Current, Potential Difference and Circuit Analysis

Current, Potential Difference and Circuit Analysis

1 / 41
next
Slide 1: Slide
New lesson editorPhysicsFurther Education (Key Stage 5)

This lesson contains 41 slides, with interactive quizzes and text slides.

time-iconLesson duration is: 50 min
Report this lesson

Items in this lesson

Current, Potential Difference and Circuit Analysis

This item has no instructions

Learning objective

I can analyse series, parallel and potential-divider circuits using current, potential difference and conservation laws.

This item has no instructions

What words do you link with current and potential difference?

Use this to activate prior knowledge and surface misconceptions such as 'current is used up' or 'voltage flows'. Invite students to explain one word they submitted.

Lesson overview

This KS5 physics lesson explores Current, Potential Difference and Circuit Analysis. Students apply conservation laws, resistivity and component characteristics to analyse series, parallel and potential-divider circuits. It is suitable for A level classroom teaching, independent study or exam revision.

This item has no instructions

Current: what is flowing?

Current is the rate of flow of charge.


$ I = \dfrac{Q}{t} $


  • current is measured in amperes, A

  • charge is measured in coulombs, C

  • time is measured in seconds, s

  • 1 A means 1 C of charge passes a point each second

Students often say current is 'used up'. Emphasise that charge is conserved: the current entering a component equals the current leaving it in a steady circuit.

Conventional current and electrons

  • Conventional current is defined as the direction positive charge would move

  • in metal wires, electrons move in the opposite direction

  • circuit diagrams and calculations use conventional current

Useful distinction for A level wording: current direction on diagrams is not the same as electron drift direction in a metal conductor.

Potential difference: energy transfer per coulomb

Potential difference is the energy transferred per unit charge.


$ V = \dfrac{W}{Q} $


  • potential difference is measured in volts, V

  • energy transferred is measured in joules, J

  • 1 V means 1 J of energy transferred for each coulomb of charge

Link this to a battery or supply: the source gives energy to charges, and components transfer that energy to other forms such as thermal energy or light.

Current and potential difference are not the same

  • Current tells us how much charge flows each second

  • Potential difference tells us how much energy each coulomb transfers

  • a circuit can have the same current through several components but different potential differences across them

A common misconception is to treat voltage as something that flows. Clarify that charge flows; potential difference is a measure of energy transfer.

What does a current of 1 A mean?

A

1 C each second

B

1 J each second

C

1 V each coulomb

D

1 Ω each second

Checks the definition I = Q/t. Distractors mix up charge, energy and resistance units.

Complete the summary

In a steady circuit, charge is conserved, so current is not up by a component. Potential difference is the energy transferred per unit , not something that flows around the circuit.

charge
is conserved, so current is not
up by a component. Potential difference is the energy transferred per unit
voltage
split
resistance
current

Targets the opening conceptual distinctions: current as rate of flow of charge, and potential difference as energy transferred per coulomb.

Why is 'current is used up' wrong?

Expected elements: current is conserved at a component in a steady circuit, so the same current enters and leaves; the component transfers energy, so potential difference is linked to energy per coulomb, not loss of charge.

Conservation laws in circuits

Circuit analysis is built on two conservation ideas:


  • Charge is conserved → current into a junction equals current out

  • Energy is conserved → the total potential difference supplied equals the total potential difference across components in a complete loop

  • these rules apply before substituting values into equations

This is the conceptual bridge into series and parallel circuits. Students should see Kirchhoff-style rules as conservation laws, not isolated facts to memorise.

Series circuits

In a series circuit there is one path for charge flow.


  • the current is the same through every component

  • the potential differences add up to the supply potential difference

  • the total resistance is the sum of the resistances

  • adding more components increases total resistance

This item has no instructions

Parallel circuits

In a parallel circuit there are separate branches.


  • the potential difference is the same across each branch

  • the current splits between branches

  • the total current from the source is the sum of the branch currents

  • adding a branch reduces the total resistance

Students often reverse the series/parallel rules. Stress the path idea: one path gives same current; shared branches give same potential difference across each branch.

Using conservation to solve circuits

A reliable approach is:


  1. identify series sections and parallel branches

  2. apply the current rule at junctions

  3. apply the potential difference rule around loops

  4. use $V = IR$ for individual components or sections

  5. check that your answers are physically consistent

The final check matters: branch currents should add correctly, and potential differences should match the supply where expected.

In a parallel circuit, what is the same across each branch?

A

Resistance

B

Current

C

Potential difference

D

Charge flow path

Tests the core series/parallel contrast. Common error is to swap current and potential difference rules.

Complete the method

To analyse a circuit, first identify series sections and parallel . Then apply the current rule at and the potential difference rule around before using V = IR.

To analyse a circuit, first identify series sections and parallel
. Then apply the current rule at
and the potential difference rule around
components
wires
cells
sources

Reinforces the structured method slide and the conservation-law language used in circuit analysis.

Resistance and Ohm's law

For an ohmic conductor at constant temperature:


$ V = IR $


  • resistance is measured in ohms, $\Omega$

  • a larger resistance gives a smaller current for the same potential difference

  • the equation links current, potential difference and resistance during circuit analysis

Remind students that Ohm's law in the strict sense applies when current is directly proportional to potential difference, typically at constant temperature.

What sets the resistance of a wire?

Resistance depends on both geometry and material.


$ R = \rho \dfrac{L}{A} $


  • $\rho$ is the resistivity of the material

  • longer wires have greater resistance

  • larger cross-sectional area gives smaller resistance

  • materials with high resistivity oppose charge flow more strongly

Students may confuse resistance and resistivity. Resistance belongs to a component; resistivity is a material property.

Resistivity in context

  • copper has low resistivity, so it is useful for connecting wires

  • filament materials have higher resistivity, helping energy transfer by heating

  • changing the wire length or area changes resistance even if the material stays the same

If useful, mention that temperature can also change resistance, especially in metal conductors, but keep the main focus on the resistivity equation.

Current–potential difference characteristics

Not all components behave like fixed resistors.


  • an ohmic conductor gives a straight-line I–V graph through the origin at constant temperature

  • a filament lamp is non-ohmic because heating increases resistance

  • a diode conducts easily in one direction but very little in the reverse direction

Students should recognise that using V = IR remains valid for a component at a particular operating point, even when resistance is not constant overall.

Why component characteristics matter

Component characteristics affect circuit behaviour.


  • a filament lamp does not have constant resistance

  • a diode can control current direction

  • a fixed resistor is often used when predictable behaviour is needed

This sets up why realistic circuit analysis must consider the type of component, not only the numbers in a formula.

If wire length doubles and material and area stay the same, resistance is

A

Halved

B

Doubled

C

Unchanged

D

Quadrupled

Uses R = ρL/A. A common misconception is to think length has no effect if the material is unchanged.

Complete the paragraph

An ohmic conductor gives a I–V graph through the origin at constant temperature. A filament lamp is because heating changes its resistance. A diode conducts mainly in direction.

An ohmic conductor gives a
I–V graph through the origin at constant temperature. A filament lamp is
because heating changes its resistance. A diode conducts mainly in
curved
constant
reverse
both

Connects graph shape to component behaviour and checks three high-value terms from this subtopic.

How is resistivity different from resistance?

Expected elements: resistance belongs to a particular component or wire; resistivity is a material property; changing length or area changes resistance even when resistivity stays the same.

Potential dividers

A potential divider uses resistors in series to share the supply potential difference.


  • the supply potential difference is split between the components

  • the larger resistance gets the larger share of the potential difference

  • potential dividers are used to provide a chosen output potential difference

Phrase carefully: the potential difference is not 'used up' by the first resistor; the total is shared across the series components according to resistance.

Potential divider equation

For two resistors in series:


$ V{out} = V{in} \times \dfrac{R2}{R1 + R_2} $


  • $V_{out}$ is taken across the chosen resistor

  • increasing that resistor increases its share of the supply potential difference

  • the equation follows from the series current being the same through both resistors

Be explicit about where Vout is measured. Students often substitute the wrong resistor into the numerator.

Variable potential dividers

  • replacing one resistor with a thermistor or light-dependent resistor makes the output depend on temperature or light intensity

  • this allows sensing and control circuits

  • the analysis still depends on series current and the sharing of potential difference

Keep the focus on physics reasoning rather than electronics detail. The key idea is that changing resistance changes the voltage share.

A method for circuit analysis

When analysing an unfamiliar circuit:


  • redraw the circuit clearly if needed

  • label known currents, potential differences and resistances

  • simplify series and parallel sections where valid

  • apply conservation laws before calculation

  • use equations only after the physical structure is clear

This is the exam-technique slide: students often rush to equations before identifying the structure of the circuit.

Worked example: series circuit

A 12 V supply is connected to two resistors of 2 $\Omega$ and 4 $\Omega$ in series.


  • total resistance = 6 $\Omega$

  • current = $12/6 = 2$ A

  • potential difference across 2 $\Omega$ = 4 V

  • potential difference across 4 $\Omega$ = 8 V

  • 4 V + 8 V = 12 V, so the loop is consistent

This slide ties together total resistance, same current in series, and voltage sharing in proportion to resistance.

Worked example: parallel circuit

A 6 V supply is connected across two parallel resistors of 3 $\Omega$ and 6 $\Omega$.


  • each branch has 6 V across it

  • current in 3 $\Omega$ branch = 2 A

  • current in 6 $\Omega$ branch = 1 A

  • total current from the source = 3 A

Point out the contrast with the series example: now the potential difference is the same across branches, while currents differ.

Worked example: potential divider

A 9 V supply is connected across 1 k$\Omega$ and 2 k$\Omega$ in series. The output is taken across the 2 k$\Omega$ resistor.


  • total resistance = 3 k$\Omega$

  • current = $9/3000 = 3.0 \times 10^{-3}$ A

  • output potential difference = $I R = 6$ V

  • this matches $V_{out} = 9 \times 2/3 = 6$ V

Useful to show both methods: direct use of the divider equation and reasoning from current plus V = IR.

Key ideas to retain

  • current is the rate of flow of charge

  • potential difference is energy transferred per coulomb

  • current is conserved at junctions

  • energy is conserved around a complete loop

  • series and parallel circuits follow different current and potential difference rules

  • component characteristics and resistivity affect real circuit behaviour

This slide resolves the central question by pulling the rules together into one coherent model for analysis.

A potential divider gives the largest Vout across the

A

Smaller resistor

B

Larger resistor

C

Cell

D

Junction

Based on the slide stating that the larger resistance gets the larger share of the supply potential difference.

Complete the applied example

In the 12 V series example, the total resistance is Ω, so the current is A. In the 6 V parallel example, the branch currents add to a total current of A.

In the 12 V series example, the total resistance is
Ω, so the current is
A. In the 6 V parallel example, the branch currents add to a total current of
4
1
4.5
12

This is the applied task check, drawing directly on the worked examples for series and parallel analysis.

What is your first step with an unfamiliar circuit?

Expected elements: identify series/parallel structure first; label known quantities; apply conservation laws; then use V = IR or the divider equation; check physical consistency.

What is one idea from today that now feels secure?

This item has no instructions

Which part of circuit analysis still feels hardest?

This item has no instructions

One word for what helped you understand this lesson best

Use responses to identify which explanations or examples supported learning most effectively.

Glossary

current - the rate of flow of charge

charge - a property of matter measured in coulombs

potential difference - energy transferred per unit charge

resistance - a measure of how much a component opposes current

ohmic conductor - a component for which current is proportional to potential difference at constant temperature

resistivity - a material property linking resistance to length and cross-sectional area

series circuit - a circuit in which components are connected in a single path

This item has no instructions

Glossary

parallel circuit - a circuit with components arranged in separate branches

junction - a point where current can split or combine

branch current - the current in one path of a parallel circuit

potential divider - a series arrangement used to produce a chosen output potential difference

filament lamp - a non-ohmic component whose resistance increases as it heats up

diode - a component that conducts mainly in one direction

cross-sectional area - the area of the wire perpendicular to the direction of current

This item has no instructions