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Nuclear Physics and Radioactivity Lecture 23 Ch 30-31 Mural painted on the birthplace of Marie Curie in Warsaw, in 2011. To mark the 100 th anniversary of her second Nobel prize, which she shared with her daughter Irene.
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Page 1: Nuclear Physics and Radioactivity - Piazza

Nuclear Physics

and

Radioactivity

Lecture 23

Ch 30-31

Mural painted on the birthplace of Marie Curie in Warsaw, in 2011. To mark the 100th anniversary of her second Nobel prize, which she shared with her daughter Irene.

Page 2: Nuclear Physics and Radioactivity - Piazza

30.8 Half-Life and Rate of Decay

Nuclear decay is a random process; the decay of any nucleus is not influenced by the decay of any other.

Page 3: Nuclear Physics and Radioactivity - Piazza

30.8 Half-Life and Rate of Decay •  The number of decays in a short time interval is

proportional to the number of nuclei present

•  Where λ is the probability that a given nucleus will decay at any particular instant.

•  λ is often called the called the decay constant.

•  If we have a known amount of an element, and a geiger counter, we can easily compute λ from its activity.

Lets do a simple example…..

(30-3a)

Page 4: Nuclear Physics and Radioactivity - Piazza

PET scan – positron emission tomography

O15 decay probability λ=0.00569 If the patient eats glucose containing 1mg of this isotope, What will be her activity A.  Initially?

B.  After one minute?

C.  After one hour? D.  After 2 hours?

Page 5: Nuclear Physics and Radioactivity - Piazza

Positron Emission Tomography (PET)

Page 6: Nuclear Physics and Radioactivity - Piazza

30.8 Half-Life and Rate of Decay

The previous equation can be solved, using calculus, for N as a function of time to give the exponential radioactive decay law

(30-4)

Page 7: Nuclear Physics and Radioactivity - Piazza

PET scan – positron emission tomography

O15 decay probability λ=0.00569 If the patient eats glucose containing 1mg of this isotope, What will be her activity A.  Initially?

B.  After one minute?

C.  After one hour? D.  After 2 hours?

Page 8: Nuclear Physics and Radioactivity - Piazza

30.8 Half-Life and Rate of Decay The half-life is the time it takes for half the nuclei in a given sample to decay. It is related to the decay constant:

Substituting into the previous eqn, it can be shown that there are 2 equivalent equations:

N = N0 2-t/t

(30-6)

1/2

Page 9: Nuclear Physics and Radioactivity - Piazza

30.8 Half-Life and Rate of Decay

N = N0 2-t/t

Page 10: Nuclear Physics and Radioactivity - Piazza

You have 16 kg of a radioactive sample with a certain half-life of 30 years. How much is left after 90 years?

(1) 8 kg

(2) 4 kg

(3) 2 kg

(4) 1 kg

(5) nothing

ConcepTest 30.8a Radioactive Decay Law I

Page 11: Nuclear Physics and Radioactivity - Piazza

The total time (90 years) is 3 half-lives. After one half-life ⇒ 8 kg left. After two half-lives ⇒ 4 kg left. After three half-lives ⇒ 2 kg left.

You have 16 kg of a radioactive sample with a certain half-life of 30 years. How much is left after 90 years?

(1) 8 kg

(2) 4 kg

(3) 2 kg

(4) 1 kg

(5) nothing

ConcepTest 30.8a Radioactive Decay Law I

Follow-up: When will the sample be reduced to nothing?

Page 12: Nuclear Physics and Radioactivity - Piazza

30.10 Decay Series

One unstable radioactive element decays into another,

and so on….

For a given starting point there may be

multiple generations of unstable daughter

nuclei

Form the relative abundance of the

parent and daughters, accurate dates can be

calculated

E.g. the age of the Earth

Page 13: Nuclear Physics and Radioactivity - Piazza

30.11 Radio-Carbon Dating •  Radioactive dating can be done by analyzing the fraction of carbon in organic material that is carbon-14.

•  The ratio of carbon-14 to carbon-12 in the atmosphere has been roughly constant over thousands of years. A living plant or tree will be constantly exchanging carbon with the atmosphere, and will have the same carbon ratio in its tissues.

•  When the plant dies, this exchange stops. Carbon-14 has a half-life of about 5730 years; it gradually decays away and becomes a smaller and smaller fraction of the total carbon in the plant tissue.

•  This fraction can be measured, and the age of the tissue deduced.

Page 14: Nuclear Physics and Radioactivity - Piazza

• Objects older than about 60,000 years (> ten half-lives) cannot be dated this way – there is too little carbon-14 left.

•  Carbon 14 is produced by the solar wind splitting atoms in the upper atmosphere (the same mechanism as the Aurora Borealis)

•  Variations in the Sun, and Earth’s magnetic Field cause the rate of C14 production to vary slightly.

•  Atmospheric Nuclear Weapons use/testing greatly elevated the C14 rate for a while.

Page 15: Nuclear Physics and Radioactivity - Piazza

30.11 Radioactive Dating

Other isotopes are useful for geologic time scale dating.

Uranium-238 has a half-life of 4.5 x 109 years, and has been used to date the oldest rocks on Earth as about 4 billion years old.

Page 16: Nuclear Physics and Radioactivity - Piazza

Leona Woods (August 9, 1919 – November 10, 1986), was an American physicist who helped build the first nuclear reactor and the first atomic bomb. After WW2 she became interested in ecological and environmental issues, and devised the method of using the isotope ratios of in tree rings to study changes in temperature and rainfall patterns hundreds of years before records were kept, opening the door to the study of climate change

More advanced variations of radioactive dating have been developed

Page 17: Nuclear Physics and Radioactivity - Piazza

30.13 Detection of Radiation A cloud chamber contains a supercooled gas; when a charged particle goes through, droplets form along its track. Similarly, a bubble chamber contains a superheated liquid, and it is bubbles that form. In either case, the tracks can be photographed and measured.

Page 18: Nuclear Physics and Radioactivity - Piazza

Summary of Chapter 30

•  Nuclei contain protons and neutrons – nucleons

•  Total number of nucleons, A, is atomic mass number

•  Number of protons, Z, is atomic number

•  Isotope notation:

•  Nuclear masses are measured in u; carbon-12 is defined as having a mass of 12 u

Page 19: Nuclear Physics and Radioactivity - Piazza

Summary of Chapter 30

•  Difference between mass of nucleus and mass of its constituents is binding energy

•  Unstable nuclei decay through alpha, beta, or gamma emission

•  An alpha particle is a helium nucleus; a beta particle is an electron or positron; a gamma ray is a highly energetic photon

•  Nuclei are held together by the strong nuclear force; the weak nuclear force is responsible for beta decay

Page 20: Nuclear Physics and Radioactivity - Piazza

Summary of Chapter 30

•  Electric charge, linear and angular momentum, mass-energy, and nucleon number are all conserved

•  Radioactive decay is a statistical process

•  The number of decays per unit time is proportional to the number of nuclei present:

•  The half-life is the time it takes for half the nuclei to decay

Page 21: Nuclear Physics and Radioactivity - Piazza

What weighs more, an electron and a proton, or a hydrogen atom?

1) electron and proton

2) hydrogen atom

3) both the same

ConcepTest 30.2a Binding Energy I

Page 22: Nuclear Physics and Radioactivity - Piazza

What weighs more, an electron and a proton, or a hydrogen atom?

1) electron and proton

2) hydrogen atom

3) both the same

ConcepTest 30.2a Binding Energy I

The total energy (or mass) of a hydrogen atom must be less than the energies (or masses) of the electron plus the proton individually in order for the electron to be bound.

Page 23: Nuclear Physics and Radioactivity - Piazza

1) the 2 neutrons and 1 proton 2) the tritium nucleus 3) they both weigh the same 4) it depends on the specific isotope of tritium

On a balance scale, you put 2 neutrons and 1 proton on one side and you put a tritium nucleus (3H) on the other. Which side weighs more?

ConcepTest 30.2c Binding Energy III

Page 24: Nuclear Physics and Radioactivity - Piazza

The mass of the 2 neutrons and 1 proton is less when they are bound together as tritium. The mass difference is the binding energy.

need to add 8.5 MeV to balance scale

1) the 2 neutrons and 1 proton 2) the tritium nucleus 3) they both weigh the same 4) it depends on the specific

isotope of tritium

On a balance scale, you put 2 neutrons and 1 proton on one side and you put a tritium nucleus (3H) on the other. Which side weighs more?

ConcepTest 30.2c Binding Energy III

Page 25: Nuclear Physics and Radioactivity - Piazza

1) removing a proton takes more energy 2) removing a neutron takes more energy 3) both take the same amount of energy

Does it take more energy to remove one proton or one neutron from 16O?

ConcepTest 30.3 Separation Energy

Page 26: Nuclear Physics and Radioactivity - Piazza

Removing a proton takes less energy because the repulsive Coulomb force between positively charged protons helps to push the proton out of the nucleus. Remember that neutrons are uncharged.

1) removing a proton takes more energy 2) removing a neutron takes more energy 3) both take the same amount of energy

Does it take more energy to remove one proton or one neutron from 16O?

ConcepTest 30.3 Separation Energy

Page 27: Nuclear Physics and Radioactivity - Piazza

A radioactive nucleus undergoes gamma decay. How large would you expect the energy of the emitted photon to be?

1) less than 13.6 eV 2) 13.6 eV 3) hundreds of eV 4) millions of eV 5) billions of eV

ConcepTest 30.5 Radioactive Decay Energy

Page 28: Nuclear Physics and Radioactivity - Piazza

The binding energy of nuclei is of the order several MeV (millions of eV). So, we would expect the energy of gamma decay to be in the same ballpark.

A radioactive nucleus undergoes gamma decay. How large would you expect the energy of the emitted photon to be?

1) less than 13.6 eV 2) 13.6 eV 3) hundreds of eV 4) millions of eV 5) billions of eV

ConcepTest 30.5 Radioactive Decay Energy

Follow-up: What process could release a photon with billions of eV?

Page 29: Nuclear Physics and Radioactivity - Piazza

What element results when 14C undergoes beta decay?

1) 15C

2) 15N

3) 14C

4) 14N

5) 15O

ConcepTest 30.7 Beta Decay

Page 30: Nuclear Physics and Radioactivity - Piazza

The reaction is: neutrinoeNC 14

7

14

6 ++→ −

What element results when 14C undergoes beta decay?

1) 15C

2) 15N

3) 14C

4) 14N

5) 15O

Inside the nucleus, the reaction n → p + e- + ν has occurred, changing a neutron into a proton, so the atomic number Z increases by 1. However the mass number (A = 14) stays the same.

ConcepTest 30.7 Beta Decay

Follow-up: How would you turn 14C into 15N?

Page 31: Nuclear Physics and Radioactivity - Piazza

You have 12 kg of a radioactive substance. Ten years later, you find that you only have 3 kg left. Find the half-life of the material.

(1) 20 years

(2) 10 years

(3) 7.5 years

(4) 5 years

(5) 2.5 years

ConcepTest 30.8b Radioactive Decay Law II

Page 32: Nuclear Physics and Radioactivity - Piazza

After one half-life ⇒ 6 kg left. After two half-lives ⇒ 3 kg left. So if the total time is 10 years, then the half-life must be 5 years.

(2 half-lives = 10 years)

You have 12 kg of a radioactive substance. Ten years later, you find that you only have 3 kg left. Find the half-life of the material.

(1) 20 years

(2) 10 years

(3) 7.5 years

(4) 5 years

(5) 2.5 years

ConcepTest 30.8b Radioactive Decay Law II

Follow-up: How much of the sample is left after another 10 years?

Page 33: Nuclear Physics and Radioactivity - Piazza

You have 400 g of a radioactive sample with a half-life of 20 years. How much is left after 50 years?

1) more than 100 g

2) 75 - 100 g

3) 75 g

4) 50 - 75 g

5) less than 50 g

ConcepTest 30.8c Radioactive Decay Law III

Page 34: Nuclear Physics and Radioactivity - Piazza

You have 400 g of a radioactive sample with a half-life of 20 years. How much is left after 50 years?

Total time (50 years) is 2 1/2 half-lives. After one half-life ⇒ 200 g left After two half-lives ⇒ 100 g left. After three half-lives ⇒ 50 g left. So after 2 1/2 half-lives ⇒ 75 g left ?

No!! Exponential function is not linear!

⇒ 70.7 g left N = Noe–(0.693 / T1/2)t

1) more than 100 g

2) 75 - 100 g

3) 75 g

4) 50 - 75 g

5) less than 50 g

ConcepTest 30.8c Radioactive Decay Law III

Page 35: Nuclear Physics and Radioactivity - Piazza

You have 10 kg each of a radioactive sample A with a half-life of 100 years, and another sample B with a half-life of 1000 years. Which sample has the higher activity?

1) sample A

2) sample B

3) both the same

4) impossible to tell

ConcepTest 30.9a Activity and Half-Life I

Page 36: Nuclear Physics and Radioactivity - Piazza

If a sample has a shorter half-life, this means that it decays more quickly (larger decay constant λ) and therefore has a higher activity:

In this case, that is sample A.

You have 10 kg each of a radioactive sample A with a half-life of 100 years, and another sample B with a half-life of 1000 years. Which sample has the higher activity?

1) sample A

2) sample B

3) both the same

4) impossible to tell

ConcepTest 30.9a Activity and Half-Life I

ΔN/Δt = –λ N

Follow-up: What is the ratio of activities for the two samples?

Page 37: Nuclear Physics and Radioactivity - Piazza

Which type of radiation goes farther in matter before losing all of its energy ?

1) alpha radiation

2) beta radiation

3) gamma radiation

4) all about the same distance

ConcepTest 31.6 Radiation Shielding

Page 38: Nuclear Physics and Radioactivity - Piazza

α

β

γ

paper aluminum lead

Alpha particles have such a large charge, they ionize many atoms in a short distance, and so lose their energy rapidly and stop. Gamma rays travel great distances before ionizing an atom.

Which type of radiation goes farther in matter before losing all of its energy ?

1) alpha radiation

2) beta radiation

3) gamma radiation

4) all about the same distance

ConcepTest 31.6 Radiation Shielding

Page 39: Nuclear Physics and Radioactivity - Piazza

Curly is twice as far from a small radioactive source as Moe. Compared to Curly’s position, the intensity of the radiation (and therefore exposure) at Moe’s position is about:

1) one-quarter 2) one-half 3) the same 4) double 5) quadruple

Curly Moe radioactive source

ConcepTest 31.7a Radiation Exposure I

Page 40: Nuclear Physics and Radioactivity - Piazza

A small source can be treated as a point source and so it obeys the inverse square law of intensity. Twice as close means 4 times the intensity (and therefore exposure).

Curly is twice as far from a small radioactive source as Moe. Compared to Curly’s position, the intensity of the radiation (and therefore exposure) at Moe’s position is about:

1) one-quarter 2) one-half 3) the same 4) double 5) quadruple

Curly Moe radioactive source

ConcepTest 31.7a Radiation Exposure I

Page 41: Nuclear Physics and Radioactivity - Piazza

Curly is working 5 m from a highly radioactive source and must reduce his exposure by at least a factor of 10. Assuming that an inverse square law (1/r2) applies in this case, to what distance should he move?

1) 7.5 m

2) 10 m

3) 15 m

4) 20 m

5) 50 m

Curly radioactive source

ConcepTest 31.7b Radiation Exposure II

Page 42: Nuclear Physics and Radioactivity - Piazza

A small source can be treated like a point source and so it obeys the inverse square law of intensity. Moving to 15 m (3 times farther) only reduces the exposure by 9 times. He has to move farther away (20 m) in order to get a factor of 16 reduction, which meets the “safety limit” of 10 times.

Curly is working 5 m from a highly radioactive source and must reduce his exposure by at least a factor of 10. Assuming that an inverse square law (1/r2) applies in this case, to what distance should he move?

1) 7.5 m

2) 10 m

3) 15 m

4) 20 m

5) 50 m

Curly radioactive source

ConcepTest 31.7b Radiation Exposure II

Page 43: Nuclear Physics and Radioactivity - Piazza

Radiation can damage matter such as metals or biological tissue by:

1) heating up the material

2) causing cancer in the metal

3) producing fission reactions in the material

4) removing electrons from the atoms

5) producing fusion reactions in the material

ConcepTest 31.8 Radiation Damage

Page 44: Nuclear Physics and Radioactivity - Piazza

Radiation can ionize the atoms in matter, which means knocking out electrons. Metals become brittle and cell processes can be disrupted.

Radiation can damage matter such as metals or biological tissue by:

1) heating up the material

2) causing cancer in the metal

3) producing fission reactions in the material

4) removing electrons from the atoms

5) producing fusion reactions in the material

ConcepTest 31.8 Radiation Damage

Follow-up: What type of radiation will tend to do the most damage?