โ† Back to Electricity

โšก Electrical Charge and Current

Spec 6.2.1.2 ๐Ÿ“— Foundation
๐Ÿ“– In-Depth Theory

Electric Current โ€” Flow of Charge

ELECTRIC CURRENT is a flow of electrical charge.
For current to flow, two conditions must be met:
1. There must be a CLOSED CIRCUIT โ€” a complete, unbroken conducting path.
2. There must be a SOURCE OF POTENTIAL DIFFERENCE (a battery or power supply) to drive the charge.
Current is measured in AMPERES (A).
1 ampere = 1 coulomb of charge passing a point per second.
In metal conductors, the charge carriers are FREE ELECTRONS.
In solutions (electrolytes), the charge carriers are IONS.
CONVENTIONAL CURRENT flows from + to โˆ’ around the external circuit.
ELECTRON FLOW is actually from โˆ’ to + (electrons repelled from the negative terminal).
Conventional current direction was defined before electrons were discovered.

Charge, Current and Time

Q = I ร— t
Q = charge flow (coulombs, C)
I = current (amperes, A)
t = time (seconds, s)
Rearranging:
I = Q รท t
t = Q รท I
EXAMPLE 1:
A current of 2 A flows for 30 s:
Q = 2 ร— 30 = 60 C
EXAMPLE 2:
120 C flows in 4 minutes:
t = 4 ร— 60 = 240 s
I = 120 รท 240 = 0.5 A
One coulomb โ‰ˆ 6.24 ร— 10ยนโธ electrons.

Current in Series and Parallel Circuits

SERIES circuit:
Current is the SAME everywhere โ€” only one path for charge.
Iโ‚ = Iโ‚‚ = Iโ‚ƒ
PARALLEL circuit:
Current SPLITS at junctions โ€” more paths available.
I_total = Iโ‚ + Iโ‚‚ + Iโ‚ƒ
Branches with lower resistance carry more current.
MEASURING CURRENT:
Use an AMMETER connected in SERIES.
Ammeters have very LOW resistance โ€” do not significantly affect the circuit.
โš ๏ธ Common Mistake

Time must be in SECONDS when using Q = It. If given minutes, multiply by 60 first. In a series circuit, current is the SAME at every point โ€” it does not get 'used up' passing through components.

๐Ÿ“ Variables
QCharge (Q) is measured in coulombs (C)
ICurrent (I) is measured in amperes (A)
tTime (t) is measured in seconds (s)
๐Ÿ“ Key Equations
Q = I ร— t
๐Ÿ“Œ Key Note

Current = rate of flow of charge. Q = It. Unit: ampere (A). Series: same current everywhere. Parallel: current splits โ€” I_total = sum of branches. Charge carriers in metals = electrons. Conventional current: + to โˆ’. Electron flow: โˆ’ to +.

๐ŸŽฏ Matching Activity โ€” Charge and Current

Match each scenario to the correct value. โ€” drag the symbols on the right to match the component names on the left.

60 C
Drop here
0.5 A
Drop here
Same everywhere
Drop here
Splits at junctions
Drop here
Current = 3 A, time = 20 s โ€” Q = 3 ร— 20
Charge = 90 C, time = 3 minutes โ€” I = 90 รท 180
Current at each point in a series circuit
Current behaviour in a parallel circuit
โšฝ FIFA Worked Examples
Charge Calculation

A current of 0.4 A flows through a lamp for 5 minutes. Calculate the charge that flows.

F

Q = I ร— t

I

I = 0.4 A, t = 5 ร— 60 = 300 s

F

Q = 0.4 ร— 300

A

Q = 120 C

๐Ÿงช Required Practical

๐Ÿ”ฌ RP15 (Physics) โ€” Set up series and parallel circuits; measure current with ammeters at different positions to verify series current is constant and parallel currents sum to total.

Know the method, variables, equipment and how to analyse results.

๐ŸŽฏ Test Yourself
Question 1 of 2
1. A charge of 180 C flows through a resistor in 2 minutes. What is the current?
2. In a series circuit, an ammeter before the first lamp reads 0.3 A. What does an ammeter between the two lamps read?
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