Fusion & Stars

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Fusion Reactions in Stars

  • Nuclear fusion is the joining of two small nuclei to produce a larger nucleus, releasing energy.
  • In stars, four hydrogen nuclei (protons) fuse to form one helium nucleus, releasing a huge amount of energy.
  • The proton-proton chain is the series of reactions that produces helium from hydrogen in stars like the Sun.
  • The energy released provides an outward radiation pressure that prevents the star from collapsing under gravity.
  • For fusion to occur, nuclei must overcome electrostatic repulsion and get close enough for the strong nuclear force to act.
  • This requires extremely high temperature and density, such as in the core of a star, or high-speed collisions in a particle accelerator.
  • On Earth, research focuses on the deuterium-tritium (D-T) reaction: ²₁H + ³₁H → ⁴₂He + ¹₀n, which releases a large amount of energy per unit mass.

Hydrogen fusion in a star

Hydrogen fusion in a star

Energy Released in Fusion Reactions

  • When two small nuclei fuse, the resulting larger nucleus has a higher binding energy per nucleon than the original nuclei.
  • The mass defect (difference in mass between reactants and products) is converted into energy according to ΔE = Δmc².
  • For example, fusing two deuterium nuclei into helium releases about 24 MeV (28 MeV − 4 MeV).
  • In the proton-proton chain, the overall reaction is 4¹₁H → ⁴₂He + 2e⁺ + 2νₑ, releasing energy.
  • The energy released per fusion reaction can be calculated from the mass defect and used to determine the rate of hydrogen consumption in a star.

Star Formation

  • Stars form from a nebula — a giant cloud of hydrogen gas and dust.
  • Gravitational collapse causes denser clumps to form, heating up and glowing as a protostar.
  • When the core temperature reaches millions of kelvin, hydrogen fusion begins, producing helium and releasing energy.
  • The outward radiation pressure and gas pressure balance the inward gravitational force, leading to a stable main sequence star.
  • If outward pressure > gravitational force, the star expands; if outward pressure < gravitational force, the star contracts.
  • Equilibrium is maintained as long as the inward and outward forces are balanced.

Star formation stages

Star formation stages

Life Cycle of a Star

  • All stars begin with the same stages: nebula → protostar → main sequence star.
  • A star spends most of its life on the main sequence, where it is stable due to balanced forces.
  • Low-mass stars (like the Sun) evolve: red giant → planetary nebula → white dwarf.
  • High-mass stars evolve: red supergiant → supernova → neutron star or black hole.
  • In red giants, helium fusion occurs in the core, and the outer layers expand and cool.
  • In massive stars, fusion continues up to iron, after which the core collapses and a supernova occurs.
  • The remnant of a supernova can be a neutron star or, if massive enough, a black hole.

Life cycle of a large mass star

Life cycle of a large mass star

The Hertzsprung–Russell (HR) Diagram

  • The HR diagram plots stellar luminosity (y-axis) against surface temperature (x-axis, decreasing to the right).
  • Most stars lie on the main sequence, a diagonal band where luminosity increases with temperature.
  • Red giants and red supergiants are above the main sequence, with high luminosity but cooler temperatures.
  • White dwarfs are below and to the left of the main sequence: hot but low luminosity.
  • The HR diagram only shows stars in stable phases; transitory phases are short-lived.
  • The Sun is a main sequence star with a luminosity of 1 (relative to itself) and a surface temperature of about 5800 K.

Emission & Absorption Spectra in Stars

  • A continuous spectrum contains all wavelengths and is produced by hot, dense sources like stellar cores.
  • An emission line spectrum consists of bright lines on a black background, produced by hot, low-pressure gases.
  • An absorption line spectrum consists of dark lines on a continuous spectrum, produced when white light passes through a cooler gas.
  • Each element produces a unique pattern of spectral lines, acting as a fingerprint for identifying elements in stars.
  • Stars emit an absorption spectrum because their outer atmospheres are cooler than the core.
  • The chemical composition of a star can be determined by comparing its absorption spectrum with known emission spectra.

Stellar Parallax

  • Stellar parallax is the apparent shift in position of a nearby star against distant background stars as Earth orbits the Sun.
  • The parallax angle p (in arcseconds) is related to distance d (in parsecs) by p = 1/d.
  • This method is accurate for stars up to about 100 pc away.
  • 1 parsec is the distance at which 1 AU subtends an angle of 1 arcsecond: 1 pc ≈ 3.1 × 10¹⁶ m.
  • 1 light-year is the distance light travels in one year: 1 ly ≈ 9.5 × 10¹⁵ m.
  • 1 astronomical unit (AU) is the mean Earth-Sun distance: 1 AU ≈ 1.5 × 10¹¹ m.

Determination of Stellar Radii

  • The radius of a star can be found by combining Wien's displacement law and the Stefan-Boltzmann law.
  • Wien's displacement law: λmax T = 2.9 × 10⁻³ m K, gives the surface temperature from the peak wavelength.
  • The Stefan-Boltzmann law: L = 4πr²σT⁴, relates luminosity, radius, and temperature.
  • If luminosity and temperature are known, the radius can be calculated.
  • For example, Betelgeuse has a radius about 1000 times that of the Sun.

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Câu hỏi luyện tập

Xem trước miễn phí — 8 trên 63 câu hỏi. Đăng ký để xem tất cả.
  1. 1.Which of the following is the correct definition of nuclear fusion?

    Easy
    • AThe joining of two small nuclei to produce a larger nucleus
    • BThe splitting of a large nucleus into two smaller nuclei
    • CThe joining of two large nuclei to produce a smaller nucleus
    • DThe emission of an α particle from a nucleus
  2. 2.Which of the following is the correct definition of nuclear fission?

    Easy
    • AThe joining of two small nuclei to produce a larger nucleus
    • BThe splitting of a large nucleus into two smaller nuclei
    • CThe joining of two large nuclei to produce a smaller nucleus
    • DThe emission of a β particle from a nucleus
  3. 3.In a main sequence star, the inward gravitational force is balanced by the outward radiation pressure.

    Easy

    True or false?

  4. 4.Which force must be overcome for two nuclei to fuse?

    Easy
    • AGravitational force
    • BElectrostatic repulsion between protons
    • CStrong nuclear force
    • DWeak nuclear force
  5. 5.What is the name of the force that acts when nuclei get close enough to fuse?

    Easy
    • AElectrostatic force
    • BGravitational force
    • CStrong nuclear force
    • DWeak nuclear force
  6. 6.What are the two factors that the power output of a star depends on according to the Stefan-Boltzmann law?

    Medium
    • ASurface temperature and radius
    • BLuminosity and distance
    • CMass and age
    • DColour and chemical composition
  7. 7.What is the definition of a parsec?

    Medium
    • AThe distance travelled by light in one year
    • BThe mean distance from the centre of the Earth to the centre of the Sun
    • CThe distance at which the parallax angle is 1 arcsecond
    • DThe distance at which the parallax angle is 1°
  8. 8.A light-year is a unit of time.

    Easy

    True or false?

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