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6.2.5Radioactivity

Nuclear Fusion

5 min read 6 parts Lesson 15 of 15 Unit quiz

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Section 1 of 6What Fusion Is

6.2.5 Nuclear Fusion

Fusion joins small nuclei into a larger one and releases energy.

Joining nuclei
  • Two light nuclei, such as isotopes of hydrogen, merge to form a single heavier nucleus.
Energy release
  • The new nucleus has slightly less mass than the starting nuclei, and the difference is released as energy.
In stars
  • The Sun and other main sequence stars shine because hydrogen nuclei fuse to make helium nuclei in their cores.
Example reaction
  • Deuterium and tritium fuse to give helium-4 and a neutron: ²₁H + ³₁H → ⁴₂He + ¹₀n, with energy released.

Section 2 of 6Conditions Needed

Fusion only happens when nuclei are forced extremely close together.

1
All nuclei carry positive charge, so any two nuclei repel each other through a strong electrostatic force.
2
To fuse, nuclei must approach so closely that the short range attraction between nucleons can take over.
3
This needs very high speeds, so the fuel must be heated to millions of degrees Celsius.
4
At such temperatures atoms lose their electrons and the fuel becomes a hot gas of charged particles called a plasma.
5
A very high pressure or density is also needed, so that collisions between nuclei happen often enough.

Section 3 of 6Fusion Compared with Fission

Fusion Compared with Fission
Fission
  • A large unstable nucleus such as uranium-235 splits into two smaller nuclei after absorbing a neutron.
Fusion
  • Small nuclei combine into one larger nucleus, and this process releases more energy per kilogram of fuel than fission.
Waste
  • Fusion produces no long lived radioactive waste of the kind made in fission, though some reactor parts become radioactive.
Fuel
  • Hydrogen isotopes can be obtained from water, so the fuel supply is very large.
FeatureFissionFusion
Change to nucleiOne large nucleus splitsTwo small nuclei join
Typical fuelUranium or plutoniumHydrogen isotopes
ConditionsControlled in a reactor at moderate temperatureMillions of degrees and high pressure
Used for power now?Yes, in power stationsNo, still experimental on Earth

Section 4 of 6Fusion on Earth

Containment problem
  • No solid container can survive plasma at millions of degrees, so strong magnetic fields hold the plasma away from the walls.
Energy balance
  • So far experimental reactors have found it hard to produce more useful energy than they use to heat the plasma.
Cold fusion
  • Claims of fusion at room temperature were never reliably repeated by other scientists, so they were not accepted.
Why keep trying
  • Fusion could give a large, low carbon electricity supply with plentiful fuel, which is why research continues.

Section 5 of 6Worked Example

Question Show that the equation ²₁H + ³₁H → ⁴₂He + ¹₀n is balanced for nucleon number and proton number.

  1. Add the nucleon (mass) numbers on the left: 2 + 3 = 5.
  2. Add the nucleon numbers on the right: 4 + 1 = 5, so they match.
  3. Add the proton (atomic) numbers on the left: 1 + 1 = 2.
  4. Add the proton numbers on the right: 2 + 0 = 2, so they match.

Answer Both totals are equal on each side (5 and 2), so the equation is balanced.

Section 6 of 6Exam Checklist & Tips

6.2.5 – Key Points for the Exam

  • Nuclear fusion The joining of two light nuclei to form a heavier nucleus, releasing energy.
  • Plasma A very hot gas in which atoms have lost electrons, so it contains free nuclei and electrons.
  • Electrostatic repulsion The force pushing positively charged nuclei apart, which must be overcome for fusion.
  • Isotope Atoms of the same element with different numbers of neutrons, such as ²₁H and ³₁H.
  • Nuclear fission The splitting of a large nucleus into smaller nuclei, releasing energy.

Common Mistakes

  • Mixing up fission and fusionfission splits nuclei, fusion joins them.
  • Saying fusion happens easily because it needs little energy; it needs extreme temperature and pressure.
  • Forgetting that nuclei repel each other, which is the reason the conditions are so extreme.
  • Writing equations whose nucleon numbers or proton numbers do not add up on both sides.
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