Essential idea: One of the earliest uses for electricity was to produce light and heat. This technology continues to have a major impact on the lives of people around the world.
Understandings: Circuit diagrams; Kirchhoff's circuit laws; Resistance expressed as R = V/I
Applications and skills: Drawing and interpreting circuit diagrams; Solving problems involving potential difference, current, charge, Kirchhoff’s circuit laws, power, resistance and resistivity; Investigating combinations of resistors in parallel and series circuits
Data booklet equations: Rtotal = R1 + R2 + …; 1/Rtotal = 1/R1 + 1/R2 + …
To solve a circuit is a lot like solving an equation. You have a situation with some knowns and some unknowns, and you must use your knowledge of physics to know the unknowns and find out everything about a circuit. The concept of solving circuits is also known as circuit analysis or (in advanced forms) network analysis.
For a circuit to be solved you should know:
The resistance of any part of a circuit (any component or combination of components)
The current at any point in a circuit
The potential difference between any two points in a circuit
The tools you have include:
V = IR
P = VI (and P = I2R and P = V2/R)
The rules for combining components
Kirchhoff's laws of circuit analysis (current law and voltage law) <--- see section 5.2e.
An important distinction in circuit analysis is the difference between series and parallel. When components are arranged in series they follow each other and the current (the charge carriers) must pass through both. When components are arranged in parallel the current can pass through them simultaneously - charge carriers pass through one component OR the other. Parallel circuits include junctions - places the current will separate and rejoin. There are no junctions in the series part of a circuit.
The three minimum divisions of a working circuit are the supply, the cables and the load (control elements, such as switches, and meters, such as a voltmeter, are additional elements). In an ideal circuit the cables have no resistance. The supply may have a resistance (internal resistance, which we will look at in more detail later) and the load must have a resistance - unless energy transformation is occurring you do not have a useful circuit.
There are many components that can form part of the load, but in many cases we do not need to know the details when solving a circuit. Frequently, we can consider all components of the load in terms of their resistance only - and think of them as resistors.
A common first step in solving circuits is to determine the total resistance of a circuit. In order to do this, you must be able to determine the combined resistance of more than one resistor (or other component with a resistance). This may take several steps before you have the final value.
Uses the ANSI symbols for resistors, but otherwise a good summary
Mentions Kirchhoff but not in the detail we will go into later. Introduces a useful cheat for two (only two) parallel resistors.
Oxford Physics: pages 204 - 207, good worked examples
Hamper HL (2014): pages 229- 232, also good examples
pages 248 - 254