nuclear reactions, transmutations, fission and fusion

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Nuclear Reactions, Nuclear Reactions, Transmutations, Transmutations, Fission and Fission and Fusion Fusion

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Page 1: Nuclear Reactions, Transmutations, Fission and Fusion

Nuclear Reactions, Nuclear Reactions, Transmutations, Transmutations,

Fission and FusionFission and Fusion

Page 2: Nuclear Reactions, Transmutations, Fission and Fusion

Till now we have discussed only transmutations of one nuclei to another by emmiting radioactive particle that occur only naturally.

Natural transmutation (radioactivity)

Induced (artificial) transmutation

This change of one element to another through the This change of one element to another through the bombardment of a nucleus is known as bombardment of a nucleus is known as artificial artificial transmutation.transmutation.

Induced transmutation doesn’t mean it can not happen naturally Induced transmutation doesn’t mean it can not happen naturally – it means bombarment only– it means bombarment onlyexample: production of nitrogen from carbon in atmosphere or example: production of nitrogen from carbon in atmosphere or artificially induced in the labartificially induced in the lab

14 1 14 17 0 6 1N n C p

Page 3: Nuclear Reactions, Transmutations, Fission and Fusion

● ● Alpha particleAlpha particle, neutrons, protons, and deuterons …. can , neutrons, protons, and deuterons …. can be used to produce artificial nuclear reactions.be used to produce artificial nuclear reactions.

● ● The key to understanding these reactions and making The key to understanding these reactions and making predictions about the products of such reactions is being predictions about the products of such reactions is being able to balance nuclear equations.able to balance nuclear equations.

Energy released in nuclear reaction or decay is found the same way as binding energy: first find mass difference

Δm = LHS – RHS in u

and then E = Δm x 931.5 (MeV)

▪ conservation of total energy (energy + mass) must be satisfied

● For the nuclear equation : A → C + D or A + B → C + D

▪ nucleon and proton numbers must balance on each side of the equation.

Page 4: Nuclear Reactions, Transmutations, Fission and Fusion

TransmutationsTransmutations Examples Examples

Page 5: Nuclear Reactions, Transmutations, Fission and Fusion

Energy released in a decay: A → C + D

226 222 488 86 2Ra Rn + α M > m1 + m2 , but

total energy on the left = total energy on the right

2 2 21 2 1 2Mc = m c + m c + KE + KE

spontaneous decay: M > m1 + m2 → binding energy of the decaying nucleus < binding energies of the product nuclei. The daughter is more stable. This is why radioactive decay happens with heavy elements lying to the right of maximum in the binding energy curve. Energy released is in the form of kinetic energy of the products.

Page 6: Nuclear Reactions, Transmutations, Fission and Fusion

decay

Thorium – 228 decays by – emission:

Mass of thorium-228 nucleus = 227.97929 u

Mass of radium-224 nucleus + -particle = 223.97189 u + 4.00151 u = 227.97340 u

Mass difference = 227.97929 u – 227.97340 u = 0.00589 u = 5.49 MeV

What happens to this binding energy? It appears mostly as kinetic energy of – particle. The radium nucleus also recoils slightly (and so momentum is conserved).

22490 88

228 42 Th Ra

Page 7: Nuclear Reactions, Transmutations, Fission and Fusion

decay

Aluminum – 29 decays by – emission:

Mass of aluminum-29 nucleus = 28.97330 u

Mass of silicon-29 nucleus + -particle + antineutrino =

= 28.96880 u + 0.000549 u + 0 = 28.969349 u

Mass difference = 28.97330 u – 28.969349 u = 0.003951 u = 3.68 MeV

Again this becomes the kinetic energy of the decay products.

29 29 013 14 1Al Si + +

Page 8: Nuclear Reactions, Transmutations, Fission and Fusion

Energy released in a nuclear reaction/artificial transmutation

Nitrogen-14 will decay only if energy is supplied to it –collision with fast moving α particle:

14 4 17 17 2 8 1N O p

Famous 1. Rutherford’s induced Famous 1. Rutherford’s induced transmutation: bombarding nitrogen gas transmutation: bombarding nitrogen gas with alpha particles from bismuth‑214.with alpha particles from bismuth‑214.

18.0057 u < 18.0070 u

α particle must have enough kinetic energy to make up for imbalance in masses, and to provide for kinetic energy of products. This energy is suplied by a particle accelerator used to accelerate the helium nucleus.

2. or requires energy input

Nuclear reactions A + B → C + D can either

1. release energy

Δm = (mA + mB) – (mC + mD) < 0

if Δm = (mA + mB) – (mC + mD) > 0

The total amount of energy released will be E = Δmc2 in the form of kinetic energy of products. If there was initial kinetic energy, that will be added up to released energy.

Page 9: Nuclear Reactions, Transmutations, Fission and Fusion

FissionFission

● ● Fission means splitting up a Fission means splitting up a large nucleus (A > 200) into large nucleus (A > 200) into two smaller nuclei.two smaller nuclei.

● ● the total BE would increase the total BE would increase which means that the which means that the daughters are more stable daughters are more stable than parent.than parent.

● ● The excess energy is The excess energy is released by the reaction.released by the reaction.

Page 10: Nuclear Reactions, Transmutations, Fission and Fusion

● ● Spontaneous fission is very rare. Uranium is the largest Spontaneous fission is very rare. Uranium is the largest nucleus found on Earth. nucleus found on Earth. Its isotopes will sometimes fission Its isotopes will sometimes fission naturally. But half-life for U-235 is naturally. But half-life for U-235 is 7.04x108 years

● ● Bombarding the nucleus with neutrons can trigger a fission Bombarding the nucleus with neutrons can trigger a fission reaction. reaction.

● ● For exampleFor example

The strong forces that hold the nucleus together only act over a very short distance. When a uranium nucleus absorbs a neutron it

knocks the nucleus out of shape. If the nucleus deforms enough, the electrostatic repulsion between the protons in each half becomes greater than the strong force. It then splits in two.

The nuclei splits randomly.In the diagram, the fission fragments are shown as isotopes of Ba and Kr.This is just one of the many possible combinations.Fission of a uranium nucleus gives out about 200 MeV of energy.

Page 11: Nuclear Reactions, Transmutations, Fission and Fusion

Chain Chain ReactionsReactions

● ● When the uranium nucleus splits, a number of neutrons When the uranium nucleus splits, a number of neutrons are also ejected.are also ejected.

● ● If each ejected neutron causes another uranium nucleus If each ejected neutron causes another uranium nucleus to undergo fission, we get a chain reactionto undergo fission, we get a chain reaction

● ● The number of fissions increases rapidly and a huge The number of fissions increases rapidly and a huge amount of energy is released.amount of energy is released.

● ● Uncontrolled chain reactions are used in nuclear bombsUncontrolled chain reactions are used in nuclear bombs● ● The energy they unleash is devastating.The energy they unleash is devastating.● ● Nuclear power stations use the heat released in carefully Nuclear power stations use the heat released in carefully

controlled fission reactions to generate electricity.controlled fission reactions to generate electricity.● ● They use control rods to absorb some of the neutrons.They use control rods to absorb some of the neutrons.

Page 12: Nuclear Reactions, Transmutations, Fission and Fusion

FusionFusion

● ● Fusion means joining up two Fusion means joining up two small nuclei to form a small nuclei to form a bigger nucleus.bigger nucleus.

● ● When two small nuclei the When two small nuclei the product of fusion would product of fusion would have more BE per nucleon.have more BE per nucleon.

● ● The increases in binding energy per nucleon are much larger for fusion than for fission reactions, because the graph increases more steeply for light nuclei.

● ● So fusion gives out more energy per nucleon involved in the reaction than fission.

Page 13: Nuclear Reactions, Transmutations, Fission and Fusion

● ● The stars are powered by fusion reactions.The stars are powered by fusion reactions.

● ● Each second, in our Sun, more than 560 million tonnes of Each second, in our Sun, more than 560 million tonnes of hydrogen fuse together to make helium.hydrogen fuse together to make helium.

● ● One series of reactions for this is shown here:One series of reactions for this is shown here:

Each small nucleus has a positive charge so they will repel each other. To make the nuclei come close enough for the strong force to pull them together, they must be thrown together with very igh velocity. For this to take place, the matter must either be heated to temperatures as high as the core of the sun (about 13 million Kelvin) or the particles must be thrown together in a particle accelerator)

Page 14: Nuclear Reactions, Transmutations, Fission and Fusion

● ● The energy released is radiated by the Sun at a rate of 3.90 x The energy released is radiated by the Sun at a rate of 3.90 x 10102020 MW. MW.

● ● This is the power output of a million million million large power This is the power output of a million million million large power stations!stations!

● ● Not surprisingly scientists are keen to develop fusion as a Not surprisingly scientists are keen to develop fusion as a source of power (fusion reactor).source of power (fusion reactor).

● ● One possible reaction is the fusion of deuterium and tritium.One possible reaction is the fusion of deuterium and tritium.

● ● These are isotopes of hydrogenThese are isotopes of hydrogen

Page 15: Nuclear Reactions, Transmutations, Fission and Fusion

● ● Fusion has a number of advantages over fission:Fusion has a number of advantages over fission:● ● greater power output per kilogram,greater power output per kilogram,● ● the raw materials are cheap and readily available,the raw materials are cheap and readily available,● ● no radioactive elements are produced directly,no radioactive elements are produced directly,● ● irradiation by the neutrons leads to radioactivity in the reactor irradiation by the neutrons leads to radioactivity in the reactor

materials but these have relatively short half lives and only materials but these have relatively short half lives and only need to be stored safely for a short time.need to be stored safely for a short time.

● ● So why don't we use fusion in nuclear power stations?So why don't we use fusion in nuclear power stations?

● ● The JET (Joint European Torus) project was set up to carry out The JET (Joint European Torus) project was set up to carry out research into fusion power.research into fusion power.

● ● It has yet to generate a self‑sustaining fusion reaction.It has yet to generate a self‑sustaining fusion reaction.

● ● The main problem is getting two nuclei close enough for long The main problem is getting two nuclei close enough for long enough for them to fuse.enough for them to fuse.

Page 16: Nuclear Reactions, Transmutations, Fission and Fusion

●● Each small nucleus has a positive charge so they will repel each other. To make the nuclei come close enough for the strong force to pull them together, they must be thrown together with very igh velocity. For this to take place, the matter must either be heated to temperatures as high as the core of the sun (about 13 million Kelvin) or the particles must be thrown together in a particle accelerator)

●● At this temperature all matter exists as an ionised gas or At this temperature all matter exists as an ionised gas or plasma.plasma.

● ● Problem: containment. What can you use to hold something this hot?Problem: containment. What can you use to hold something this hot?

● ● JET (and Princeton) uses magnetic fields in a doughnutshaped JET (and Princeton) uses magnetic fields in a doughnutshaped chamber called a torus to keep the plasma away from the container chamber called a torus to keep the plasma away from the container walls.walls.

● ● Unfortunately generating high temperatures and strong magnetic Unfortunately generating high temperatures and strong magnetic fields uses up more energy than the fusion reaction produces!fields uses up more energy than the fusion reaction produces!

● ● The same problem is with accelerators, the path taken by Japan.The same problem is with accelerators, the path taken by Japan.

● ● We are still some years off a fusion power station.We are still some years off a fusion power station.

Page 17: Nuclear Reactions, Transmutations, Fission and Fusion
Page 18: Nuclear Reactions, Transmutations, Fission and Fusion

Applying the binding energy curve – checking stability

For example consider thefission reactionQuestion: has the system become more stable?

238 1 90 146 192 0 38 54 0U + n Sr + U + 3 n

total binding energy of U-238 = 7.6×238 = 1800 MeV

total binding energy of Sr-90 = 8.7×90 = 780 MeV

total binding energy of Xe-146 = 8.2×146 = 1200 MeV

The sum of the total binding energies of the fissionnuclei is greater than the binding energy of theuranium-238 nucleus. Effectively the system has becomemore stable by losing energy. (KEneutron provided that energy)

Page 19: Nuclear Reactions, Transmutations, Fission and Fusion

Similarly for the fusion reaction 3 41 1 22 1

0H + H He + n

the total binding energy of the helium nucleus is greater than the sum of binding energies of the tritium and deuterium nuclei. So, again as for fission, the system has effectively become more stable by losing energy.

total binding energy of H-2 = 1×2 = 2 MeV

total binding energy of H-3 = 2.8×3 = 8.4 MeV

total binding energy of He-4 = 4×7 = 28 MeV

Page 20: Nuclear Reactions, Transmutations, Fission and Fusion

nucleus

proton

neutron

electron

 The strong force does not actually occur directly between protons and neutrons in the nucleus, but in the smaller quarks making them up.

The force is mediated by fundamental particles called gluons, named for the way they glue quarks together. Each proton or neutron is

composed of three quarks. The strong nuclear force between nucleons is the result of the force holding together their constituent

quarks.