chapter 21 nuclear chemistry © 2012 pearson education, inc

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Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc.

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Page 1: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

Chapter 21

Nuclear Chemistry

© 2012 Pearson Education, Inc.

Page 2: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

The Nucleus

• Remember that the nucleus is composed of the two nucleons, protons and neutrons.

• The number of protons is the atomic number.• The number of protons and neutrons together

is effectively the atomic mass.

© 2012 Pearson Education, Inc.

Page 3: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Isotopes

• Not all atoms of the same element have the same mass, due to different numbers of neutrons in those atoms.

• There are, for example, three naturally occurring isotopes of uranium:– Uranium-234– Uranium-235– Uranium-238

© 2012 Pearson Education, Inc.

Page 4: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Radioactivity

• It is not uncommon for some nuclides of an element to be unstable, or radioactive.

• We refer to these as radionuclides.

• There are several ways radionuclides can decay into a different nuclide.

© 2012 Pearson Education, Inc.

Page 5: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Types ofRadioactive Decay

© 2012 Pearson Education, Inc.

Page 6: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Alpha Decay

Alpha decay is the loss of an α-particle (a helium nucleus):

He42

U23892

Th23490 He4

2 +

© 2012 Pearson Education, Inc.

Page 7: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Sample Exercise 21.1 Predicting the Product of a Nuclear Reaction

What product is formed when radium-226 undergoes alpha decay?

Practice ExerciseWhich element undergoes alpha decay to form lead-208?

Page 8: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. +2B. –2C. +4D. –4

Page 9: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Beta Decay

Beta decay is the loss of a -particle (a high-energy electron):

01 e0

1or

I13153 Xe131

54 + e0

1

© 2012 Pearson Education, Inc.

Page 10: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Electron Capture (K-Capture)

Addition of an electron to a proton in the nucleus is known as electron capture or K-capture.– The result of this process is that a proton is

transformed into a neutron:

p11 + e0

1 n10

© 2012 Pearson Education, Inc.

Page 11: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Positron Emission

Some nuclei decay by emitting a positron, a particle that has the same mass as, but an opposite charge to, that of an electron:

e01

C116

B115 + e0

1

© 2012 Pearson Education, Inc.

Page 12: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Gamma Emission

Gamma emission is the loss of a -ray, which is high-energy radiation that almost always accompanies the loss of a nuclear particle:

00

© 2012 Pearson Education, Inc.

Page 13: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Sample Exercise 21.2 Writing Nuclear Equations

Write nuclear equations for (a) mercury-201 undergoing electron capture; (b) thorium-231 decaying to protactinium-231.

Practice ExerciseWrite a balanced nuclear equation for the reaction in which oxygen-15 undergoes positron emission.

Page 14: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. Alpha particleB. NeutronC. ProtonD. Beta particle

Page 15: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Neutron–Proton Ratios• Any element with more than one proton

(i.e., anything but hydrogen) will have repulsions between the protons in the nucleus.

• A strong nuclear force helps keep the nucleus from flying apart.

• Neutrons play a key role stabilizing the nucleus.

• Therefore, the ratio of neutrons to protons is an important factor.

• For smaller nuclei (Z 20), stable nuclei have a neutron-to-proton ratio close to 1:1.

• As nuclei get larger, it takes a larger number of neutrons to stabilize the nucleus.

© 2012 Pearson Education, Inc.

Page 16: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Stable Nuclei

• The shaded region in the figure, the so-called belt of stability, shows what nuclides would be stable.

• Nuclei above this belt have too many neutrons.

• These nuclei tend to decay by emitting beta particles.

• Nuclei below the belt have too many protons.

• Nuclei tend to become more stable by positron emission or electron capture.

© 2012 Pearson Education, Inc.

Page 17: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Stable Nuclei

• There are no stable nuclei with an atomic number greater than 83.

• Nuclei with such large atomic numbers tend to decay by alpha emission.

© 2012 Pearson Education, Inc.

Page 18: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Sample Exercise 21.3 Predicting Modes of Nuclear Decay

Predict the mode of decay of (a) carbon-14, (b) xenon-118.

Practice ExercisePredict the mode of decay of (a) plutonium-239, (b) indium-120.

Page 19: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. 82 neutronsB. 92 neutronsC. 102 neutronsD. 112 neutrons

Page 20: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Radioactive Series

• Large radioactive nuclei cannot stabilize by undergoing only one nuclear transformation.

• They undergo a series of decays until they form a stable nuclide (often a nuclide of lead).

© 2012 Pearson Education, Inc.

Page 21: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Some Trends

Nuclei with 2, 8, 20, 28, 50, or 82 protons or 2, 8, 20, 28, 50, 82, or 126 neutrons tend to be more stable than nuclides with a different number of nucleons.

Nuclei with an even number of protons and neutrons tend to be more stable than nuclides that have odd numbers of these nucleons.

© 2012 Pearson Education, Inc.

Page 22: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. Even number of protons and fewer than three stable isotopes, 2 elements; odd number of protons and more than two isotopes, 2 elements

B. Even number of protons and fewer than three stable isotopes, 1 element; odd number of protons and more than two isotopes, 3 elements

C. Even number of protons and fewer than three stable isotopes, 4 elements; odd number of protons and more than two isotopes, 1 element

D. Even number of protons and fewer than three stable isotopes, 3 elements; odd number of protons and more than two isotopes, 0 elements

Page 23: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. All have an even number of neutrons.B. All have an odd number of neutrons.C. F and Na have an odd number of neutrons whereas Al and P have

an even numberD. F and P have an odd number of neutrons whereas Al and Na have

an even number.

Page 24: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Sample Exercise 21.4 Predicting Nuclear Stability

Predict which of these nuclei are especially stable: , , .

Practice ExerciseWhich of the following nuclei would you expect to exhibit a special stability: , , ?

.

Page 25: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Nuclear Transformations

Nuclear transformations can be induced by accelerating a particle and colliding it with the nuclide.

© 2012 Pearson Education, Inc.

Page 26: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Particle Accelerators

These particle accelerators are enormous, having circular tracks with radii that are miles long.

© 2012 Pearson Education, Inc.

Page 27: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Sample Exercise 21.5 Writing a Balanced Nuclear Equation

Write the balanced nuclear equation for the process summarized as .

Practice ExerciseWrite the condensed version of the nuclear reaction

Page 28: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. Yes, because a neutron has mass and can interact with an electrostatic or magnetic field and is accelerated by an electrostatic or magnetic field.

B. No, because a neutron has no charge and therefore cannot be accelerated by an electrostatic or magnetic field.

Page 29: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

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Kinetics of Radioactive Decay

• Nuclear transmutation is a first-order process.

• The kinetics of such a process, you will recall, obey this equation:

= −kt Nt

N0

ln

© 2012 Pearson Education, Inc.

Page 30: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Kinetics of Radioactive Decay

• The half-life of such a process is

= t1/2 0.693

k

• Comparing the amount of a radioactive nuclide present at a given point in time with the amount normally present, one can find the age of an object.

© 2012 Pearson Education, Inc.

Page 31: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

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A. 25.0 gB. 12.5 gC. 6.25 gD. 3.13 g

Page 32: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Practice ExerciseCarbon-11, used in medical imaging, has a half-life of 20.4 min. The carbon-11 nuclides are formed, and the carbon atoms are then incorporated into an appropriate compound. The resulting sample is injected into a patient, and the medical image is obtained. If the entire process takes five half-lives, what percentage of the original carbon-11 remains at this time?

Sample Exercise 21.6 Calculation Involving Half-Lives

The half-life of cobalt-60 is 5.3 yr. How much of a 1.000-mg sample of cobalt-60 is left after 15.9 yr?

Page 33: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Measuring Radioactivity

• One can use a device like this Geiger counter to measure the amount of activity present in a radioactive sample.

• The ionizing radiation creates ions, which conduct a current that is detected by the instrument.

© 2012 Pearson Education, Inc.

Page 34: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Kinetics of Radioactive Decay

A wooden object from an archeological site is subjected to radiocarbon dating. The activity of the sample that is due to 14C is measured to be 11.6 disintegrations per second. The activity of a carbon sample of equal mass from fresh wood is 15.2 disintegrations per second. The half-life of 14C is 5715 yr. What is the age of the archeological sample?

© 2012 Pearson Education, Inc.

Page 35: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Kinetics of Radioactive Decay

First we need to determine the rate constant, k, for the process:

= t1/2 0.693

k

= 5715 yr 0.693

k

= k 0.693

5715 yr

= k 1.21 104 yr1© 2012 Pearson Education, Inc.

Page 36: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Kinetics of Radioactive Decay

Now we can determine t:

= −kt Nt

N0

ln

= −(1.21 104 yr1)t 11.615.2

ln

= −(1.21 104 yr1)t ln 0.763

= t 2240 yr

© 2012 Pearson Education, Inc.

Page 37: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. Spontaneous radioactive processes have differing reaction mechanisms that do not fit a zero-order or second-order kinetic process.

B. Spontaneous radioactive processes have differing reaction rates that do not fit a zero-order or second-order kinetic process.

C. Spontaneous radioactive processes are either unimolecular or trimolecular processes leading to a first-order or third-order kinetic process.

D. Spontaneous radioactive processes are unimolecular processes leading only to a first-order kinetic process.

Page 38: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. (a) Yes (see equation 21.18)(b) No (see equation 21.20)

B. (a) No (see equation 21.18)(b) Yes (see equation 21.20)

C. (a) No (see equation 21.18)(b) No (see equation 21.20)

D. (a) Yes (see equation 21.18)(b) Yes (see equation 21.20)

Page 39: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A rock contains 0.257 mg of lead-206 for every milligram of uranium-238. The half-life for the decay of uranium-238 to lead-206 is 4.5 × 109 yr. How old is the rock?

Sample Exercise 21.7 Calculating the Age of a Mineral

Practice ExerciseA wooden object from an archeological site is subjected to radiocarbon dating. The activity due to 14C is measured to be 11.6 disintegrations per second. The activity of a carbon sample of equal mass from fresh wood is 15.2 disintegrations per second. The half-life of 14C is 5715 yr. What is the age of the archeological sample?

Page 40: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

If we start with 1.000 g of strontium-90, 0.953 g will remain after 2.00 yr. (a) What is the half-life of strontium-90? (b) How much strontium-90 will remain after 5.00 yr? (c) What is the initial activity of the sample in becquerels and curies?

Sample Exercise 21.8 Calculations Involving Radioactive Decay

Practice ExerciseA sample to be used for medical imaging is labeled with 18F, which has a half-life of 110 min. What percentage of the original activity in the sample remains after 300 min?

Page 41: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. YesB. No. Alpha and beta particles will pass through

matter with equal efficiency but not gamma raysC. No. Alpha particles and gamma rays will pass

through matter with equal efficiency but not beta particles.

D. No. Alpha particles are more readily absorbed by matter than beta particles and gamma rays.

Page 42: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Energy in Nuclear Reactions

• There is a tremendous amount of energy stored in nuclei.

• Einstein’s famous equation, E = mc2, relates directly to the calculation of this energy.

• In the types of chemical reactions we have encountered previously, the amount of mass converted to energy has been minimal.

• However, these energies are many thousands of times greater in nuclear reactions.

© 2012 Pearson Education, Inc.

Page 43: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

Energy in Nuclear Reactions

For example, the mass change for the decay of 1 mol of uranium-238 is 0.0046 g.

The change in energy, E, is then

E = (m)c2

E = (4.6 106 kg)(3.00 108 m/s)2

E = 4.1 1011 J

© 2012 Pearson Education, Inc.

Page 44: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

How much energy is lost or gained when 1 mol of cobalt-60 undergoes beta decay, ? The mass of a atom is 59.933819 amu, and that of a atom is 59.930788 amu.

Sample Exercise 21.9 Calculating Mass Change in a Nuclear Reaction

Practice ExercisePositron emission from 11C, , occurs with release of 2.87 × 1011 J per mole of 11C. What is the mass change per mole of 11C in this nuclear reaction? The masses of 11B and 11C are 11.009305 and 11.011434 amu, respectively.

Page 45: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. The atomic mass of iron-56 is the weighted average of the naturally occurring isotopes of iron-56, not just the mass of the nucleus.

B. The values in Table 21.7 reflect only the mass of the nucleus while the atomic mass of iron-56 also includes the mass of its neutrons.

C. The values in Table 21.7 reflect only the mass of the nucleus while the atomic mass of iron-56 also includes the mass of its electrons.

D. The values in Table 21.7 reflect only the mass of the nucleus while the atomic mass iron-56 also includes the mass of its protons.

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A. Yes, nuclei having mass numbers around 100 are not very stable nuclei.

B. No, nuclei have mass numbers around 100 are among the most stable of nuclei.

Page 47: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

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Nuclear Fission

• How does one tap all that energy?• Nuclear fission is the type of reaction carried

out in nuclear reactors.

© 2012 Pearson Education, Inc.

Page 48: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

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Nuclear Fission

• Bombardment of the radioactive nuclide with a neutron starts the process.

• Neutrons released in the transmutation strike other nuclei, causing their decay and the production of more neutrons.

• This process continues in what we call a nuclear chain reaction.

© 2012 Pearson Education, Inc.

Page 49: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

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Nuclear Fission

Therefore, there must be a certain minimum amount of fissionable material present for the chain reaction to be sustained: critical mass.

© 2012 Pearson Education, Inc.

Page 50: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

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Nuclear Reactors

In nuclear reactors, the heat generated by the reaction is used to produce steam that turns a turbine connected to a generator.

© 2012 Pearson Education, Inc.

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A. To provide sufficient water to condense the secondary coolant after it passes through a turbine

B. To provide a water pond for storage of nuclear wasteC. To provide steam to heat the reactorD. To provide sufficient coolant to cool the entire operating

environment containing the nuclear reactor

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Country: Most Reactors Most Reactors Highest % Operating Construction

A. China United States GermanyB. United States China FranceC. France China RussiaD. China France Canada

Page 53: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

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Nuclear Reactors• The reaction is kept in

check by the use of control rods.

• These rods block the paths of some neutrons, keeping the system from reaching a dangerous supercritical mass.

© 2012 Pearson Education, Inc.

Page 54: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

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Nuclear Fusion

• Fusion would be a superior method of generating power.– The good news is that the

products of the reaction are not radioactive.

– The bad news is that in order to achieve fusion, the material must be in the plasma state at several million kelvins.

© 2012 Pearson Education, Inc.

Page 55: Chapter 21 Nuclear Chemistry © 2012 Pearson Education, Inc

NuclearChemistry

A. Alpha rays are dangerous only when the alpha emitter is near cells inside the body.

B. Alpha rays do not penetrate the exterior skin effectively but once inside the body they are dangerous to cells.

C. Alpha rays need to be close to blood cells to be damaging but other cells inside the body are far less affected.

D. Alpha rays can penetrate the walls of cells inside the body only when the alpha emitter is in direct contact with the cells.

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A. Absorbed dose, 3 rads; effective dosage, 33 rems.B. Absorbed dose, 5 rads; effective dosage, 50 rems.C. Absorbed dose, 10 rads; effective dosage, 100 rems.D. Absorbed dose, 15 rads; effective dosage, 150 rems.