2):         I2=Itotal−I1=4 mA−2 mA=2 mAI_2 = I_{\text{total}} - I_1 = 4\,mA - 2\,mA = 2\,mA
    • Voltage drop across R4R_4 (VR4V_{R4}):         VR4=I2×R4=2 mA×1 kΩ=2 VV_{R4} = I_2 \times R_4 = 2\,mA \times 1\,k\Omega = 2\,V
    • Voltage drop across R5R_5 (VR5V_{R5}):
      • Remaining voltage across parallel combination R5∥R6R_5 \parallel R_6 is equal to VR3−VR4=4 V−2 V=2 VV_{R3} - V_{R4} = 4\,V - 2\,V = 2\,V
      • Therefore, VR5=2 VV_{R5} = 2\,V

Wheatstone Bridge Circuits

  • Circuit Drawing and Balance Conditions:

    • Students must know how to construct and draw a standard Wheatstone bridge circuit diagram.
    • A Wheatstone bridge is considered balanced when the differential output voltage across the central bridge terminals is zero (Vout=0 VV_{\text{out}} = 0\,V).
    • Balance Ratio Formula:R1R2=R3R4\frac{R_1}{R_2} = \frac{R_3}{R_4}
  • Application Procedures:

    • The formula for output voltage under unbalanced conditions is provided on the exam formula sheet.
    • Given one reference resistor value and the balance condition, solve for unknown branch resistances before substituting parameters into the output voltage equation.

AC Series RC Circuit Analysis

  • Circuit Parameters Given in Problem Statement:

    • AC Source Voltage Amplitude (VsV_s) = 3 V3\,V
    • Frequency (ff) = 1 kHz=1000 Hz1\,kHz = 1000\,Hz
    • Resistance (RR) = 1 kΩ=1000 Ω1\,k\Omega = 1000\,\Omega
    • Capacitance (CC) = 10 μF=10×10−6 F10\,\mu F = 10 \times 10^{-6}\,F
  • **Step-by-Step