Separation of Isotopes by Laser Excitation

In summary, this technology was developed in the early '70s at Lawrence Livermore National Laboratory: the process is called AVLIS - Atomic Vapor Laser Isotope Separation. You need a VERY precise tunable laser and send it zig-zagging through a chamber of UF6 gas or vaporized U to ionize the U-235, but not the U-238.
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  • #3
kaos said:
kaos,

Actually this technology was developed in the early '70s at Lawrence Livermore
National Laboratory:

http://www.llnl.gov/50th_anniv/decades/1970s.htm

[Scroll down to the entry for the year 1973 ]

The process is called AVLIS - Atomic Vapor Laser Isotope Separation.

Here's how it works. The equations of Quantum Mechanics that describe how
electrons "orbit" atoms contains in one of its terms the mass of the electron.
However, since the electron orbits a nucleus of finite mass; this is a "two-body"
problem - and one has to use the so-called "reduced mass" of the electron -
m = m*M / (m + M) where "m" is the electron mass, and "M" is the mass of the
nucleus.

Therefore, the mass of the nucleus "M" enters into the equations that define the
orbits of the electrons. When you do the calculations, you will find that the
"ionization potential" - that is the amount of energy you have to add to the outermost
electron to kick it free and form a charged ion - is very slightly less for U-235 than it
is for U-238.

You then need a VERY precise tunable laser. LLNL developed a tunable dye laser
pumped by copper vapor lasers. You tune the laser to a frequency so that the laser
photons have enough energy to ionize U-235; but not enough energy to ionize U-238.

You send this laser zig-zagging through a chamber of UF6 gas or vaporized U and
the laser will ionize the U-235, but not the U-238. The U-235 can then be deflected
electrostatically by a charged plate into a separate stream from the U-238.

To learn more about AVLIS, tunable laser applications, and a spin-off from this
work called the "laser guide star" - a powerful new tool for astronomers first deployed
on the 3m Shane telescope at Lick Observatory - but now in use at largest telescopes
in the world - the Keck telescopes on Mauna Kea in Hawaii; see:

www.llnl.gov/str/pdfs/05_00.2.pdf

Dr. Gregory Greenman
Physicist
 
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  • #4
Morbius said:
When you do the calculations, you will find that the
"ionization potential" - that is the amount of energy you have to add to the outermost
electron to kick it free and form a charged ion - is very slightly less for U-235 than it
is for U-238.

I have a figure in one of my texts that shows that light of a lower wavelength is used for U-235. Does this not correspond to a higher energy for ionization for U-235 than for U-238?
 
  • #5
theCandyman said:
I have a figure in one of my texts that shows that light of a lower wavelength is used for U-235. Does this not correspond to a higher energy for ionization for U-235 than for U-238?
Candyman,

You may be correct. I forget whether U-235 absorbs at a lower frequency - in which
case it has a lower ionization potential; or at a lower wavelength [ higher frequency ],
in which case it has a higher ionization potential.

Dr. Gregory Greenman
Physicist
 
  • #6
theCandyman said:
I have a figure in one of my texts that shows that light of a lower wavelength is used for U-235. Does this not correspond to a higher energy for ionization for U-235 than for U-238?
The 'shorter' wavelength corresponds to a slightly higher ionization energy, but not by much.

According to Wikipedia - The absorption lines of 235U and 238U differ slightly; for example, the 238[/sup]U absorption peak shifts from 5027.4 Angstroms to 5027.3 Angstroms in 235U.

According to the UWisc NE notes, the wavelength used to ionized U-235 is 5915 Å, so I'll have to find other references to clarify.

Some discussion here - http://fti.neep.wisc.edu/neep423/FALL99/lecture8.pdf

Contrary to what other sources say, USEC took over ALVIS from LLNL then abandoned it.

USEC to Go Private

President Clinton has approved proceeding with the privatization of the United States Enrichment Corporation (USEC). USEC manages the Laboratory's Atomic Vapor Laser Isotope Separation (AVLIS) project, which is intended to produce enriched uranium for commercial nuclear reactor fuel. USEC was created in 1992 by Congress to privatize federal uranium enrichment activities, which convert natural uranium to enriched uranium for reactor fuel. With Clinton's approval, USEC will now be moved to the private sector.

"The vision . . . is to move uranium enrichment out of the government and into the private sector while realizing a substantial return for the U.S. taxpayer," said USEC Chairman William J. Rainer. "This latest action moves us to the final stages of realizing that vision." The action also furthers the nation's largest technology transfer effort.

USEC officials estimate it will take approximately six months to convert to private ownership. Added Victor Lopiano, director of the AVLIS program at Livermore, "This is an important first step toward AVLIS deployment."
ref: http://www.llnl.gov/str/News1097.html

http://www.usec.com/v2001_02/Content/News/NewsTemplate.asp?page=/v2001_02/Content/News/Speeches/09-07-00.htm

Other interesting data - Table of Ionization Energies (eV) of Atoms and Ions -
http://www.astro.lsa.umich.edu/~cowley/ionen.htm
 
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Related to Separation of Isotopes by Laser Excitation

1. What is "Separation of Isotopes by Laser Excitation"?

"Separation of Isotopes by Laser Excitation" is a technique used in isotope separation, which is the process of separating different isotopes of an element. It involves using lasers to excite specific isotopes, causing them to separate from the other isotopes and become concentrated in a specific area.

2. How does "Separation of Isotopes by Laser Excitation" work?

This technique works by using lasers to target specific isotopes of an element. The lasers excite the electrons in the isotopes, causing them to move to higher energy levels. As the isotopes move to different energy levels, they become easier to separate from the other isotopes and can be collected in a specific area.

3. What are the benefits of using "Separation of Isotopes by Laser Excitation"?

One of the main benefits of this technique is that it is highly precise and efficient. It allows for the separation of isotopes with very similar properties, which can be difficult to achieve using other methods. Additionally, it is a non-destructive method, meaning the separated isotopes can be collected and used for further research or applications.

4. What are some applications of "Separation of Isotopes by Laser Excitation"?

This technique has a wide range of applications, including in nuclear power plants, medical imaging and treatments, and scientific research. It is also used in the production of enriched uranium for nuclear weapons and in the purification of rare isotopes for use in scientific experiments.

5. Are there any limitations or challenges associated with "Separation of Isotopes by Laser Excitation"?

One of the main challenges with this technique is the high cost of the equipment and resources needed for the process. It also requires a high level of expertise and precision to achieve successful separation. Additionally, the process can only be used for elements that have different isotopes with distinct energy levels, limiting its applicability to some elements.

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