5.1 an introduction to nuclear nuclear reactions

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Nuclear Reactions: Chemistry 5.1 AN INTRODUCTION TO NUCLEAR CHEMISTRY

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Page 1: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Nuclear Reactions:

Chemistry

5.1 AN INTRODUCTION TO NUCLEAR CHEMISTRY

Page 2: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Discovery of Radioactivity

Page 3: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Roentgen

● In 1895 Wilhelm Konrad Roentgen discovered X-rays.

• Roentgen observed that a vacuum discharge tube enclosed in a thin, black cardboard box had caused a nearby piece of paper coated with the salt barium platinocyanide to phosphorescence.

Page 4: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Roentgen

● From this and other experiments he concluded that certain rays, which he called X-rays, were emitted from the discharge tube, penetrated the box, and caused the salt to glow.

Page 5: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Becquerel

● Shortly after Roentgen’s discovery, Antoine Henri Becquerel attempted to show a relationship between X-rays and the phosphorescence of uranium salts.

• Becquerel wrapped a photographic plate in black paper, sprinkled a sample of a uranium salt on it, and exposed it to sunlight.

Page 6: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Becquerel

● When Becquerel attempted to repeat the experiment the sunlight was intermittent.

• He took the photographic plate wrapped in black paper with the uranium sample on it, and placed the whole setup in a drawer.

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Becquerel

● Several days later he developed the film and was amazed to find an intense image of the uranium salt on the plate.

• He repeated the experiment in total darkness with the same result.

Page 8: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Radioactivity is the spontaneous emission of particles and/or rays from the nucleus of an atom.

Becquerel

● This proved that the uranium salt emitted rays that affected the photographic plate, and that these rays were not a result of phosphorescence due to exposure to sunlight.

Elements having this property are radioactive.

• One year later, in 1896, Marie Curie coined the name radioactivity.

Page 9: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Rutherford● In 1899 Rutherford began to investigate the

nature of the rays emitted by uranium.

• He found two particles in the rays. He called them alpha and beta particles.

• Rutherford’s nuclear atom description led scientists to attribute the phenomenon of radioactivity to reactions taking place in the nuclei of atoms.

• In 1899, when testing Uranium, he realized it emitted particles changing into another element.

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Villiard

● The gamma ray, a third type of emission from radioactive material, was discovered by Paul Villiard in 1900.

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Definitions

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Natural Radioactivity

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● Radioactive elements continuously undergo radioactive decay or disintegration to form different elements.

• Radioactivity is a property of an atom’s nucleus. It is not affected by temperature, pressure, chemical change or physical state.

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Farley Visitors Center14

radioactive decay the process by which a radioactive element emits particles or rays and is transformed into another element.

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● Each radioactive nuclide disintegrates at a specific and constant rate, which is expressed in units of half-life.

• The half-life (t1/2) is the time required for one-half of a specific amount of a radioactive nuclide to disintegrate.

Page 16: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

The half-life of 131I is 8 days. How much 131I from a 32-g sample remains after five half-lives?

Take a perpendicular line from any multiple of 8 days on the x-axis to the line on the graph.

half-lives

number of days

amount remaining

0

32 g

1

8

16 g

2

16

8 g

Trace a horizontal line from this point on the plotted line to the y-axis and read the corresponding grams of 131I.

3

24

4 g

4

32

2 g

5

40

1 g

18.1

Page 17: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

● Nuclides are said to be either stable (nonradioactive) or unstable (radioactive).

• Elements that have an atomic number greater than 83 are naturally radioactive.

• Some of the naturally occurring nuclides of elements 81, 82 and 83 are radioactive and some are stable.

Page 18: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Date I-1311/14 27601/15 26121/16 23831/17 22871/18 20881/21 15421/23 13221/24 12261/25 11661/29 8191/30 7371/31 6842/1 6002/5 5122/6 4032/7 3852/8 343

2/11 2632/12 255

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Page 20: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Alpha Particles,Beta Particles

and Gamma Rays

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Marie Curie, in a classic experiment, proved that alpha and beta particles are oppositely charged.radiation passes between the poles of an electromagnet

a radioactive source was placed inside a lead block

Alpha rays are less strongly deflected to the negative pole.

Gamma rays are not deflected by the magnet.Beta rays are strongly deflected to the positive pole.

three types of radiation are detected by a photographic plate

18.1

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Alpha Particles

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αIt consists of two protons and two neutrons.

It has a mass of 4 amu.

It has an atomic number of 2.

The symbols of an alpha particle are

An alpha particle is a helium nucleus.

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Loss of an alpha particle from the nucleus results in loss of 4 in the mass number

loss of 2 in the atomic number

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Formation of thorium from the radioactive decay of uranium can be written as

or

mass number decreases by 4

atomic number decreases by 2

Page 26: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

To have a balanced nuclear equation• the sum of the mass numbers (superscripts)

on both sides of the equation must be equal.

• the sum of the atomic numbers (subscripts) on both sides of the equation must be equal.

sum of mass numbers = 238

sum of atomic numbers = 92

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Beta Particles

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Its charge is -1.

The symbols of the beta particle are

The beta particle is identical in mass and charge to an electron.

β

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Loss of a beta particle from the nucleus results in

– no change in the mass number– an increase of 1 in the atomic number

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Gamma Rays

Page 31: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

It is emitted by radioactive nuclei.

It has no measurable mass.

It has no electrical charge.

The symbol of a gamma ray is

A gamma ray is a high energy photon.

γ

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Loss of a gamma ray from the nucleus results in

– no change in the mass number– no change in atomic number

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Write an equation for the loss of an alpha particle from the nuclide 194Pt.

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78 protons

Pt78194

78 protons + 116 neutrons

A nuclide of platinum

Atomic number(number of protons in the nucleus)

Mass number(sum of protons and neutrons in the nucleus)

Write an equation for the loss of an alpha particle from the nuclide 194Pt.

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Write an equation for the loss of an alpha particle from the nuclide 194Pt. Loss of an alpha particle, 4He, results in a decrease of 4 in the mass number and a decrease of 2 in the atomic number.

Mass of new nuclide: 194 – 4 = 190

Atomic number of new nuclide: 78 – 2 = 76Element number 76 is Os, osmium.

The equation is

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What nuclide is formed when 194Ra loses a beta particle from its nucleus?

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88 protons

Ra88228

88 protons + 140 neutrons

A nuclide of radium

Atomic number(number of protons in the nucleus)

Mass number(sum of protons and neutrons in the nucleus)

What nuclide is formed when 194Ra loses a beta particle from its nucleus.

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The loss of a beta particle from a 194Ra nucleus means a gain of 1 in the atomic number with no essential change in mass.

Mass of new nuclide: 228 – 0 = 228

Atomic number of new nuclide: 88 + 1 = 89

What nuclide is formed when 194Ra loses a beta particle from its nucleus.

The equation is

Page 39: 5.1 AN INTRODUCTION TO NUCLEAR Nuclear Reactions

Penetrating Powerof Radiation

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The ability of radioactive rays to pass through various objects is in proportion to the speed at which they leave the nucleus.

Thin sheet of aluminum – stops α and β particles.

18.2

Thin sheet of paper – stops α particles.

5-cm lead block – will reduce, but not completely stop γ radiation

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Shielding Radiation

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Radioactive Disintegration Series

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18.3

The uranium disintegration series. 238U decays by a series of alpha (α) and beta (β) emissions to the stable nuclide 208Pb.

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