19
Nuclear Physics: Radiation, Radioactivity & its Applications

Nuclear Physics: Radiation, Radioactivity & its Applications

Embed Size (px)

DESCRIPTION

Nuclear Physics: Radiation, Radioactivity & its Applications. Nuclear Energy. The Nucleus of an atom contains Protons – Positively Charged Neutrons – no charge - PowerPoint PPT Presentation

Citation preview

Page 1: Nuclear Physics: Radiation, Radioactivity & its Applications

Nuclear Physics: Radiation, Radioactivity & its

Applications

Page 2: Nuclear Physics: Radiation, Radioactivity & its Applications

Nuclear Energy The Nucleus of an atom contains

Protons – Positively Charged Neutrons – no charge

Atomic Mass Number – denoted by the letter A, this number represents the total number of protons + neutrons in the nucleus, telling you what isotope of the element you have.

Atomic Number – denoted by the letter Z, this number represents the number of protons in the nucleus, telling you what element you have.

Page 3: Nuclear Physics: Radiation, Radioactivity & its Applications

Nuclear Energy Atomic Symbol for

a given isotope of an element is generally given as noted to the right.

A prime example is an alpha particle or helium nucleus

XAZ

He42

Page 4: Nuclear Physics: Radiation, Radioactivity & its Applications

Nuclear Reactions Two Types of Nuclear reactions

produce vast amounts of energy according to Einstein’s famous equation

E = mc2

Fission – the splitting of an atom into smaller parts

Fusion- the joining of two small nuclei to produce one larger nucleus

Page 5: Nuclear Physics: Radiation, Radioactivity & its Applications

Nuclear Reactions Mass defect – is the amount of mass that is

converted to energy during fission or fusion.

Calculation of Mass defect is the difference between the actual mass of the atom and the known mass of each of its parts

The amount of energy that this mass is converted into is called the binding energy

Page 6: Nuclear Physics: Radiation, Radioactivity & its Applications

Sample Problem

Calculate the mass defect and energy released in the creation of Carbon-13.

Solution Expected Mass: Protons = 6 (1.007276 u) = 6.043656 uNeutrons = 7(1.008665 u) = 7.060655 u 13.104311 uKnown Mass -13.003355 uMass Defect .100956 u

Energy Released = (931.5 MeV/u)(0.100956 u) = 94.04 MeV

Page 7: Nuclear Physics: Radiation, Radioactivity & its Applications

Radioactivity Three types of Radioactivity

Alpha – α – is the nucleus of a helium atom Can be stopped by a sheet of paper, is harmful only if

ingested Beta – β – emission of an electron or positron

Can be stopped by a sheet of lead, is harmful to all living tissue

Gamma – γ – emission of a high energy photon Cannot be completely stopped. Very harmful to all

living tissue.

Page 8: Nuclear Physics: Radiation, Radioactivity & its Applications

Nuclear Reactions

Alpha Decay

Beta Decay

Gamma Emission

HeRnRa 42

22286

22688

NN AZ

AZ *

eNC 147

146

Page 9: Nuclear Physics: Radiation, Radioactivity & its Applications

Half Life The half life of a radioactive

material is the amount of time required for ½ of the sample to decay into another element or isotope.

Half lives are calculated according to the equation:

a = a0(½)x

Page 10: Nuclear Physics: Radiation, Radioactivity & its Applications

Half Life a = amount of material left at any time a0 = amount of material that you begin with x = the number of half lives that have

passed since you have begun counting This type of decay is said to be

exponential since it can be described graphically as a hyperbola

Page 11: Nuclear Physics: Radiation, Radioactivity & its Applications

Sample Problem

Carbon-14, a radioactive isotope of carbon, has a half life of 5730 years. If a 20 gram sample of carbon-14 is allowed to decay for 10,000 years, how much remains at the end of this period?

Page 12: Nuclear Physics: Radiation, Radioactivity & its Applications

Solution

a = a0(½)x

a0 = 20 grams

x = 10,000 yrs/5730 yrs/half life = 1.75So a = 20 grams(½)1.75 = 5.95 grams

Page 13: Nuclear Physics: Radiation, Radioactivity & its Applications

Detection of Radiation Counters

Geiger Counter – Radiation causes a gas to emit electrons causing a voltage which makes the counter “click”

Scintillation counter – uses a solid, liquid, or gas scintillator – a material which is excited by radiation to emit light. The light is captured and amplified by a Photomultiplier (PM) tube – which turns it into an electric signal.

Semi-conductor detector – uses a p-n junction diode which produces a short electric pulse when irradiated

Page 14: Nuclear Physics: Radiation, Radioactivity & its Applications

Detection of Radiation Trackers

Photographic emulsion – the particle passing through the emulsion ionizes atoms in its path

Cloud chamber – a gas is cooled to a temperature slightly below its normal condensation temperature hence it condenses on any ionized molecule present this “tracks” the particle

Bubble chamber – a liquid is kept close to its boiling temperature and hence “bubbles” around any ionized particle – the bubbles are then left in the wake of the particle and photographed

Page 15: Nuclear Physics: Radiation, Radioactivity & its Applications

Applications of Nuclear Processes

Energy can be released in a nuclear reaction by one of two processes: Fission – the splitting of a nucleus into

smaller nuclei Fusion – the joining of two smaller

nuclei into a larger nuclei

Page 16: Nuclear Physics: Radiation, Radioactivity & its Applications

Fission Usually caused by neutron bombardment

of the nucleus, causing the nucleus to split Mass is converted into energy All current nuclear reactor technology uses

fission Fission is controlled by using a

moderator, a material which absorbs neutrons to keep the chain reaction under control

Page 17: Nuclear Physics: Radiation, Radioactivity & its Applications

Fusion Fusion reactions take lighter nuclei,

often an isotope of hydrogen called deuterium and fuse them together to make a heavier nuclei, often helium

This must occur at high energy and is very difficult to produce under laboratory conditions

Currently no workable fusion reactor has been produced on earth

The sun and stars all produce energy due to nuclear fusion

Page 18: Nuclear Physics: Radiation, Radioactivity & its Applications

Measurement of Radiation: Dosimetry

Since radiation can harm the body it is important to quantify the amount of radiation received, or the dose. The study of this is called dosimetry and is an important part of an emerging field known as Health Physics

Dosimetry is most often concerned with the number of rads or millirads of radiation received.

A rad is defined as the amount of radiation which deposits energy at a rate of 0.01 J/kg in any absorbing material

Page 19: Nuclear Physics: Radiation, Radioactivity & its Applications

Things to Know Atomic number, Atomic mass number, atomic

symbols, atomic equations Mass defect, binding energy Types of Radiation

Alpha Beta Gamma

Detection of Radiation Nuclear Reactions

Fission Fusion

Dosimetry