Saturday, April 25, 2009

Introduction to Nuclear Fusion

     Fusion is a nuclear process in which two light nuclei combine to form a single heavier nucleus. An example of a fusion reaction important in thermonuclear weapons and in future nuclear reactors is the reaction between two different hydrogen isotopes to form an isotope of helium:


  2H + 3H ----> 4He + n

    

This reaction liberates an amount of energy more than a million times greater than one gets from a typical chemical reaction. Such a large amount of energy is released in fusion reactions because when two light nuclei fuse, the sum of the masses of the product nuclei is less than the sum of the masses of the initial fusing nuclei. Once again, Einstein's equation, E=mc2, explains that the mass that is lost it converted into energy carried away by the fusion products.

     Even though fusion n is an energetically favorable reaction for light nuclei, it does not occur under standard conditions here on Earth because of the large energy investment that is required. Because the reacting nuclei are both positively charged, there is a large electrostatic repulsion between them as they come together. Only when they are squeezed very close to one another do they feel the strong nuclear force, which can overcome the electrostatic repulsion and cause them to fuse.

     Fusion reactions have been going on for billions of years in our universe. In fact, nuclear fusion reactions are responsible for the energy output of most stars, including our own Sun. Scientists on Earth have been able to produce fusion reactions for only about the last sixty years. At first, there were small scale studies in which only a few fusion reactions actually occurred. However, these first experiments later lead to the development of thermonuclear fusion weapons (hydrogen bombs).

     Fusion is the process that takes place in stars like our Sun. Whenever we feel the warmth of the Sun and see by its light, we are observing the products of fusion. We know that all life on Earth exists because the light generated by the Sun produces food and warms our planet. Therefore, we can say that fusion is the basis for our life.

     When a star is formed, it initially consists of hydrogen and helium created in the Big Bang, the process that created our universe. Hydrogen isotopes collide in a star and fuse forming a helium nucleus. Later, the helium nuclei collide and form heavier elements. Fusion is a nuclear reaction in which nuclei combine to form a heavier nucleus. It is the basic reaction which drives the Sun. 

Lighter elements fuse and form heavier elements. These reactions continue until the nuclei reach iron (around mass sixty), the nucleus with the most binding energy. When a nucleus reaches mass sixty, no more fusion occurs in a star because it is energetically unfavorable to produce higher masses. 

Once a star has converted a large fraction of its core's mass to iron, it has almost reached the end of its life.


     The fusion chain cannot continue so its fuel is reduced. Some stars keep shrinking until they become a cooling ember made up of iron. However, if a star is sufficiently massive, a tremendous, violent, brilliant explosion can happen. A star will suddenly expand and produce, in a very short time, more energy than our Sun will produce in a lifetime. When this happens, we say that a star has become a supernova.

     While a star is in the supernova phase, many important reactions occur. The nuclei are accelerated to much higher velocities than can occur in a fusing star. With the added energy caused by their speed, nuclei can fuse and produce elements higher in mass than iron. 

The extra energy in the explosion is necessary to over come the energy barrier of a higher mass element. Elements such as lead, gold, and silver found on Earth were once the debris of a supernova explosion. The element iron that we find all through the Earth and in its center is directly derived from both super novae and dead stars.

More peaceful uses of fusion are being researched today with the hope that soon we will be able to control fusion reactions to generate clean, inexpensive power. 


Source: 

http://www.lbl.gov/abc/Basic.html

Saturday, April 18, 2009

Introduction to Applied Nuclear Physics

As taught in: Spring 2003



The Rutherford-Bohr model of the atom. (Courtesy of EPA.)

Level:

Undergraduate

Instructors:

Prof. Kim Molvig

Course Description

This course concentrates on the basic concepts of nuclear physics with emphasis on nuclear structure and radiation interactions with matter. Included: elementary quantum theory; nuclear forces; shell structure of the nucleus; alpha, beta, and gamma radioactive decays; interactions of nuclear radiations (charged particles, gammas, and neutrons) with matter; nuclear reactions; and fission and fusion.
The course is divided into three main sections:
  1. Quantum Mechanics Fundamentals
  2. Nuclear Structure and Nuclear Decays
  3. Interactions in Nuclear Matter and Nuclear Reactions
Sources:
1. http://web.mit.edu/nse/index.html
2. http://ocw.mit.edu/courses/nuclear-engineering/

Friday, April 10, 2009

Half-Life and Reactions

Half-life

     The time required for half of the atoms in any given quantity of a radioactive isotope to decay is the half-life of that isotope. Each particular isotope has its own half-life. For example, the half-life of 238U is 4.5 billion years. That is, in 4.5 billion years, half of the 238U on Earth will have decayed into other elements. In another 4.5 billion years, half of the remaining 238U will have decayed. 

One fourth of the original material will remain on Earth after 9 billion years. The half-life of 14C is 5730 years, thus it is useful for dating archaeological material. Nuclear half-lives range from tiny fractions of a second to many, many times the age of the universe.

For more information on half-life and isotopes, please refer to the Isotopes Project at LBNL where you can also find the Table of Isotopes online.

Reactions

     If nuclei come close enough together, they can interact with one another through the strong nuclear force, and reactions between the nuclei can occur. As in chemical reactions, nuclear reactions can either be exothermic (i.e. release energy) or endothermic (i.e. require energy input). Two major classes of nuclear reactions are of importance: fusion and fission.

Sumber:

http://www.lbl.gov/abc/Basic.html
 

Wednesday, April 1, 2009

Readings by Lecture Topic: Neutron Science and Reactor Physics


Readings

Amazon logo Help support MIT OpenCourseWare by shopping at Amazon.com! MIT OpenCourseWare offers direct links to Amazon.com to purchase the books cited in this course. Click on the Amazon logo to the left of any citation and purchase the book from Amazon.com, and MIT OpenCourseWare will receive up to 10% of all purchases you make. Your support will enable MIT to continue offering open access to MIT courses.

Textbooks

The text book for this course is:

Amazon logo Lamarsh, John. Introduction to Nuclear Engineering. 3rd ed. Englewood Cliffs, NJ: Prentice Hall, 2001. ISBN: 9780201824988.

This covers basic reactor physics as part of a complete survey of nuclear engineering.
Readings may also be assigned from certain of the books listed below:
Amazon logo Henry, A. F. Nuclear Reactor Analysis. Cambridge, MA: MIT Press, 1975. ISBN: 9780262080811.

Amazon logo Shultis, J., and R. Faw. Fundamentals of Nuclear Science and Engineering. New York, NY: Marcel Dekker, 2002. ISBN: 9780824708344.

Amazon logo Hewitt, G., and J. Collier. Introduction to Nuclear Power. New York, NY: Taylor and Francis, 2000. ISBN: 9781560324546.

Amazon logo Turner, J. Atoms, Radiation, and Radiation Protection. New York, NY: Pergamon Press, 1986. ISBN: 9780080319377.

Amazon logo Kneif, R. Nuclear Criticality Safety: Theory and Practice. American Nuclear Society, 1985. ISBN: 9780894480287.
Amazon logo Knoll, G. Radiation Detection and Measurement. New York, NY: Wiley, 2000. ISBN: 9780471073383.

Readings by Lecture Topic

 


Note: "L" refers to the Lamarsh text.

Lec # Topics Readings
1 Introduction/reactor layout and classification Henry - Section 1.8 (PDF - 2.5 MB) (Courtesy of MIT Press. Used with permission.)
2 Chart of nuclides/neutron sources L - Chapter 2
Knoll - pp. 20 to 28
3 Neutron reactions/Boltzman distribution/number density Turner -Section 9.7
4 Neutron cross-sections
5 Binding energy/liquid drop model/fission process Shultis - Section 3.2
L - Section 3.7

Tour of MIT research reactor
6 Burners, converters, breeders/neutron life cycle L - Section 4.2
7 Neutron life cycle
8 Criticality accidents/why is radiation dangerous Kneif - Chapter 3
9 Neutron flux, reaction rates, current L - Sections 5.1 and 5.2
10 One velocity model L - Sections 5.3 and 5.4

Exam 1
11 Non-multiplying media L - Section 5.6
12 Multiplying media L - Sections 6.1 to 6.3
13 Criticality conditions L - Section 6.4
14 Kinematics of neutron scattering L - Section 3.6
Henry - Section 2.5
15 Group diffusion method L - Section 5.8
Henry - Sections 3.1 and 3.2
16 Solution of group equations Henry - Section 3.3

Exam 2
17 Energy dependence of flux Henry - Section 3.4
18 Group theory/four factor formula Henry - Section 3.5
19 Reactors of finite size Henry - Section 4.4 to 4.7
20 Reactors of multiple regions: One group Henry - Sections 4.9 and 4.10
21 Reactors of multiple regions: Two group Henry - Section 4.11
22 Application of the two-group equations L - pp. 304 to 308
23 Few group and multi-group approaches L - Section 6.7
Henry - Section 4.13
24 Monte Carlo analysis Henry - pp. 371 to 379

Exam 3
25 Subcritical multiplication and reactor startup
26 Reactor operation without feedback L - Section 7.1 to 7.2
L - Section 7.1
27 Analytic solution of reactor kinetics Henry - Section 7.5
28 Dynamic period and inhour equation Bernard, John A., and Lin Wen Hu. "Dynamic Period Equation: Derivation, Relation to Inhour Equation, and Precursor Estimation." IEEE Transactions on Nuclear Science 46, no. 3 (1999): 425-437.
29 Reactor operation with feedback effects L - Sections 7.3 and 7.4
Henry - Section 6.3
30 Achievement of feedback effects Hewitt - Sections 2.4.6 and 5.2.7

Exam 4
31 Shutdown margin/review of TMI

Review


Sumber:

http://web.mit.edu/nse/index.html