Pictures first. Formulas boxed. Every exam keyword highlighted.
HOW TO STUDY WITH THIS
Read the π‘ box the whole topic in 1 line
Study the diagram cover it, redraw it
Learn the yellow formulas & keywords
Redo the worked example without looking
THE CHAPTERS
π
CH 1
General Properties of Waves
v = fΞ»
π‘
CH 2
Electromagnetic Spectrum
order
π‘
CH 3
Light: Reflection & Refraction
laws
π
CH 4
Lenses
converging lens
π
CH 5
Charge & Current Electricity
Q = It
π
CH 6
D.C. Circuits
series
π
CH 7
Practical Electricity
power
π§²
CH 8
Magnetism & Electromagnetism
magnetic fields
β’οΈ
CH 9
Radioactivity
Ξ± Ξ² Ξ³
π NOTESchools split Sec 3 / Sec 4 physics differently β check the other year if a chapter is missing.
π¨ PRINTCtrl+P β Save as PDF Β· Scale 100% Β· Margins None Β· Background graphics ON
Sec 4 Combined Physics Β· SEC K326
π
1
General Properties of Waves
v = fΞ», transverse & longitudinal, sound
BIG IDEAWaves transfer energy without transferring matter. v = fΞ» Β· f = 1 Γ· T
crest-to-crest = wavelength; centre to crest = amplitude
Term
Meaning
amplitude A
max displacement from rest
wavelength Ξ»
distance between successive crests
frequency f
waves per second (Hz)
period T
time for one wave (s)
wavefront
line joining points in phase (crests)
Transverse
Longitudinal
vibration β direction of travel
vibration β₯ direction of travel
crests & troughs
compressions & rarefactions
light, water, EM waves
sound
π Sound
needs a medium (not in vacuum) Β· fastest in solids Β· loudness β with amplitude Β· pitch β with frequency Β· human range 20 Hzβ20 kHz
Echo
distance = (speed Γ time) Γ· 2 β sound goes there and back
π WHY IT WORKSWhy v = fΞ»: in one period T, the wave moves forward exactly one wavelength. So speed = Ξ» Γ· T = fΞ».
π§ Worked example β follow the thinking
A boy claps 170 m from a wall and hears the echo 1.0 s later. Find the speed of sound.
Step
Why I do this
Total distance = 2 Γ 170 = 340 m
π Sound travels to the wall AND back.
v = 340 Γ· 1.0 = 340 m/s
π speed = distance Γ· time.
Sec 4 Combined Physics Β· SEC K326
π‘
2
Electromagnetic Spectrum
order, uses, hazards
BIG IDEAAll EM waves are transverse, travel at 3.0 Γ 10βΈ m/s in vacuum and need no medium.
"Raging Martians Invaded Venus Using X-ray Guns"
Wave
Use
Hazard
radio
radio/TV broadcasting
β
microwave
cooking, mobile phones, satellites
internal heating of tissue
infrared
remote controls, thermal imaging, toasters
skin burns
visible
seeing, optical fibres, photography
eye damage (lasers)
ultraviolet
sterilising, detecting forged notes
sunburn, skin cancer
X-ray
medical images, airport security
ionising β cell damage, cancer
gamma
killing cancer cells, sterilising food
ionising β cancer, mutation
π WHY IT WORKSWhy higher frequency is more dangerous: high-frequency EM waves carry more energy per "packet", enough to ionise atoms in cells and damage DNA. Low-frequency waves mainly just heat.
π§ Worked example β follow the thinking
A radio station broadcasts at 100 MHz. Find the wavelength.
Step
Why I do this
v = 3.0 Γ 10βΈ m/s
π All EM waves have this speed.
Ξ» = v Γ· f = 3.0 Γ 10βΈ Γ· 100 Γ 10βΆ
π Rearrange v = fΞ»; M = 10βΆ.
Ξ» = 3.0 m
π
Sec 4 Combined Physics Β· SEC K326
π‘
3
Light: Reflection & Refraction
laws, refractive index
BIG IDEAReflection: i = r. Refraction: n = sin i Γ· sin r = c Γ· v. Light bends towards the normal entering a denser medium.
angles from the normal
Laws
reflection: i = r; incident ray, reflected ray and normal in the same plane refraction: light changes speed β changes direction plane-mirror image: same size, upright, laterally inverted, virtual, same distance behind
Refractive index n
n = speed in vacuum Γ· speed in medium glass n β 1.5 β light at 2 Γ 10βΈ m/s in glass no bending if ray enters along the normal
Everyday
pool looks shallower Β· straw looks bent Β· mirage
π WHY IT WORKSWhy a pool looks shallower: light from the bottom bends away from the normal as it leaves water. Your brain traces the ray back in a straight line, so the bottom seems higher than it is.
π§ Worked example β follow the thinking
Light hits glass (n = 1.5) at i = 40Β°. Find r.
Step
Why I do this
sin r = sin 40Β° Γ· 1.5
π n = sin i Γ· sin r rearranged.
= 0.643 Γ· 1.5 = 0.4285
π Calculator in DEGREE mode.
r = sinβ»ΒΉ(0.4285) = 25.4Β°
π r < i: bends towards the normal (denser).
Sec 4 Combined Physics Β· SEC K326
π
4
Lenses
converging lens, focal length, images
BIG IDEAA converging (convex) lens bends parallel rays to meet at the focal point F. Focal length f = lens to F.
ray 1: parallel β through F Β· ray 2: through the optical centre β straight on
Object
Image
Image is
Use
beyond 2F
between F and 2F
real, inverted, diminished
camera, eye
at 2F
at 2F
real, inverted, same size
photocopier (1:1)
between F and 2F
beyond 2F
real, inverted, magnified
projector
at F
at infinity
β
spotlight
inside F
same side as object
virtual, upright, magnified
magnifying glass
Real vs virtual
real: rays actually meet β can be caught on a screen virtual: rays only seem to come from it
Find f quickly
focus a distant object (window) on a screen β lens-to-screen distance β f
π WHY IT WORKSWhy the rays are chosen: we already know where these special rays go without measuring angles. Two rays from the top of the object are enough β where they meet is the top of the image.
π§ Worked example β follow the thinking
An object is 30 cm from a lens of focal length 10 cm. Describe the image.
Step
Why I do this
2F = 20 cm, object at 30 cm β beyond 2F
π Compare the object distance with f and 2f.
Image: real, inverted, diminished, between F and 2F
π Use the table / two rays.
Sec 4 Combined Physics Β· SEC K326
π
5
Charge & Current Electricity
Q = It, e.m.f., p.d., resistance
BIG IDEAQ = It Β· V = W Γ· Q Β· R = V Γ· I. Current = rate of flow of charge.
Quantity
Definition
Unit
charge Q
β
coulomb C
current I
charge per unit time
ampere A
e.m.f. E
work done by source per unit charge to drive charge round the whole circuit
R β length (longer β more collisions) Β· R β 1 Γ· cross-sectional area (thicker β easier) Β· R = ΟL Γ· A
π WHY IT WORKSWhy a longer wire has more resistance: electrons collide with more metal ions along a longer path. A thicker wire gives more paths side by side, so the current flows more easily.
π§ Worked example β follow the thinking
A charge of 120 C flows through a 6 V lamp in 1 minute. Find I, R and the energy transferred.
BIG IDEASeries: same current, voltages add, R = Rβ + Rβ. Parallel: same p.d., currents add, 1/R = 1/Rβ + 1/Rβ.
Symbol
Component
β|ββ
cell (long line +)
βββ
lamp
βββ
fixed resistor
ββββ
variable resistor
β(A)β
ammeter (series)
β(V)β
voltmeter (parallel)
ββ~β
fuse
ββ·|β
diode / LED (arrows out)
Series
I same everywhere Vtotal = Vβ + Vβ Rtotal = Rβ + Rβ (bigger than each)
Parallel
V same across each branch Itotal = Iβ + Iβ Rtotal smaller than the smallest branch
π WHY IT WORKSWhy parallel R is smaller: each new branch is an extra path for charge, so more current flows for the same p.d. β and R = V Γ· I gets smaller.
fuse: thin wire melts if I too large Β· rating just above normal current (3, 5, 13 A) circuit breaker: trips, can be reset earthing: metal case connected to earth β fault current flows to earth, blows fuse double insulation (β§): plastic casing, no earth wire needed
Hazards
damaged insulation β shock Β· overheating of cables (too much current) Β· damp / wet conditions β water conducts
Why on the live wire?
if the fuse/switch were on neutral, the appliance would still be at high voltage even when off/blown β shock risk
π WHY IT WORKSWhy heating happens: charges collide with ions in the resistor, transferring energy to them β the resistor gets hot. Used in kettles, irons, heaters.
π§ Worked example β follow the thinking
A 230 V kettle is rated 2.3 kW. Choose a fuse: 3 A, 5 A or 13 A.
Step
Why I do this
I = P Γ· V = 2300 Γ· 230 = 10 A
π Normal working current.
Fuse must be slightly higher than 10 A
π Too low β blows in normal use; too high β no protection.
Choose 13 A
π
Sec 4 Combined Physics Β· SEC K326
π§²
8
Magnetism & Electromagnetism
magnetic fields, electromagnets, motor effect
BIG IDEAField lines go N β S. A current makes a magnetic field; a current in a field feels a force (Fleming's left-hand rule).
bar magnet field (closer lines = stronger)
Magnets
like poles repel, unlike attract Β· iron: soft β easily magnetised and loses it (temporary, electromagnets) Β· steel: hard β permanent magnets Β· induced magnetism: iron near a magnet becomes a magnet
Fields from currents
straight wire: circles round the wire β right-hand grip rule solenoid: like a bar magnet; stronger with more turns, more current, iron core reverse current β field reverses
β Fleming's left-hand rule
First finger = Field Β· seCond = Current Β· thuMb = Motion (force) motor: coil in field β turning effect
π WHY IT WORKSWhy a current-carrying wire moves in a field: the wire's own circular field adds to the magnet's field on one side and cancels it on the other. The wire is pushed from the strong-field side to the weak-field side.
π§ Worked example β follow the thinking
A wire lies flat on the page. Field points to the right β, current flows up the page β. Which way is the force?
Step
Why I do this
First finger β field: point it right
π Fingers at right angles to each other.
Second finger β current: point it up the page
π Twist your LEFT hand to fit.
Thumb now points into the page β force into the page
π Thumb = motion. Reverse either I or B β force reverses.
Sec 4 Combined Physics Β· SEC K326
β’οΈ
9
Radioactivity
Ξ± Ξ² Ξ³, half-life, isotopes
BIG IDEAUnstable nuclei decay randomly and spontaneously, giving out Ξ±, Ξ² or Ξ³. Half-life = time for half the nuclei to decay.
Nuclide notation
ᴬZX A = nucleon number (p + n) Β· Z = proton number isotopes: same Z, different A (e.g. ΒΉΒ²C, ΒΉβ΄C)
each half-life halves the activity
Ξ± alpha
Ξ² beta (Ξ²β»)
Ξ³ gamma
Is
helium nucleus (2p 2n)
fast electron
EM wave
Ionising
strongest
medium
weakest
Stopped by
paper / few cm air
few mm aluminium
thick lead / concrete
Charge
+2
β1
0
Uses
Ξ³: kill cancer cells, sterilise Β· Ξ²: paper thickness control Β· Ξ±: smoke detectors Β· tracers (short half-life)
Safety
background radiation from rocks, cosmic rays, food Β· minimise time, maximise distance, use shielding Β· tongs, lead aprons
π WHY IT WORKSWhy we use half-life: we can never say WHEN one nucleus will decay β it is random. But with billions of nuclei, the fraction left after a set time is very predictable.
π§ Worked example β follow the thinking
A sample has activity 800 Bq; half-life 3 days. Find activity after 12 days.