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Theme E — Nuclear and Quantum Physics

E.1.5 Rutherford Scattering and Nuclear Radius — IB Physics HL Revision Notes & Topical Questions

5 min read 9 parts Lesson 7 of 45 1 quiz

📚 IB Physics HL Hub / Topical Revision
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Curriculum Equation Key قوانين الرقم الهيدروجيني والاتزان الأيوني - pH & Acid-Base Equilibrium FormulasFast Exam Solution
pH = -log[H⁺] | pOH = -log[OH⁻] | pH + pOH = 14 | [H⁺][OH⁻] = 10⁻¹⁴
Word Equation & Conditions: الرقم الهيدروجيني = -لوغاريتم تركيز أيون الهيدروجين | pH + pOH = 14
Location & Specifications: الاتزان الأيوني، كيمياء 3 ثانوي، التحصيلي، و AP Chemistry.
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Lesson summary

E.1.5 Rutherford Scattering and Nuclear Radius — IB PHYSICS HL notes: Use R = R0 A1/3), nuclear density and the closest approach method to estimate nuclear size.Dependence — the radius depends on the nucleon number A because more nucleons need more spaceRelation — R = R0A1/3, fou…

  • Fermi radius
  • Doubling A
  • Data booklet
  • What the symbols mean
  • Much denser
  • Initial energy

Part 1 of 7Nuclear radius

Dependence
  • Dependence the radius depends on the nucleon number A because more nucleons need more space
Relation
  • R = R0A1/3, found from experimental data such as scattering
Fermi radius
  • R0 = 1.20 × 10−15 m (1.20 fm), the radius of a hydrogen nucleus with A = 1
Graph
  • R against A1/3 is a straight line through the origin with gradient R0
Doubling A
  • Doubling A raises the radius by only a factor 21/3 = 1.26
Data booklet
  • Data booklet the value of R0 is given

Part 2 of 7Nuclear density

Volume
  • V = (4/3)πR3 = (4/3)πR03A for a spherical nucleus
Mass
  • Mass m = Au where u is the atomic mass unit
Density
  • ρ = m/V = 3u/(4πR03), since A cancels
    What the symbols mean: ρ = density (kg m−3 or g cm−3) · m = mass (kg) · V = volume (m3)
Result
  • Result the density is the same for all nuclei and independent of radius
Value
  • Value of the order 1017 kg m−3, about 2.3 × 1017 kg m−3
Meaning
  • Meaning nucleons are evenly spaced throughout the nucleus whatever its size

Part 3 of 7Comparison with the atom

Much denser
  • Much denser nuclear density is far larger than atomic density
Mass
  • Mass most of the atom's mass is in the nucleus
Size
  • Size the nucleus is very small compared with the atom
Space
  • Space atoms are mostly empty space

Part 4 of 7Rutherford scattering and closest approach

Initial energy
  • Initial energy the alpha particle starts with kinetic energy Ek = ½mv2
Back-scattering
  • Back-scattering some alpha particles return, showing electrostatic repulsion by the nucleus
Closest approach
  • Closest approach the repulsion reduces the speed to zero momentarily at distance d before the direction reverses
Energy balance
  • Energy balance at that point the initial kinetic energy equals the electric potential energy, Ek = Ep

Part 5 of 7Closest approach equation

Potential energy
  • Ep = kQq/d with Q = 2e for the alpha particle and q = Ze for the target
Result
  • Ep = k(2e)(Ze)/d = 2kZe2/d
Distance
  • Distance d = 2kZe2/Ek
Charge
  • Charge an alpha particle has the charge of two protons
Units
  • Units convert MeV to joules by multiplying by 1.60 × 10−13

Part 6 of 7Interpretation

Upper limit
  • Upper limit d is an upper limit on the nuclear radius if the particle feels only the electrostatic force
Higher energy
  • Higher energy brings the particle closer to the nucleus
Strong force
  • Strong force when the energy is large enough to reach the strong-force region, the scattering departs from the electrostatic prediction
Angle dependence
  • Angle dependence scattering to large angles is greater for smaller impact parameter, larger Z and smaller energy
Scattering law
  • Scattering law the number at angle θ is proportional to 1/sin4(θ/2)
Shortcut
  • Shortcut kZe2 = 1.44 Z MeV fm, so d = 2 × 1.44Z/Ek fm with Ek in MeV
Head-on only
  • Head-on only the equation applies to head-on collisions

Part 7 of 7More from the specification

Rutherford Alpha Scattering
  • Directing alpha particles at thin gold foil proved that atoms possess a dense, positively charged nucleus containing most atomic mass, surrounded by orbiting electrons.
Discrete Atomic Energy Levels
  • Bound electrons occupy quantized energy levels;
    • de-excitation between orbits causes the emission of light with energy equal to the energy gap Delta E = E2 - E1.
Photon Emission and Planck's Constant
  • The wavelength of an emitted photon is determined by the de-excitation energy via Delta E = hf = hc / lambda,
  • where h represents Planck's constant.
Atomic Line Emission Spectrum
  • Because energy level separations are unique to each chemical element, the resulting emission and absorption spectra display characteristic discrete spectral lines.
Emission spectrum
  • The set of discrete wavelengths emitted by excited atoms of an element.
Photon
  • A quantum of electromagnetic energy, E = hf
Wavelength
  • Distance between a point on one wave and the same point on the next wave
Spectrum
  • Range of colours in white light.
Constant
  • Not changing.
Absorption
  • The conversion of wave energy to internal energy of the medium.
Energy level
  • A discrete energy an electron in an atom can have
Photon energy
  • E = hf = hc/λ, the energy carried by one photon.
Angular momentum
  • L = Iω for a rigid body; L = mvr⊥ for a particle.
∆E
∆E hf = E2 − E1
What the symbols mean: E = energy of one photon (J) · h = Planck constant (6.63 × 10−34 J s) · f = frequency (Hz)

Key terms

TermMeaning
Fermi radiusR0 = 1.20 fm, the constant in R = R0A1/3.
Nuclear densityThe same for all nuclei, ρ = 3u/(4πR03), about 2 × 1017 kg m−3.
Distance of closest approachThe distance at which the incident particle stops momentarily, d = 2kZe2/Ek.
Femtometre10−15 m.
Collimated beamA narrow parallel beam.

Avoid these mistakes

1
Using the charge e for the alpha particle — it is 2e.
2
Treating the distance of closest approach as the exact nuclear radius.
3
Taking R proportional to A instead of A1/3.
4
Forgetting to convert MeV to joules.
5
Applying the head-on formula to glancing collisions.

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