Theory — Voltage in Series and Parallel Circuits
What is Voltage?
Voltage (V) is the electrical potential difference between two points in a circuit — the "push" that drives current through a resistor. It is measured in Volts (V) using a voltmeter connected in parallel across a component.
Series Circuit
Components are connected end-to-end in a single path. The same current flows through every resistor. The total voltage from the battery is shared (divided) among all resistors in proportion to their resistance.
I = same everywhere
R_total = R₁ + R₂ + R₃ + ...
Parallel Circuit
Components are connected side-by-side, sharing the same two nodes. Every branch has the same voltage across it — equal to the battery voltage. Current divides among branches inversely proportional to resistance.
I_total = I₁ + I₂ + I₃ + ...
1/R_total = 1/R₁ + 1/R₂ + ...
Ohm's Law — The Foundation
I = V / R
R = V / I
Kirchhoff's Voltage Law (KVL)
The sum of all voltage drops around any closed loop in a circuit equals the source voltage. This is the theoretical basis for why voltages add up in series.
V_R1 + V_R2 + V_Rh = V_battery
Instructions — Running the Virtual Experiment
This lab has two circuit types — Parallel (Section A) and Series (Section B). Work through each section in order a, b, c, d as shown on the simulation tabs.
Section A — Parallel Circuit
Section B — Series Circuit
Simulation — Circuit Voltage Measurements
Battery
Resistors
Voltmeter Location
Battery
Fixed Resistors
Variable Resistor Rh
Data Table
| Measurement | Circuit | R1 (Ω) | R2 (Ω) | V_battery (V) | V_R1 (V) | V_R2 (V) | V_Rh (V) |
|---|---|---|---|---|---|---|---|
| Step a-c | Parallel | N/A | |||||
| Steps a-c | Series | N/A | |||||
| Step d (with Rh) | Series+Rh |
Team Questions
Example Lab Report
Voltage in Circuits
Physics SC-172 | Section: [Your Section] | Date: [Date]
Lab Members: [Names of all members present]
Purpose
To measure voltage in series and parallel circuits and determine the relationships between individual voltages, total battery voltage, and component resistance values.
Theory
Ohm's Law states V = IR. In a parallel circuit, all branches share the same voltage equal to the battery voltage. In a series circuit, voltage divides among components in proportion to resistance, and the sum of all voltage drops equals the source voltage (Kirchhoff's Voltage Law).
Data Table
| Step | Circuit | R1 | R2 | V_battery | V_R1 | V_R2 | V_Rh |
|---|---|---|---|---|---|---|---|
| a–c | Parallel | 300 Ω | 500 Ω | 9.00 V | 9.00 V | 9.00 V | — |
| a–c | Series | 300 Ω | 500 Ω | 9.00 V | 3.38 V | 5.63 V | — |
| d | Series+Rh | 300 Ω | 500 Ω | 9.00 V | 2.70 V | 4.50 V | 1.80 V |
Sample Calculations — Series Circuit (R1=300Ω, R2=500Ω, V=9V)
Total resistance: R_total = 300 + 500 = 800 Ω
Current: I = V/R = 9.00/800 = 0.01125 A = 11.25 mA
V_R1: V = IR = 0.01125 × 300 = 3.375 V ≈ 3.38 V
V_R2: V = IR = 0.01125 × 500 = 5.625 V ≈ 5.63 V
KVL check: 3.38 + 5.63 = 9.01 V ≈ 9.00 V ✓
Voltage ratio: V_R1/V_R2 = 3.38/5.63 = 0.600 R1/R2 = 300/500 = 0.600 ✓ (ratios equal)
Discussion
Q1 — Parallel voltage: The voltmeter read exactly 9.00 V across R1 — identical to battery voltage. In a parallel circuit, all branches connect directly between the same two nodes as the battery. Therefore every branch must have the same potential difference as the source.
Q3 — Series voltage and resistance: V_R1/V_R2 = 3.38/5.63 = 0.600 and R1/R2 = 300/500 = 0.600. The ratios are equal, confirming that in a series circuit, voltage across each resistor is proportional to its resistance: V_n = V_total × (R_n / R_total).
Q5 — Adding Rh: When Rh (200Ω) was added, V_R1 dropped from 3.38 V to 2.70 V and V_R2 dropped from 5.63 V to 4.50 V. This demonstrates Kirchhoff's Voltage Law — the total voltage is still 9.00 V, but it is now shared among three resistors instead of two. Adding resistance reduces current, which reduces the voltage across each original resistor.
Conclusion
The experiment confirmed the fundamental rules of series and parallel circuits. In parallel: all branch voltages equal the source voltage. In series: voltages divide proportionally to resistance and sum to the source voltage. Kirchhoff's Voltage Law was verified experimentally in all configurations.