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Nuclear Reactions IB Physics Power Points Topic 07 and 13 Atomic and Nuclear Physics www.pedagogics.ca

Ppt djy 2011 2 topic 7 and 13 nuclear reactions

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Page 1: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Nuclear Reactions

IB Physics Power Points

Topic 07 and 13

Atomic and Nuclear Physics

www.pedagogics.ca

Page 2: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Nuclear TransmutationsDefinition: A nuclear reaction where one nuclide is changed into another. Examples of nuclear reactions include fission, fusion, and radioactive decay

Page 3: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Artificial (induced) Transmutations

• target nucleus is bombarded with another particle such as a nucleon, an alpha particle or another small nucleus

• if the target nucleus ‘captures’ an incoming particle a transmutation reaction occurs

   

Page 4: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Artificial (induced) Transmutations

This reaction was first observed by Rutherford in 1919.

This nuclear reaction equation is balanced. The sums of the mass and atomic numbers are equal for both sides of the reaction arrow (don’t worry about the electrons ie the ionic charges).

4 2+ 14 17 1 +2 7 8 1He N O + p

Page 5: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

PracticeA neutron is observed to strike a 16O nucleus and a deuteron (2H) is given off. What is the nuclide that results?

1 16 20 8 1 ?n O H

1 16 2 150 8 1 7n O H N

Page 6: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Nuclear Reactions – common notations  

01

42

10

11

alpha particle He or

neutron n or n

electron e or

proton p or p

Page 7: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Unified atomic mass unit  

/121 amu = 931.46 MeV/c2 = 0.93146 GeV/c2

1.660538782(83)×10−27 kg

Page 8: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Einstein’s mass – energy equivalence  

E=mc2

1 amu = 931.46 MeV = 0.93146 GeV of energy

Big Ideamass and energy are

interconvertible

Einstein’s equation relates rest mass to an equivalent energy1 kg = c2 J of energy (a lot!)

Page 9: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Now convert the energy value (in Joules) to electron volts

10 191.494 10 1.6 10 934 MeV

Page 10: Ppt djy 2011 2   topic 7 and 13 nuclear reactions
Page 11: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

mass defect

Consider a helium nucleus: 2 protons and 2 neutrons

mass 4.001504 u

Total mass of protons and neutrons?

4.031882 u

mass defect = 4.031882 – 4.001504 = 0.030378 u (Δm or σ)

Page 12: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Practice1.The mass of an atom of Ne-20 is 19.992435 u. Determine the mass defect for this nuclide.

10 (0.000549 1.007276 1.008665) 19.992435

0.172465

m

m u

Page 13: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

binding energy – explaining the missing mass

“assembling” a nucleus

binding energy

Individual protons and neutrons

Page 14: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Practice1. Determine the binding energy in O-16 (MeV and J). The mass of an O-16 atom is 15.994915 u.

8 (0.000549 1.007276 1.008665) 15.994915

0.137005

m

m u

0.137005 931.5 127.6 MeVE u

Page 15: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

binding energy per nucleon

depends on nuclide

iron has highest value – mental note

Page 16: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

PracticeUse the graph to estimate the binding energy per nucleon for Fe-56. Verify your estimate mathematically. Mass of Fe-56 ATOM is 55.934940 u

2

(26 0.000549) (26 1.007276) (30 1.008665) 55.934940

0.52846

0.52846 931.5 492.26049

492.26049 8.79 /

56

m

m amu

amu MeV c MeV

MeVMeV nucleon

Page 17: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

How much energy is required to remove a neutron from a C-13 nucleus? Write a balanced nuclear equation for this reaction.C-13 atom mass = 13.003355 amu, and of course C-12 has a mass of ? 13 12 1

6 6 0C C n

2

(12.000 1.008665) 13.003355

0.00531

0.00531 931.5 4.946

m

m amu

amu MeV c MeV

Page 18: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

STOP HERE and Complete Worksheet 1

Page 19: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

fusion and fission reactions

where does the energy come from?

Page 20: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

fusion and fission reactions

Fusion 2 light nuclides (low binding energy per nucleon) combine to make one heavy nuclide (higher binding energy per nucleon)

Fission One heavy nuclide (lower binding energy per nucleon) splits to form lighter nuclides (higher binding energy per nucleon)

Page 21: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

(235.043924 1.008665) (90.910187 141.929630 3 1.008665)

0.186777

931.5 173.99MeV

Page 22: Ppt djy 2011 2   topic 7 and 13 nuclear reactions
Page 23: Ppt djy 2011 2   topic 7 and 13 nuclear reactions
Page 24: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

1 1 2 01 1 1 +1

1 2 31 1 2

3 3 4 12 2 2 1

H + H H + e + ν + 0.4 MeV

H + H He + 5.5 MeV

He + He He + 2 H + 12.9 MeV

Page 25: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Big Fusion Problem Number 1: Confinement of plasma

Possibility 1 – inertial confinement: beams of laser light or ions compress a fuel pellet from all sides while heating it.

Possibility 2 – magnetic confinement: using a magnetic field to cause plasma (charged gas particles) to circulate endlessly within a confined space. 

 .

Page 26: Ppt djy 2011 2   topic 7 and 13 nuclear reactions

Big Fusion Problem Number 1: Confinement of plasmaPossibility 1 – inertial confinement: beams of laser light or ions compress a fuel pellet from all sides while heating it.Possibility 2 – magnetic confinement: using a magnetic field to cause plasma (charged gas particles) to circulate endlessly within a confined space. 

 Big Fusion Problem Number 2: Extracting energy

Once a fusion reaction is initiated and confined, the energy must be extracted in order to be any use (and to stop the whole thing melting down).

One possibility is to use a molten lithium blanket surrounding the fusion reaction to transfer the heat to a water based heat transport system.