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25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Chapter 25

Nuclear Chemistry

25.1 Nuclear Radiation

25.2 Nuclear Transformations

(2)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

What is the source of radon in homes?

CHEMISTRY & YOU

CHEMISTRY & YOU

Radon may

accumulate in a

basement that is

not well ventilated.

Test kits are

available to

measure the

(3)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

Nuclear Stability and Decay

(4)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

The

nuclear force

is an attractive force

that acts between

all

nuclear particles that

are extremely close together, such as

(5)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

The

nuclear force

is an attractive force

that acts between

all

nuclear particles that

are extremely close together, such as

protons and neutrons in a nucleus.

(6)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

The stability of a nucleus depends on the

ratio of neutrons to protons.

Interpret Data

Interpret Data

• This graph shows the number of

neutrons vs. the number of

(7)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

The stability of a nucleus depends on the

ratio of neutrons to protons.

Interpret Data

Interpret Data

• The region of the graph in which these points are located is called the band of

(8)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

The stability of a nucleus depends on the

ratio of neutrons to protons.

Interpret Data

Interpret Data

• For elements of low atomic number

(below about 20), this ratio is about 1. • Above atomic

number 20, stable nuclei have more neutrons than

(9)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

A nucleus may be unstable and undergo

spontaneous decay for different reasons.

The neutron-to-proton ratio in a

(10)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

Some nuclei are unstable because they

have too many neutrons relative to the

number of protons.

• When one of these nuclei decays, a neutron

(11)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

Some nuclei are unstable because they

have too many neutrons relative to the

number of protons.

• When one of these nuclei decays, a neutron

emits a beta particle (fast-moving electron) from the nucleus.

– A neutron that emits an electron becomes a proton.

n

1

0 p +

1

1 e

(12)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

Some nuclei are unstable because they

have too many neutrons relative to the

number of protons.

• When one of these nuclei decays, a neutron

emits a beta particle (fast-moving electron) from the nucleus.

– A neutron that emits an electron becomes a proton.

n

1

0 p +

1

1 e

0 –1

– This process is known as beta emission. – It increases the number of protons while

(13)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

Radioisotopes that undergo beta emission

include the following.

Cu

66

29 Zn +

66

30 e

0 –1

C

14

6 N +

14

7 e

(14)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

Other nuclei are unstable because they

have too few neutrons relative to the

number of protons.

• These nuclei increase their stability by converting a proton to a neutron.

– An electron is captured by the nucleus during this process, which is called electron capture.

Co

59 27

Ni + e

59 28 0 –1 Cl 37 17

Ar + e

37 18

(15)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

A

positron

is a particle with the mass of an

electron but a positive charge.

• Its symbol is e.

• During positron emission, a proton changes to a neutron, just as in electron capture.

0 +1

B

8

5 Be +

8 4 e 0 +1 O 15

8 N +

15

7 e

0 +1

– When a proton is converted to a neutron, the

(16)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

Nuclei that have an atomic number greater

than 83 are radioactive.

• These nuclei have both too many neutrons and too many protons to be stable.

– Therefore, they undergo radioactive decay.

– Alpha emission increases the neutron-to-proton ratio, which tends to increase the stability of the nucleus.

(17)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

In alpha emission, the mass number

decreases by four and the atomic number

decreases by two.

Ra

226

88 Rn + He

222 86

4 2

Th

232

90 Ra + He

228 88

(18)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Nuclear Stability and DecayNuclear Stability and Decay

Recall that conservation of mass is an

important property of chemical reactions.

• In contrast, mass is not conserved during nuclear reactions.

(19)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

During nuclear decay, if the atomic

number decreases by one but the mass

number is unchanged, the radiation

emitted is

A.

a positron.

B.

an alpha particle.

C.

a beta particle.

(20)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

During nuclear decay, if the atomic

number decreases by one but the mass

number is unchanged, the radiation

emitted is

A. a positron.

B.

an alpha particle.

C.

a beta particle.

(21)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Half-LifeHalf-Life

Half-Life

(22)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

1 2

A

half-life

(t ) is the time required for

one-half of the nuclei in a radioisotope sample

to decay to products.

Interpret Graphs

Interpret Graphs

After each half-life, half of the original

(23)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Half-LifeHalf-Life

Half-lives can be as short as a second or as long as billions of years.

Half-Lives of Some Naturally Occurring Radioisotopes

Isotope Half-life Radiation emitted

Carbon-14 5.73 × 103 years

Potassium-40 1.25 × 109 years 

Radon-222 3.8 days  Radium-226 1.6 × 103 years 

Thorium-234 24.1 days 

Uranium-235 7.0 × 108 years 

Uranium-238 4.5 × 109 years

(24)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Half-LifeHalf-Life

• Scientists use half-lives of some long-term

radioisotopes to determine the age of ancient objects.

• Many artificially produced radioisotopes have short half-lives, which makes them useful in nuclear medicine.

– Short-lived isotopes are not a long-term radiation hazard for patients.

(25)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Half-LifeHalf-Life

Comparing Half-Lives

• The age of

uranium-containing minerals can be estimated by measuring the ratio of uranium-238 to

lead-206.

• Because the half-life of uranium-238 is 4.5 × 109 years, it is possible to use its half-life to date rocks as old as the solar system.

(26)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Uranium compounds are found in

rocks and in soils that form from these

rocks. How can these uranium

compounds lead to a buildup of radon

in homes and other buildings?

CHEMISTRY & YOU

(27)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Uranium compounds are found in

rocks and in soils that form from these

rocks. How can these uranium

compounds lead to a buildup of radon

in homes and other buildings?

CHEMISTRY & YOU

CHEMISTRY & YOU

Radon gas is a product of the decay of

uranium. As the uranium compounds in

the soil beneath homes and buildings

(28)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Half-LifeHalf-Life

Radiocarbon Dating

Plants use carbon dioxide to produce

carbon compounds, such as glucose.

• The ratio of carbon-14 to other carbon isotopes is constant during an organism’s life.

• When an organism dies, it stops exchanging carbon with the environment and its radioactive C atoms decay without being replaced.

• Archaeologists can use this data to estimate when an organism died.

(29)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Half-LifeHalf-Life

Exponential Decay Function

A stands for the amount remaining.

A0 stands for the initial amount.

n stands for the number of half-lives.

You can use the following equation to

calculate how much of an isotope will

remain after a given number of half-lives.

A

=

A

0

1

2

(30)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Half-LifeHalf-Life

• The exponent n indicates how many times A0

must be multiplied by to determine 12 A.

A

=

A

0

1

2

n

(31)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Half-LifeHalf-Life

Decay of Initial Amount (A0) of Radioisotope

Half-Life Amount Remaining

0 A0 × ( )0 = A 0

1 A0 × ( )1 = A

0 ×

2 A0 × ( )2 = A

0 × ×

This table shows examples in which

n

= 1 and

n

= 2.

Exponential Decay Function

1 2 1 2 1 2 1 2 1

(32)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Using Half-Lives in Calculations

Sample Problem 25.1

Sample Problem 25.1

Carbon-14 emits beta radiation and decays with a half-life (t ) of 5730 years. Assume that you start

with a mass of 2.00 × 10–12 g of carbon-14.

1 2

a. How long is three half-lives?

b. How many grams of the

(33)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

KNOWNS UNKNOWNS

3 half-lives = ? years

mass remaining = ? g

Analyze List the knowns and the unknowns.

1

Sample Problem 25.1

Sample Problem 25.1

• To calculate the length of three half-lives, multiply the half-life by three.

• To find the mass of the radioisotope

remaining, multiply the original mass by for each half-life that has elapsed.

1 2

t = 5730 years

initial mass (A0) = 2.00 × 10–12 g

number of half-lives (n) = 3

(34)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

a. Multiply the half-life of carbon-14 by

the total number of half-lives.

Calculate Solve for the unknowns.

2

Sample Problem 25.1

Sample Problem 25.1

t × 1 n = 5730 years × 3 = 17,190 years

(35)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Calculate Solve for the unknowns.

2

Sample Problem 25.1

Sample Problem 25.1

b. The initial mass of carbon-14 is

reduced by one-half for each half-life. So, multiply by three times.1

2

Remaining mass = 2.00 × 10–12 g × × ×1

2 12 12

(36)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Calculate Solve for the unknowns.

2

Sample Problem 25.1

Sample Problem 25.1

b. You can get the same answer by

using the equation for an exponential decay function.

= (2.00 × 10–12 g)

= 0.250 × 10–12 g

= 2.50 × 10–13 g

A = A0

( )

1 = (2.00 × 10–12 g)

2

n

( )

1 2

3

(37)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Evaluate

Do the results make sense?

3

Sample Problem 25.1

Sample Problem 25.1

• The mass of carbon-14 after three half-lives should be one-eighth of the original mass.

(38)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

The half-life of phosphorus-32 is

(39)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

The half-life of phosphorus-32 is

14.3 days. How many milligrams of

phosphorus-32 remain after 100.1

days if you begin with 2.5 mg of the

radioisotope?

n = 100.1 days × = 7 half-lives 1 half-life14.3 days

= (2.5 mg) = 2.0 × 10–2 mg

A = A0

( )

12 = (2.5 mg) n

( )

12 7

( )

1

(40)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

Transmutation Reactions

(41)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

For thousands of years, alchemists tried to

change lead into gold.

• What they wanted to achieve is

transmutation, or the conversion of an atom of one element into an atom of another

(42)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

Transmutation can occur by radioactive

decay, or when particles bombard the

nucleus of an atom.

(43)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

Ernst Rutherford performed the earliest

artificial transmutation in 1919.

• He bombarded nitrogen gas with alpha particles.

• The unstable fluorine atoms quickly decay to form a stable isotope of oxygen and a proton.

O +

17 8 p 1 1 F 18 9 Proton Oxygen-17 Fluorine-18

N +

(44)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

Rutherford’s experiment eventually led to

the discovery of the proton.

• He and other scientists noticed a pattern as they did different transmutation experiments. Hydrogen nuclei were emitted.

• Scientists realized that these hydrogen nuclei (protons) must have a fundamental role in atomic structure.

He Alpha particle N Nitrogen atom F Unstable fluorine atom O Oxygen P Proton 4

(45)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

James Chadwick’s discovery of the neutron

in 1932 also involved a transmutation

experiment.

• Neutrons were produced when beryllium-9 was bombarded with alpha particles.

C +

12 6 n 1 0 Neutron Carbon-12

Be +

(46)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

Elements with atomic numbers above 92,

the atomic number of uranium, are called

transuranium elements

.

• None of these elements occurs in nature. • All of them are radioactive.

(47)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

Transuranium elements are synthesized in nuclear reactors and nuclear accelerators.

• Reactors produce beams of low-energy particles.

• Accelerators are used to increase the speed of bombarding

particles to very high speeds.

(48)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

• When uranium-238 is bombarded with the relatively slow neutrons from a nuclear reactor, some uranium nuclei capture these neutrons. The product is uranium-239.

• Uranium-239 is radioactive and emits a beta particle. The other product is an isotope of the artificial

radioactive element neptunium (atomic number 93).

• Neptunium is unstable and decays, emitting a beta particle and a second artificial element, plutonium (atomic number 94).

Np +

239 93 e 0 –1 U 239 92

U +

238 92 n 1 0 U 239 92

Pu +

(49)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Transmutation ReactionsTransmutation Reactions

Scientists in Berkeley, California,

synthesized the first two artificial elements

in 1940.

• Since that time, more than 20 additional

(50)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Which of the following always changes

when transmutation occurs?

A.

The number of electrons

B.

The mass number

C.

The atomic number

(51)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Which of the following always changes

when transmutation occurs?

A.

The number of electrons

B.

The mass number

C. The atomic number

(52)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Key ConceptsKey Concepts

The neutron-to-proton ratio in a

radioisotope determines the type of decay that occurs.

After each half-life, half of the original

radioactive atoms have decayed into atoms of a new element.

(53)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Key EquationKey Equation

A

=

A

0

1

2

(54)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Glossary TermsGlossary Terms

nuclear force: an attractive force that acts

between all nuclear particles that are

extremely close together, like protons and

neutrons in a nucleus

band of stability: the location of stable nuclei on a neutron-vs.-proton plot

(55)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations > Glossary TermsGlossary Terms

half-life: the time required for one-half of the nuclei of a radioisotope sample to decay to products

transmutation: the conversion of an atom of

one element to an atom of another element

(56)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

Electrons and the Structure of Atoms

• Unstable atomic nuclei decay by emitting alpha or beta particles.

• Often gamma rays are emitted.

(57)

25.2 Nuclear Transformations >

25.2 Nuclear Transformations >

END OF 25.2

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