lecture 11 - nassau community college 152/152 lecture 1… ·  · 2012-05-23homer trapped in the...

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1 Copyright © 2009 Charles Hicks Lecture 11 Professor Hicks Inorganic Chemistry (CHE152) Copyright © 2009 Charles Hicks Radioactive decays are all first order processes Copyright © 2009 Charles Hicks Half-Lives of Various Nuclides Nuclide Half-Life Type of Decay Th-232 1.4 x 10 10 yr alpha U-238 4.5 x 10 9 yr alpha C-14 5730 yr beta Rn-220 55.6 sec alpha Th-219 1.05 x 10 6 sec alpha

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Copyright © 2009 Charles Hicks

Lecture 11Professor Hicks

Inorganic Chemistry (CHE152)

Copyright © 2009 Charles Hicks

Radioactive decays are all

first order processes

Copyright © 2009 Charles Hicks

Half-Lives of Various Nuclides

Nuclide Half-LifeType of

Decay

Th-232 1.4 x 1010 yr alpha

U-238 4.5 x 109 yr alpha

C-14 5730 yr beta

Rn-220 55.6 sec alpha

Th-219 1.05 x 10–6 sec alpha

2

Copyright © 2009 Charles Hicks

Copyright © 2009 Charles Hicks

Carbon-14 dating

Earth

Earth’s atmosphere

space

cosmic radiation promotes

Transmutation

of nitrogen-14 to carbon-14

N +147 n1

0 C +146 p1

1

CO2146

photosynthesisC6H12O6

(sugar)

donuts

study the slides on

C-14 for their content

Copyright © 2009 Charles Hicks

Carbon-14 dating

Earth

Earth’s atmosphere

space

eating the donuts makes

Homer slightly radioactive

Rest in

Peace

when Homer dies he stops replenishing the

carbon-14 in his body and the amount that

is there starts to decay

3

Copyright © 2009 Charles Hicks

Carbon-14 dating

• almost all life is part of the same food chain

• plants make sugars

• animals eat plants

• animals eat animals

• %carbon-14 is constant for an organism constantly taking in food

• when they die they stop replenishing carbon-14 and the clock on its decay starts

• t ½ = 5730 years

• [14C] = [14C]initiale-kt

• useful for dating 1000-50,000 years

Copyright © 2009 Charles Hicks

8

Carbon-14 dating% C-14 (compared to living

organism)Object’s Age (in years)

100% 0

90% 870

80% 1850

60% 4220

50% 5730

40% 7580

25% 11,500

10% 19,000

5% 24,800

1% 38,100

Copyright © 2009 Charles Hicks

Kinetics of radioactive decay

• first order process

• [Uranium-238] = [Uranium-238]initiale-kt

• [ ]’s can be replaced with any quantity that

proportional to the amount of element:

mass, moles, volume under constant T, P,

or rate of radiation emission

• Shorter half-lifemore decay per second

- we say the sample is hotter and in many

cases it is at higher temperature

4

Copyright © 2009 Charles Hicks

Example: An ancient skull gives 4.50 particles/min∙gC. If a

living organism gives 15.3 particles/min∙gC, how old is the

skull?

= e-kt

1

2

[C-14]

[C-14]initial

= e-kt1/2

(4.5/15) = e -0.0001209*t

1

2= e-k*5730

k = 1.209 x 10-4 yr-1

= 0.0001209 yr-1

ln(1/2) = -k*5730

t = 9958 yr

1) use half-life t½ to find k 2) use the k value to solve for t

use ratio of rates of particle

emission instead of ratio of [ ]’s

Copyright © 2009 Charles Hicks

Copyright © 2009 Charles Hicks

Mass Defect and

Binding Energy

• when a nucleus forms, some of the mass of the

separate nucleons is converted into energy

• the difference in mass between the separate

nucleons and the combined nucleus is called the

mass defect

• the energy that is released when the nucleus

forms is called the binding energy

E = mc2

Albert Einstein Lise MeitnerLise Meitner

5

Copyright © 2009 Charles Hicks

homer on the

earth’s surface

separated protons, neutrons

homer trapped in the well b/c he

does not have energy to escape

heat

released

heat

released

binding energy = heat released when nucleus forms

it comes from mass energy

binding

energy=

carbon-12

nucleus

+

+

+ N

N

N

+

+

+ N

N

N

+ +

+

+

+

N

N

N

N

N

N

+N

mass

energy

total mass =

12.000000 amu

12.0984 amu

total mass

6 1.00866

+ 6 1.00783

E = mc2

c = speed light

m = mass defect

0.0984 amu here

E = binding energy

Copyright © 2009 Charles Hicks

14

• compare elements binding energy per nucleon

• Iron-56 has the most stable nucleus

• energy will be released when:

Copyright © 2009 Charles Hicks

Calculate the amount of energy released

when a helium-4 nucleus is formed from

two protons and two neutrons. This is also

referred to as the binding energy of a

helium-4 nucleus.

Mass He-4 = 4.00150

Mass Neutron = 1.00866

Mass proton = 1.00728

6

Copyright © 2009 Charles Hicks

Fission/Fusion• a few nuclei are so unstable that

if their nucleus is hit by a neutron, the large nucleus splits into two smaller nuclei - this is called fission

• small nuclei can be smashed together to make a larger nucleus - this is called fusion

• both fission and fusion release enormous amounts of energy– fusion releases more energy per

gram than fission

Lise Meitner

Copyright © 2009 Charles Hicks

Fission

Copyright © 2009 Charles Hicks

where does the energy from

fission/fusion come from?

• during nuclear fission, mass is converted into energy as a more stable nucleus forms

• the energy can be calculated from E=mc2

• U-235 that undergoes fission produces about 1.7 x 1013 J per mole

– a very exothermic chemical reaction produces around 106 J per mole

7

Copyright © 2009 Charles Hicks

Fission Chain Reaction• a chain reaction occurs when a reactant in

the process is also a product of the process

– in fission it is neutrons

– small amount of neutrons start the chain

• many of the neutrons produced in fission are

either ejected from the uranium before they

hit another U-235 or are absorbed by the

surrounding U-238

• minimum amount of fissionable isotope

needed to sustain the chain reaction is called

the critical mass

Copyright © 2009 Charles Hicks

if sample is very dilute most neutrons will escape

- they will not initiate another reaction

if sample is absorbing more than 1 neutron on the

average then the process will very rapidly accelerate

- this is called a Criticality Excursion

Copyright © 2009 Charles Hicks

Criticality excursions

• Samples that are undergoing fission, releasing

neutrons, can experience sudden accelerations

due to nuclear chain reactions

• Caused by

• Precipitations

• Neutrons reflected back

• Change in shape of container

• Powerful bursts of radiation emitted

All increase the number of

emitted neutrons that are

absorbed initiating the next

step of the chain reaction

8

Copyright © 2009 Charles Hicks

Nuclear Power Plants - Core• fissionable material is stored in long tubes,

called fuel rods, arranged in a matrix

• between the fuel rods are control rods

made of neutron absorbing material

– B or Cd

– neutrons needed to sustain the chain reaction

• when the rods are lowered slow down

ejected neutrons, called a moderator

– allows rate of chain reaction to be controlled

Copyright © 2009 Charles Hicks

Nuclear Fusion

Copyright © 2009 Charles Hicks

Fusion

• potentially safer fuels than fission

H2

1H

3

1He

4

2n

1

0+ +

products not radioactive isotopes!tritium relatively safe

t ½ = 12 years

beta decay

problems

1) activation energy is high T ~ 108 K

2) hard to create/control high enough

temperatures

9

Copyright © 2009 Charles Hicks

Fusion

Copyright © 2009 Charles Hicks

heat

released

overall

reaction

(heat absorbed)

Cold Fusion????

Copyright © 2009 Charles Hicks

Describe the effect of raising or lowering

the control rods in a nuclear fission reactor

10

Copyright © 2009 Charles Hicks

Copyright © 2009 Charles Hicks

Estimate the energy released when 1.0 mole of Am-241

undergoes alpha decay.

Mass Am-241 = 241.00471 amu

Mass Np-237 = 236.99715 amu

Mass He-4 = 4.00150 amu

Compare the value you obtain to the amount of energy obtained

from combustion of 1 mole of octane 5.0 x106 J/mol

Copyright © 2009 Charles Hicks

Example: If you have a 1.35 mg sample of Pu-236,

calculate the mass that will remain after 5.00 years

Pu-236 has a half life of 2.86 yr

1) use half-life t½ to find k 2) use the k value and the t of interest

to solve for mass at that time

11

Copyright © 2009 Charles Hicks

Blocking radiation

• An elements ability to block X-rays

increases with nuclear size (Z)

• Pb is often used as shielding because it is

almost the heaviest element that is not

radioactive itself

• Soft body tissue is mostly H2O, which is

mostly O-16 by mass

• Bone and cartilige contain substantial

amounts of Ca and P which are larger

nuclei absorb more radiation

Copyright © 2009 Charles Hicks

X-ray imaging• Medical x-rays are of the “shadows” of

denser body tissue – bones, cartilage, etc

X-ray

source

Copyright © 2009 Charles Hicks

CT Scans

• Series of x-rays used to construct a 3-

dimensional image

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Copyright © 2009 Charles Hicks

PET Scan

• imaging technique based on positron emission

positron + electron gamma rays

• isotope incorporated into a molecule

• molecule ingested

• positrons emitted from places molecule is concentrated

• gives a three dimensional “x-ray” of the region the molecule binds

• example F-18 labeled drugs that bind in the brain’s addiction centers

- F-18 labeled cocaine, heroine

Copyright © 2009 Charles Hicks

Barium

Enema

• radiation absorption increases with size of nucleus

• bones Ca, P causes them to absorb more than

soft tissue mostly H, O, C, N

• colon can be imaged with x-rays if it is filled with

BaSO4 because Ba absorbs X-rays well

Copyright © 2009 Charles Hicks

Radiation therapy

• Cancerous tumors dosed with radiation

• Can be performed with focused beams, or

• “seeding” radioactive material near the

tumor, or

• Molecules labeled with radioactive

isotopes that target specific organs

• Radiotherapy works by damaging the

DNA of the cancer cells

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Copyright © 2009 Charles Hicks

Radiation therapy

External beam radiation therapy

• Cobalt-60 often used as a source of

radiation

• It is a beta emitter

• beam is focused on

the site of the tumor

Copyright © 2009 Charles Hicks

Radiation therapy

Internal radiotherapy• I naturally accumulates in the thyroid gland

• I-131 is radioactive and can be used to treat

thyroid cancer

• I-131 after being ingested a NaI-131

accumulates in thyroid where it undergoes -

decay dosing the thyroid cancer

Non-radioactive iodine is eaten to prevent damage to the

thyroid caused by I-131 released from nuclear bombs or

accidents

It works by flooding the body with I- so that most of the I-

at the thyroid gland is not radioactive

Copyright © 2009 Charles Hicks

Radiation therapy

Internal radiotherapy• Prostate cancer treated with radioactive seeds

• Palladium-103 is an example of a seed material

• It has t½ = 17 days

• decays by electron capture emitting gamma rays

Pd-103 seeds

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Copyright © 2009 Charles Hicks

Dangers of Radioactivity• high energy radioactive decay products called

Ionizing Radiation

• Ionizing radiation can directly cleave DNA

- called primary damage, or

- can break molecules up forming species that

cause damage by chemical reactions

- called secondary damage

• most common secondary pathway is water

absorbing radiation forming hydroxyl radicals

• radical = odd number of electrons

• Very reactive and an oxidizing agent

OH

Copyright © 2009 Charles Hicks

Relative Biological Effectiveness

(at causing damage)

Type and Energy Range Relative Biological Effectiveness

X and Gamma rays 1

Electrons 1

Neutrons (energy dependent) 10

Protons 5

Alpha Particles 20

you will be provided with this table on the exam

Copyright © 2009 Charles Hicks

Dose

• amount of energy absorbed in an exposure has a unit

called the gray (Gr)

1 gray =1 Joule

kg tissue

gray is a large unit for typical exposures

A more common unit is the Radiation Absorbed Dose (RAD)

0.01 gray = 1 RAD

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Copyright © 2009 Charles Hicks

REM’s

dose in REM = dose in RAD x RBE

• unit used to measure total risk associated with a dose

• accounts for differences in extent of damage caused

by different particle types

dose (REM) effect

5 none felt, yearly limit radiation workers

50 none felt, red blood cell count lowered

1000 near 100% fatal

• typical x-ray deliver 1-100 mREM

• background level is 30-60 mREM per year

• barium enema recently? you got 400 mREM

Copyright © 2009 Charles Hicks

Factors besides size of dose• Getting a dose in regions that are mostly

muscle (legs, arms) is much less dangerous

than the same dose in your organs

• Distributing a dose over time is much less

damaging

• Cells have repair mechanisms

• If repair can keep up much less damage can

accumulate

- DNA single strand breaks are repairable

- Double strand breaks – not very repairable

Copyright © 2009 Charles Hicks

Dangers of radiation and

penetrating power

• gamma radiation strongly penetrating requires thick layers of most protecting materials

• without protection dangerous doses quickly delivered

• and emitters easy to block

• and emitters very dangerous if ingested since they can deliver large doses accumulated over time

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Copyright © 2009 Charles Hicks

Why do beta emitters not have to be kept

in a thick-walled lead containers, but

precautions must be taken to prevent

ingesting them?

Copyright © 2009 Charles Hicks

Calculate how many REMs were delivered

in 10 barium enemas if the dose for each

barium enema is 0.40 RAD

Copyright © 2009 Charles Hicks

How many RAD of alpha particles could a

radiation worker be dosed with before they

reached their yearly safety limit of 5.0

REM?