Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- =...

19
Chapter 21 1 Copyright © by Houghton Mifflin Company. All righ ts reserved. Chem 122 S04 exam s and hw 0 2 4 0 29 58 87 116 145 174 203 231 260 289 score Frequency Frequency Average = 225 A= 280+ B- = 226-247 A-=275-280 C+= 205-225 B+=269-275 C-= 160-204 B = 248-274

Transcript of Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- =...

Page 1: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 1Copyright © by Houghton Mifflin Company. All rights reserved.

Chem 122 S04 exams and hw

024

0

29

58

87

116

145

174

203

231

260

289

score

Fre

qu

en

cy

Frequency

Average = 225

A= 280+ B- = 226-247

A-=275-280 C+= 205-225

B+=269-275 C-= 160-204

B = 248-274

Page 2: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 2Copyright © by Houghton Mifflin Company. All rights reserved.

Page 3: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 3Copyright © by Houghton Mifflin Company. All rights reserved.

Mass-Energy Calculations

When nuclei decay, they form products of lower energy.

The change of energy is related to the change in mass, according to the mass-energy equivalence relation derived by Albert Einstein in 1905.

Energy and mass are equivalent and related by the equation 2mcE Here c is the speed of light, 3.00 x 108 m/s.

Page 4: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 4Copyright © by Houghton Mifflin Company. All rights reserved.

Mass-Energy Calculations

When nuclei decay, they form products of lower energy.

Consider the alpha decay of uranium-238 to thorium-234.

HeThU 42

23490

23892

We have written the atomic mass (in amu) beneath each nuclide symbol. (see Table 21.3)

238.05078 234.04359 4.00260

Page 5: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 5Copyright © by Houghton Mifflin Company. All rights reserved.

Mass-Energy Calculations

The binding energy of a nucleus is the energy needed to break a nucleus into its individual protons and neutrons.

Figure 21.16 shows the values of binding energy per nucleon plotted against the mass number for various nuclides.

Note that nuclides near mass number 50 have the largest binding energies per nucleon.

Page 6: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 6Copyright © by Houghton Mifflin Company. All rights reserved.

Figure 21.16: Plot of binding energy per nucleon versus mass number.

Page 7: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 7Copyright © by Houghton Mifflin Company. All rights reserved.

Mass-Energy Calculations

The binding energy of a nucleus is the energy needed to break a nucleus into its individual protons and neutrons.

For this reason, heavy nuclei might be expected to split to give lighter nuclei, while light nuclei might be expected to combine to form heavier nuclei.

Page 8: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 8Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fission is a nuclear reaction in which a heavy nucleus splits into lighter nuclei and energy is released.

For example, one of the possible mechanisms for the decay of californium-252 is

n4MoBaCf 10

10642

14256

25298

Page 9: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 9Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fission is a nuclear reaction in which a heavy nucleus splits into lighter nuclei and energy is released.

In some cases a nucleus can be induced to undergo fission by bombardment with neutrons.

n4SrXe 10

9038

14254

Un 23592

10 n3KrBa 1

09436

139546

n2RbCs 10

9037

14455

Page 10: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 10Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fission is a nuclear reaction in which a heavy nucleus splits into lighter nuclei and energy is released.

When uranium-235 undergoes fission, more neutrons are released creating the possibility of a chain reaction.

A chain reaction is a self-sustaining series of nuclear fissions caused by the absorption of neutrons released from previous nuclear fissions.

Page 11: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 11Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fission is a nuclear reaction in which a heavy nucleus splits into lighter nuclei and energy is released.

Figure 21.17 shows how such a chain reaction occurs.To sustain a nuclear chain reaction you must achieve a critical mass, which is the smallest mass of fissionable material required for a chain reaction.

Page 12: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 12Copyright © by Houghton Mifflin Company. All rights reserved.

Figure 21.17: Representation of a chain reaction of nuclear fissions.

Page 13: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 13Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fission is a nuclear reaction in which a heavy nucleus splits into lighter nuclei and energy is released.

A supercritical mass of fissionable material decays so rapidly as to cause a nuclear explosion (see Figure 21.18).

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Chapter 21 14Copyright © by Houghton Mifflin Company. All rights reserved.

Figure 21.18: An atomic bomb.

Page 15: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 15Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fission is a nuclear reaction in which a heavy nucleus splits into lighter nuclei and energy is released.

A nuclear fission reactor is a device that permits a controlled chain reaction of nuclear fissions. (see Figure 21.19)

Page 16: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 16Copyright © by Houghton Mifflin Company. All rights reserved.

Figure 21.19: Light-water nuclear reactor.

Page 17: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 17Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fission is a nuclear reaction in which a heavy nucleus splits into lighter nuclei and energy is released.

The fuel rods are the cylinders that contain fissionable material.Control rods are cylinders composed of substances that absorb neutrons and can therefore slow the chain reaction.

Page 18: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 18Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fusion is a nuclear reaction in which a light nuclei combine to give a stabler heavy nucleus plus possibly several neutrons, and energy is released.

An example of nuclear fusion is

nHeHH 10

42

31

21

Page 19: Chapter 211 Copyright © by Houghton Mifflin Company. All rights reserved. Average = 225 A= 280+B- = 226-247 A-=275-280C+= 205-225 B+=269-275C-= 160-204.

Chapter 21 19Copyright © by Houghton Mifflin Company. All rights reserved.

Nuclear Fission and Nuclear Fusion

Nuclear fusion is a nuclear reaction in which a light nuclei combine to give a stabler heavy nucleus plus possibly several neutrons, and energy is released.

Such fusion reactions have been observed in the laboratory using particle accelerators.

Sustainable fusion reactions require temperatures of about 100 million oC.