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Modern Physics

Eight topics on what happens when energy comes in lumps. Photons, whose energy is set by colour and never by brightness, the Bohr model and the standing-wave condition that makes its levels discrete, spectra read as differences between levels, blackbody radiation fixed by temperature alone, the photoelectric effect and its two independent knobs, Compton scattering as a two-body collision, and nuclear physics, where the books balance in nucleons and deliberately not in mass.

AP exam 12-15%8 topics
Topics
Key forms For every problem in this unit
Photon energy
E = hf = hc/λ. Set by FREQUENCY alone. Intensity counts photons per second, and never changes E
Matched unit pairs
h = 6.63 × 10⁻³⁴ J·s with λ in METRES → joules. hc = 1240 eV·nm with λ in NANOMETRES → eV. Never blend them
Size check
visible photons are a few eV. An answer far from that is a unit slip. 1 eV = 1.60 × 10⁻¹⁹ J
Wave-particle duality
ONE description; which behaviour appears depends on what the experiment measures. Nothing about the light switches
de Broglie wavelength
λ = h/p, for EVERY particle. INVERSE: faster means shorter, so a faster electron diffracts less
Bohr radius
r(n) = n² × 0.053 nm. Grows as n²
Hydrogen levels
E(n) = −13.6/n² eV. Magnitude falls as 1/n², so the levels CROWD toward 0 as n climbs
Reading the signs
−13.6 eV is the LOWEST level, not the highest. Deeper means more tightly bound
Standing-wave condition
nλ = 2πr closes the orbit on itself, which is where discrete levels come from
Transition photon
E(photon) = |E(final) − E(initial)|, a DIFFERENCE. Absorption goes UP, emission goes DOWN
Ionization
the jump to E = 0, so 13.6 eV from the ground state. Surplus energy becomes the freed electron's kinetic energy
Wien's law
λ(max) T = 2.90 × 10⁻³ m·K. INVERSE: hotter peaks BLUER
Stefan-Boltzmann
P = σeAT⁴, in KELVIN. Tripling T multiplies the power by 81
Blackbody spectrum
shape fixed by TEMPERATURE alone, not by the material. A good absorber is a good emitter
Photoelectric effect
K(max) = hf − φ. φ belongs to the METAL, f to the light. No intensity appears in it
Two independent knobs
FREQUENCY sets K(max) and the stopping voltage. INTENSITY sets how many electrons, the current
Stopping voltage plot
V(stop) against f: slope = h/e, vertical intercept = −φ/e, horizontal intercept = f₀ = φ/h
Compton scattering
a two-body COLLISION: incoming photon, scattered photon, recoiling electron. The photon does not vanish
Compton shift
Δλ = (h/m(e)c)(1 − cosθ), depending on the ANGLE only. Then λ' = λ + Δλ
Two separate books
nucleon number A and charge Z BALANCE. Mass does NOT: the defect leaves as energy
Mass-energy
E = Δmc². 1 u of defect ≈ 931 MeV
Stability
ranked by binding energy PER NUCLEON, peaking near iron at about 8.8 MeV. Total binding energy just grows with size
Why both work
moving TOWARD the iron peak from either side releases energy: fusion below it, fission above it
Half-life
each interval removes half of WHAT REMAINS: 1/2, 1/4, 1/8, never zero
Decay laws
N = N₀(½)^(t/t½) = N₀e^(−λt), with λ = 0.693/t½
What half-life depends on
the ISOTOPE alone. Not the amount, the temperature, the chemistry, or how long it has already sat
Alpha decay
A − 4, Z − 2. Emits a helium-4 nucleus
Beta-minus
A unchanged, Z + 1. A neutron becomes a proton: electron PLUS antineutrino
Beta-plus
A unchanged, Z − 1. A proton becomes a neutron: positron PLUS neutrino
Gamma decay
A and Z BOTH unchanged: the nucleus drops to a lower energy level. Same nuclide before and after
Balancing a decay
write every superscript and subscript, sum each row on each side, and let the arithmetic name the daughter
Why the neutrino is there
lepton number is conserved too, and it carries a share of the energy, which is why beta electrons come out with a SPREAD
Unit 15 tools
Challenge bank
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60 open-ended problems.

Read the question, work it out, then flip the card to compare your reasoning to the worked solution. Mark each card so you can return to the ones that still bite.

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Test the unit.

Twenty mixed items drawn from across all 8 topics, with guaranteed misconception-code coverage. Identifies which misconceptions still bite when you cannot see which topic the question came from.

20questions
8topics
28codes covered
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Check what stuck.

Units 9 through 15, drawn evenly so earlier units get the same share as this one. Twenty questions or a full 42-question section, your choice. Even coverage means this is a retention check rather than a score estimate.

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46topics
168codes covered
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