Nuclear Physics 2

Содержание

Слайд 2

ANNOUNCMENTS

CW Test on CW 11, 12
(Special Relativity and Nuclear Physics)

ANNOUNCMENTS CW Test on CW 11, 12 (Special Relativity and Nuclear Physics)
on Monday 27 Feb during normal lecture times.
Come to same room as last term CW Tests
No Labs This Week
New Textbooks are now available at Library
(College Physics, Serway, 10th Edition)

Слайд 3

Detecting radiation and nuclear energy

e.g., Geiger Muller tube
Mica window
Low pressure gas
High voltage
Anode/cathode
High

Detecting radiation and nuclear energy e.g., Geiger Muller tube Mica window Low
E field
Massive ionization
Electron avalanche
Pulse

Слайд 5

Atomic mass unit

One atomic mass unit (amu or u) is equal

Atomic mass unit One atomic mass unit (amu or u) is equal
to a mass of
1u =1.661 x 10-27 kg
This small mass can be measured using a mass spectrometer

Слайд 6

Example 1:

1u =1.661 x 10-27 kg
Find its equivalence in
Joules of Energy,

Example 1: 1u =1.661 x 10-27 kg Find its equivalence in Joules
and
MeV of Energy

Слайд 7

Example 2:

Using mass spectrometry, physicists have measured the masses of nuclei, protons

Example 2: Using mass spectrometry, physicists have measured the masses of nuclei,
and neutrons accurately. An alpha particle has a mass of 4.002603 u, a proton 1.007276 u and a neutron 1.008665 u. How is this possible?

Слайд 8

Mass defect

In any type of nuclear transformation,
reactants products
(sum of rest masses

Mass defect In any type of nuclear transformation, reactants products (sum of
of reactants)
(sum of rest masses of products)
MASS DEFECT

Слайд 9

Nuclear binding energy

Work must be done to remove any nucleon from a

Nuclear binding energy Work must be done to remove any nucleon from
nucleus.
Nuclear binding energy
is …

The nuclear binding energy is the energy equivalent of the mass defect.

Слайд 10

Binding energy per nucleon

More convenient to use ‘binding energy per nucleon’.
Mostly between

Binding energy per nucleon More convenient to use ‘binding energy per nucleon’.
7 to 9 MeV per nucleon

Слайд 11

Energy Difference of Fusion and Fission

Effect of fusion and fission
Both decrease the

Energy Difference of Fusion and Fission Effect of fusion and fission Both
average nucleon PE (increasing binding energy per nucleon). PE lost is emitted as gamma rays and KE of particles.

Слайд 12

Spontaneous and induced fission

Spontaneous – occurs naturally
Induced – requires a ‘slow’ neutron

Spontaneous and induced fission Spontaneous – occurs naturally Induced – requires a
to react with nucleus
For fission, is only one nuclear transformation possible?

Слайд 13

Fission fragments

Many different reactions are possible when U-235 fissions.
How much more probable

Fission fragments Many different reactions are possible when U-235 fissions. How much
is it that a fission product has an mass number of 110 than 85?

Слайд 14

Example 3
a) A possible fission reaction is shown above. Given that the

Example 3 a) A possible fission reaction is shown above. Given that
masses of U, La, Br and n are 235.1 u, 148.0 u, 84.90 u and 1.009 u respectively, how much energy in joules is released in each fission?
b) How many joules would be released if all the atoms in 10.00 kg of U-235 undergo fission?

Слайд 15

Some facts about reactors

As of Feb, 2012 worldwide, 31 countries have 435

Some facts about reactors As of Feb, 2012 worldwide, 31 countries have
active reactors producing 368 GW of Energy.
63 new reactors now under construction in 15 countries.
France “most nuclear”; 76.2% of electricity
UK has 19 reactors; USA 104, Kazakhstan 0 (but planning) and China 16 (26 under construction; 90 proposed).
From: http://www.euronuclear.org

Слайд 16

The ‘controversial’ business of neutrons

In fission, one slow neutron combines with U-235,

The ‘controversial’ business of neutrons In fission, one slow neutron combines with
causing the emission of two or more neutrons. In turn, these neutrons cause two fissions, etc
We obtain a chain reaction
If uncontrolled in a large amount of U-235, a chain reaction leads to…

Слайд 17

Why mushrooms?

Why mushrooms?

Слайд 18

Atomic bombs (using fission)

Atomic bombs (using fission)

Слайд 20

What do you know about the history of nuclear tests within Kazakh

What do you know about the history of nuclear tests within Kazakh territory? Semipalatinsk Test Site
territory?

Semipalatinsk Test Site

Слайд 21

Nuclear reactors - controlled fission

Nuclear reactors - controlled fission

Слайд 22

Fusion

Fusion occurs in the sun: the proton cycle.
Fusion has been used in

Fusion Fusion occurs in the sun: the proton cycle. Fusion has been
an uncontrolled way in the hydrogen bomb. A fission detonator was used to create high temperature and enable fusion.
A challenge for this century is to recreate and control fusion. One interesting reaction to use is:
In this case Q is 18.0 MeV

Слайд 23

Simulating fusion

JET, the Joint European Torus, using the TOKAMAK (toroidal magnetic chamber)

Simulating fusion JET, the Joint European Torus, using the TOKAMAK (toroidal magnetic chamber)

Слайд 24

READING Adams and Allday: 8.26 to 8.32, inclusive.
At the end of this lecture

READING Adams and Allday: 8.26 to 8.32, inclusive. At the end of
you should
Have met and understood how to use Einstein's equation ΔE=Δmc2
Understand the phrases binding energy and mass defect
Understand how energy can be released from nuclear reactions by fission and fusion
Have a basic knowledge of the 'binding energy per nucleon' curve and be able to interpret it
Know what the terms critical mass, moderator, coolant and chain reaction mean in relation to production of energy from a nuclear reactor
Be aware of the main steps of hydrogen fusion in the sun
Имя файла: Nuclear-Physics-2.pptx
Количество просмотров: 162
Количество скачиваний: 1