Study Vault
All PostsFlashcardsResourcesAI ChatBlog
  1. Home
  2. /↳All Posts
  3. /↳Physics
  4. /↳Electric Circuits
Study VaultStudy Vault

Free, comprehensive study notes for CSEC students.

matthewlloydw@gmail.com

Navigate

  • Home
  • All Posts
  • Flashcards
  • Resources
  • AI Chat

Community

  • Contributors
  • Changelog
  • Suggest a Feature
  • My Suggestions
  • Bookmarks

Mathematics and Science

  • Mathematics
  • Additional Mathematics
  • Biology
  • Chemistry
  • Physics

Arts and Humanities

  • Caribbean History
  • Geography

Business and Human Development Studies

  • Principles of Accounts
  • Principles of Business
  • Economics

Modern Languages

  • English A (Language)
  • English B (Literature)
  • French
  • Spanish

Technical Studies and Creative Arts

  • Electrical & Electronic Technology
  • Information Technology

© 2026 Matthew Williams. Made with other contributors for all.

Physics

Electric Circuits

PDF
Matthew Williams
|May 20, 2026|5 min read
AmmeterCSEC PhysicsElectric CircuitsPaper 01Paper 02ParallelResistanceSection DSeriesVoltmeter

Series and parallel circuits, equivalent resistance formulas, ammeter and voltmeter placement, circuit analysis, and cells (primary versus secondary).

Circuit Symbols and Diagrams

Standard circuit diagrams use internationally recognised symbols. Key components and their symbols:

ComponentSymbol description
CellLong line (positive) + short line (negative)
BatteryMultiple cell symbols in series
SwitchGap that can be bridged
ResistorRectangle
Variable resistorRectangle with diagonal arrow
LampCircle with cross
AmmeterCircle labelled A
VoltmeterCircle labelled V
FuseRectangle with line through it
DiodeTriangle pointing to vertical line

Series Circuits

In a series circuit, components are connected end-to-end in a single loop:

  • The same current flows through every component.
  • The total p.d. of the supply equals the sum of the p.d.s across each component.
  • The equivalent (total) resistance is the sum of all resistances:

Rs=R1+R2+R3+…R_s = R_1 + R_2 + R_3 + \ldotsRs​=R1​+R2​+R3​+…

Removing or breaking any component breaks the entire circuit.

Series circuit diagram: a 6 V battery and switch connected in series with an ammeter (A) and three resistors R1 (2 ohm), R2 (5 ohm), and R3 (10 ohm) in a single loop; a voltmeter (V) is connected in parallel across R2
Series circuit: the ammeter sits in the main loop (same current everywhere); the voltmeter bridges across R2 only.

Parallel Circuits

In a parallel circuit, components are connected across common junction points (they share the same two nodes):

  • The p.d. across each branch is the same (equal to the supply p.d.).
  • The total current from the supply equals the sum of currents through each branch.
  • The equivalent resistance satisfies:

1Rp=1R1+1R2+1R3+…\frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \ldotsRp​1​=R1​1​+R2​1​+R3​1​+…

The equivalent resistance of a parallel combination is always less than the smallest individual resistance. Adding more parallel branches reduces the overall resistance.

Parallel circuit diagram: a 6 V battery with an ammeter (A) in the main line connects to two parallel branches, R1 (2 ohm) on top and R2 (5 ohm) below; a voltmeter (V) is connected across both branches
Parallel circuit: the ammeter measures total current from the supply; the voltmeter reads the common p.d. across both branches.

Measuring Current and Voltage

Ammeters measure current and are connected in series with the component being measured (so the same current flows through both).

Voltmeters measure p.d. and are connected in parallel across the component (so they share the same two nodes). A voltmeter must have very high resistance so it does not divert significant current.

Example/Series and parallel resistances (2019 Paper 02, Q5)

Three resistors of 2 Ω, 5 Ω, and 10 Ω are connected first in series, then in parallel to a 6 V supply.

Series equivalent resistance:

Rs=2+5+10=17ΩR_s = 2 + 5 + 10 = 17 \text{Ω}Rs​=2+5+10=17Ω

Parallel equivalent resistance:

1Rp=12+15+110=510+210+110=810\frac{1}{R_p} = \frac{1}{2} + \frac{1}{5} + \frac{1}{10} = \frac{5}{10} + \frac{2}{10} + \frac{1}{10} = \frac{8}{10}Rp​1​=21​+51​+101​=105​+102​+101​=108​

Rp=108=1.25ΩR_p = \frac{10}{8} = 1.25 \text{Ω}Rp​=810​=1.25Ω

Total current from 6 V supply in parallel circuit:

I=VRp=61.25=4.8AI = \frac{V}{R_p} = \frac{6}{1.25} = 4.8 \text{A}I=Rp​V​=1.256​=4.8A

Cells: Primary and Secondary

TypeDescriptionExamples
Primary cellCannot be recharged, chemical energy converts to electrical energy until exhaustedZinc-carbon, alkaline batteries
Secondary cellCan be recharged by passing current through it in reverseLead-acid (car battery), lithium-ion (phones)

Cells connected in series add their EMFs. Cells connected in parallel keep the same EMF but can supply more current (longer life).

Exam Tip

For parallel resistance calculations, find 1/Rp1/R_p1/Rp​ first by adding the reciprocals, then take the reciprocal of the total. A common error is forgetting to take the final reciprocal.

When two resistors are in parallel, the shortcut formula is: Rp=R1R2R1+R2R_p = \frac{R_1 R_2}{R_1 + R_2}Rp​=R1​+R2​R1​R2​​.

An ammeter goes in series; a voltmeter goes in parallel. Getting this wrong in a diagram loses marks.

Previous in syllabus order
Current Electricity
Next in syllabus order
Electrical Power and Energy