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[[Image:Fission chain reaction.svg|300px|thumb|A possible [[nuclear fission]] chain reaction. 1. A [[uranium-235]] atom absorbs a [[neutron]], and fissions into two new atoms (fission fragments), releasing three new neutrons and a large amount of binding energy. 2. One of those neutrons is absorbed by an atom of [[uranium-238]], and does not continue the reaction. Another neutron leaves the system without being absorbed. However, one neutron does collide with an atom of uranium-235, which then fissions and releases two neutrons and more binding energy. 3. Both of those neutrons collide with uranium-235 atoms, each of which fissions and releases a few neutrons, which can then continue the reaction.]]


A '''nuclear chain reaction''' occurs when one [[nuclear reaction]] causes an average of one or more nuclear reactions, thus leading to a self-propagating series of these reactions.  The specific nuclear reaction may be the fission of heavy isotopes (e.g. <sup>235</sup>U).  The nuclear chain reaction releases several million times more energy per reaction than any [[chemical reaction]].


==History==
It's cooked! The new versions of our books are finally finished, converted to PDF's in addition, on waiting the dashboard you discover the members to read and go forth start off making their mark. There's just one problem: They're already old-fashioned! This is why we article. The way social media and web-based marketing change constantly to become almost impossible for the sunday paper that has months to update to stay completely current on every point in guide is designed to. This is one with the reasons it took as long to get the updates your market book. Every time we changed one thing, something else in the book would are changed.<br><br>If you are the type of human that wishes to blog, you wish to look for Blogging Interests. These could be Blogging Groups or Blogging Tribes. The blogger within these group share great help and advice. on how to grow your businesses and also help encourage each other's blog. After you get this going you'll start for just a lot of traffic. Without a doubt time but well this.<br><br>However, after you have tired of hearing some colleagues fussing that I wasn't "on board" I decided to perform a twirl. Well, I'm hooked. And guess methods? I'm making great involving this Social Media site obtaining to waste hours each single day.<br><br><br><br>Job seekers are afraid group job hunting is just too much say for example a support array. For this last reason, I blame career counseling. While the intention is nice, helping unemployed people, the application often is removed like an addiction support webinar. Job seekers are already often feeling down; they do not have to be treated like they have fallen in the wagon. Instead they to help attend networking functions compared to other professionals in which united to buy common purpose. That is support and encouragement, but is not patronizing. Individuals aren't scared haven't failed; they are looking to find jobs. We tell the particular represent themselves as top talent, on the internet we have meetings where we all sit in a circle and look lost.<br><br>List business. Keep in mind that majority of individuals that will visit your own website will not make an investment right away on vacation. However, that doesn't mean losing their business for all of eternity. You can still get them to purchase from you by building an ongoing communication all of them. You can do this by obtaining their contact information (email address and phone number) so you can easily consult them when promoting your products or services or for all those running some advertising gimmicks.<br><br>Where unearth content. Understand have a handful of your own content to begin with- in your brochures, flyers, booklets etc. Involving content to obtain you went on! However, most individuals need to "borrow" content from a different individual from in order to time. There is nothing wrong with this as long as you follow some basic rules.<br><br>C. Online PR: Writing a press release, optimized for the keywords you try to target, is very effective. They should be nearly 300 words, about something your business is doing, and also should be put up somewhere on weblog or blog (I think it's less difficult to put them on an individual blog), then submitted to online PR sites. Make use of a keyword with your title and/or sub-title. I am doing these weekly for my company and for clients.<br><br>Product use. If you are into publishing business, you've were able to have other products aside from the coaching programming. I am sure must expect men and women to spend millions of dollars for their initial purchase, right? Get these traffic to trust you by offering them with low-end products first that will cost anywhere from $10-$30. Enough pressure here is giving they will a opportunity to experience your offerings without really burning their pockets. If you strive to please them whenever they obtain you, I'm sure that they will returning for additional.<br><br>When you beloved this informative article along with you would want to be given more info with regards to [http://www.mavsocial.com/ Social Media Campaign Planning Software] generously visit our own site.
 
Chemical [[chain reaction]]s were first proposed by German chemist [[Max Bodenstein]] in 1913, and were reasonably well understood before nuclear chain reactions were proposed.<ref>[http://nobelprize.org/nobel_prizes/chemistry/laureates/1956/press.html See this 1956 Nobel lecture for history of the chain reaction in chemistry]</ref> It was understood that chemical chain reactions were responsible for exponentially increasing rates in reactions, such as produced chemical explosions.
 
The concept of a nuclear chain reaction was first hypothesized by [[Hungary|Hungarian]] scientist [[Leó Szilárd]] on Tuesday, September 12, 1933. The neutron had been discovered in 1932, shortly before. Szilard realized that if a nuclear reaction produced neutrons, which then caused further nuclear reactions, the process might be self-perpetuating. Szilárd, however, did not propose fission as the mechanism for his chain reaction, since the fission reaction was not yet discovered or even suspected. Instead, Szilard proposed using mixtures of lighter known isotopes which produced neutrons in copious amounts. He filed a patent for his idea of a simple nuclear reactor the following year.<ref>L. Szilárd, "Improvements in or relating to the transmutation of chemical elements," British patent number: GB630726 (filed: 28 June 1934; published: 30 March 1936). [http://v3.espacenet.com/textdoc?DB=EPODOC&IDX=GB630726 esp@cenet document view<!-- Bot generated title -->]</ref>
 
In 1936, Szilárd attempted to create a chain reaction using [[beryllium]] and [[indium]], but was unsuccessful. After [[nuclear fission]] was discovered by [[Lise Meitner|Meitner]], [[Otto Hahn|Hahn]] and [[Otto Robert Frisch|Frisch]] in 1938, Szilárd and [[Enrico Fermi]] in 1939 searched for, and discovered, neutron multiplication in uranium, proving that a nuclear chain reaction by this mechanism was indeed possible.<ref>[[Herbert L. Anderson|H. L. Anderson]], E. Fermi, and Leo Szilárd, "Neutron production and absorption in uranium," ''The Physical Review'', vol. 56, pages 284–286 (1 August 1939).  Available on-line at  [http://www.fdrlibrary.marist.edu/psf/box5/a64g01.html FDRlibrary.marist.edu]</ref>  This discovery prompted [[Einstein–Szilárd letter|the letter]] from Szilard{{failed verification|date=December 2012}} and signed by [[Albert Einstein]] to President [[Franklin D. Roosevelt]] warning of the possibility that [[Nazi Germany]] might be attempting to build an atomic bomb.<ref>[http://www.aip.org/history/einstein/ae43a.htm AIP.org]</ref><ref>[http://www.atomicarchive.com/Docs/Begin/Einstein.shtml Atomicarchive.com]</ref>
 
Enrico Fermi and Leo Szilárd created the first artificial self-sustaining nuclear chain reaction, called [[Chicago Pile-1]] (CP-1), in a [[racquets (sport)|racquets]] court below the bleachers of [[Stagg Field]] at the [[University of Chicago]] on December 2, 1942. Fermi's experiments at the University of Chicago were part of [[Arthur H. Compton]]'s  [[Metallurgical Laboratory]], part of the [[Manhattan Project]]; the lab was later moved outside Chicago, renamed [[Argonne National Laboratory]], and tasked with conducting research in harnessing fission for nuclear energy.<ref name="Holl">
{{cite book
|last=Holl |first=Jack
|year=1997
|title=Argonne National Laboratory, 1946-96
|publisher=[[University of Illinois Press]]
|isbn=0-252-02341-2
}}</ref>
 
In 1956, Paul Kuroda of the [[University of Arkansas]] postulated that a natural fission reactor may have once existed. Since nuclear chain reactions only require natural materials (such as water and uranium), it is possible to have these chain reactions occur where there is the right combination of materials within the Earth's crust. Kuroda's prediction was verified with the discovery of evidence of [[Natural nuclear fission reactor|natural self-sustaining nuclear chain reactions]] in the past at [[Oklo]] in Gabon, Africa in  September 1972.<ref>[http://www.ocrwm.doe.gov/factsheets/doeymp0010.shtml Oklo: Natural Nuclear Reactors—Fact Sheet]</ref>
 
==Fission chain reaction==
 
Fission chain reactions occur because of interactions between [[neutrons]] and [[fissile]] isotopes (such as <sup>235</sup>U). The chain reaction requires both the release of neutrons from fissile isotopes undergoing [[nuclear fission]] and the subsequent absorption of some of these neutrons in fissile isotopes. When an atom undergoes nuclear fission, a few neutrons (the exact number depends on several factors) are ejected from the reaction. These free neutrons will then interact with the surrounding medium, and if more fissile fuel is present, some may be absorbed and cause more fissions.  Thus, the cycle repeats to give a reaction that is self-sustaining.
 
[[Nuclear power plants]] operate by precisely controlling the rate at which nuclear reactions occur, and that control is maintained through the use of several redundant layers of safety measures.  Moreover, the materials in a nuclear reactor core and the uranium enrichment level make a nuclear explosion impossible, even if all safety measures failed. On the other hand, [[nuclear weapons]] are specifically engineered to produce a reaction that is so fast and intense it cannot be controlled after it has started.  When properly designed, this uncontrolled reaction can lead to an explosive energy release.
 
===Nuclear fission fuel===
 
Nuclear fission weapons must use an extremely high quality, highly-enriched fuel exceeding the critical size and geometry ([[Critical mass (nuclear)|critical mass]]) in order to obtain an explosive chain reaction. The fuel for a nuclear fission reactor is very different, usually consisting of a low-enriched oxide material (e.g. UO<sub>2</sub>).
 
===Fission reaction products===
{{main|nuclear fission}}
When a heavy atom undergoes nuclear fission it breaks into two or more fission fragments.  Also, several free neutrons, [[gamma rays]], and [[neutrinos]] are emitted, and a large amount of energy is released.  The sum of the rest masses of the fission fragments and ejected neutrons is less than the sum of the rest masses of the original atom and incident neutron (of course the fission fragments are not at rest). The mass difference is accounted for in the release of energy according to the equation '''E=Δmc²''':
 
'''mass of released energy''' = <math>\frac{E}{c^2} = m_\mbox{original}-m_\mbox{final}</math>
 
Due to the extremely large value of the [[speed of light]], c, a small decrease in mass is associated with a tremendous release of active energy (for example, the kinetic energy of the fission fragments). This energy (in the form of radiation and heat) '''carries''' the missing mass, when it leaves the reaction system (total mass, like total energy, is always [[conservation of mass|conserved]]). While typical chemical reactions release energies on the order of a few [[electron volt|eV]]s (e.g. the binding energy of the electron to hydrogen is 13.6&nbsp;eV), nuclear fission reactions typically release energies on the order of hundreds of millions of eVs.
 
Two typical fission reactions are shown below with average values of energy released and number of neutrons ejected:
 
:<math>{}^{235}\mbox{U} + \mbox{neutron} \rightarrow \mbox{fission fragments} + 2.4\mbox{ neutrons} + 192.9\mbox{ MeV}</math><ref name=Duderstadt>{{cite book |last=Duderstadt |first=James |coauthors=Hamilton, Louis |title=Nuclear Reactor Analysis |year=1976 |publisher=John Wiley & Sons, Inc |isbn=0-471-22363-8 }}</ref>
:<math>{}^{239}\mbox{Pu} + \mbox{neutron} \rightarrow \mbox{fission fragments} + 2.9\mbox{ neutrons} + 198.5\mbox{ MeV}</math><ref name=Duderstadt />
 
Note that these equations are for fissions caused by slow-moving (thermal) neutrons.  The average energy released and number of neutrons ejected is a function of the incident neutron speed.<ref name=Duderstadt /> Also, note that these equations exclude energy from neutrinos since these subatomic particles are extremely non-reactive and, therefore, rarely deposit their energy in the system.
 
==Timescales of nuclear chain reactions==
 
===Prompt neutron lifetime===
 
The '''prompt neutron lifetime''', ''l'',  is the average time between the emission of neutrons and either their absorption in the system or their escape from the system.<ref name=Lamarsh />  The term lifetime is used because the emission of a neutron is often considered its "birth," and the subsequent absorption is considered its "death."  For thermal (slow-neutron) fission reactors, the typical prompt neutron lifetime is on the order of 10<sup>−4</sup> seconds, and for fast fission reactors, the prompt neutron lifetime is on the order of 10<sup>−7</sup> seconds.<ref name=Duderstadt />  These extremely short lifetimes mean that in 1 second, 10,000 to 10,000,000 neutron lifetimes can pass. The ''average'' (also referred to as the ''adjoint unweighted'') prompt neutron lifetime takes into account all prompt neutrons regardless of their importance in the reactor core; the ''effective'' prompt neutron lifetime (referred to as the ''adjoint weighted'' over space, energy, and angle) refers to a neutron with average importance.<ref>[http://www.osti.gov/bridge/product.biblio.jsp?query_id=1&page=0&osti_id=991100 Deterministic and Monte Carlo Analyses of YALINA Thermal Subcritical Assembly]</ref>
 
===Mean generation time===
 
The '''mean generation time''', Λ, is the average time from a neutron emission to a capture that results in fission.<ref name=Duderstadt /> The mean generation time is different from the prompt neutron lifetime because the mean generation time only includes neutron absorptions that lead to fission reactions (not other absorption reactions). The two times are related by the following formula:
 
:<math>\Lambda = \frac{l}{k}</math>
 
In this formula, k is the effective neutron multiplication factor, described below.
 
===Effective neutron multiplication factor===
 
The '''[[six factor formula|effective neutron multiplication factor]]''', ''k'', is the average number of neutrons from one fission that cause another fission. The remaining neutrons either are absorbed in non-fission reactions or leave the system without being absorbed.  The value of ''k'' determines how a nuclear chain reaction proceeds:
 
*''k'' < 1 ([[subcriticality]]): The system cannot sustain a chain reaction, and any beginning of a chain reaction dies out over time. For every fission that is induced in the system, an average ''total'' of 1/(1&nbsp;&minus;&nbsp;''k'') fissions occur.
 
*''k'' = 1 ([[critical mass|criticality]]): Every fission causes an average of one more fission, leading to a fission (and power) level that is constant.  Nuclear power plants operate with ''k'' = 1 unless the power level is being increased or decreased.
 
*''k'' > 1 ([[supercriticality]]): For every fission in the material, it is likely that there will be "''k''" fissions after the next ''mean generation time.''  The result is that the number of fission reactions increases exponentially, according to the equation <math>e^{(k-1)t/\Lambda}</math>, where t is the elapsed time. Nuclear weapons are designed to operate under this state.  There are two subdivisions of supercriticality: prompt and delayed.
When describing kinetics and dynamics of nuclear reactors, and also in the practice of reactor operation, the concept of reactivity is used, which characterizes the deflection of reactor from the critical state. ρ=(k-1)/k. [[InHour]] is a unit of reactivity of a nuclear reactor.
 
In a nuclear reactor, ''k'' will actually oscillate from slightly less than 1 to slightly more than 1, due primarily to thermal effects (as more power is produced, the fuel rods warm and thus expand, lowering their capture ratio, and thus driving ''k'' lower). This leaves the average value of ''k'' at exactly 1. Delayed neutrons play an important role in the timing of these oscillations.
 
In an infinite medium, the multiplication factor may be described  by the [[four factor formula]]; in a non-infinite medium, the multiplication factor may be described  by the [[six factor formula]].
 
===Prompt and delayed supercriticality===
 
Not all neutrons are emitted as a direct product of fission;  some are instead due to the [[radioactive decay]] of some of the fission fragments.  The neutrons that occur directly from fission are called "[[prompt neutron]]s," and the ones that are a result of radioactive decay of fission fragments are called "delayed neutrons." The fraction of neutrons that are delayed is called β, and this fraction is typically less than 1% of all the neutrons in the chain reaction.<ref name=Duderstadt />
 
The delayed neutrons allow a nuclear reactor to respond several orders of magnitude more slowly than just prompt neutrons would alone.<ref name=Lamarsh />  Without delayed neutrons, changes in reaction rates in nuclear reactors would occur at speeds that are too fast for humans to control.
 
The region of supercriticality between k = 1 and k = 1/(1-β) is known as '''delayed supercriticality''' (or [[delayed criticality]]).  It is in this region that all nuclear power reactors operate.  The region of supercriticality for k > 1/(1-β) is known as '''prompt supercriticality''' (or [[prompt criticality]]), which is the region in which nuclear weapons operate.
 
The change in k needed to go from critical to prompt critical is defined as a [[Louis_Slotin#Dollar_unit_of_reactivity|dollar]].<ref>[http://www.sizes.com/units/dollar.htm Sizes.com]</ref>
 
==Nuclear weapons application of neutron multiplication==
 
Nuclear fission weapons require a mass of fissile fuel that is prompt supercritical.
 
For a given mass of fissile material the value of k can be increased by increasing the density. Since the probability per distance traveled for a neutron to collide with a nucleus is proportional to the material density, increasing the density of a fissile material can increase k.  This concept is utilized in the [[Nuclear weapon design#Implosion type weapon|implosion method]] for nuclear weapons. In these devices, the nuclear chain reaction begins after increasing the density of the fissile material with a conventional explosive.
 
In the [[gun-type fission weapon]] two subcritical pieces of fuel are rapidly brought together.  The value of k for a combination of two masses is always greater than that of its components. The magnitude of the difference depends on  distance, as well as the physical orientation.
 
The value of k can also be increased by using a [[neutron reflector]] surrounding the fissile material
 
Once the mass of fuel is prompt supercritical, the power increases exponentially.  However, the exponential power increase cannot continue for long since k decreases when the amount of fission material that is left decreases (i.e. it is consumed by fissions). Also, the geometry and density are expected to change during detonation since the remaining fission material is torn apart from the explosion.
 
===Predetonation===
Detonation of a nuclear weapon involves bringing fissile material into its optimal supercritical state very rapidly. During part of this process, the assembly is supercritical, but not yet in an optimal state for a chain reaction. Free  neutrons, in particular from [[spontaneous fission]]s, can cause the device to undergo a preliminary chain reaction that destroys the fissile material before it is ready to produce a large explosion, which is known as '''predetonation'''. To keep the probability of predetonation low, the duration of the non-optimal assembly period is minimized and fissile and other materials are used which have low spontaneous fission rates. In fact, the combination of materials has to be such that it is unlikely that there is even a single spontaneous fission during the period of supercritical assembly. In particular, the gun method cannot be used with plutonium (see [[nuclear weapon design]]).
 
== Nuclear power plants and control of chain reactions ==
{{main|nuclear reactor physics}}
Chain reactions naturally give rise to reaction rates that grow (or shrink) [[Exponential growth|exponentially]], whereas a nuclear power reactor needs to be able to hold the reaction rate reasonably constant. To maintain this control, the chain reaction criticality must have a slow enough time-scale to permit intervention by additional effects (e.g., mechanical control rods or thermal expansion). Consequently, all nuclear power reactors (even [[fast-neutron reactor]]s) rely on delayed neutrons for their criticality. An operating nuclear power reactor fluctuates between being slightly subcritical and slightly delayed-supercritical, but must always remain below prompt-critical.
 
It is impossible for a nuclear power plant to undergo a nuclear chain reaction that results in an explosion of power comparable with a [[nuclear weapon]], but even low-powered explosions due to uncontrolled chain reactions, that would be considered "fizzles" in a bomb, may still cause considerable damage and meltdown in a reactor. For example, the [[Chernobyl disaster]] involved a runaway chain reaction but the result was a low-powered steam explosion from the relatively small release of heat, as compared with a bomb. However, the reactor complex was destroyed by the heat, as well as by ordinary burning of the graphite exposed to air.<ref name=Lamarsh>{{cite book |last=Lamarsh |first=John |coauthors=Baratta, Anthony |title=Introduction to Nuclear Engineering |year=2001 |publisher=Prentice Hall |isbn=0-201-82498-1 }}</ref> Such steam explosions would be typical of the very diffuse assembly of materials in a [[nuclear reactor]], even under the worst conditions.
 
In addition, other steps can be taken for safety. For example, power plants licensed in the United States require a negative [[void coefficient]] of reactivity (this means that if water is removed from the reactor core, the nuclear reaction will tend to shut down, not increase). This eliminates the possibility of the type of accident that occurred at Chernobyl (which was due to a positive void coefficient). However, nuclear reactors are still capable of causing smaller explosions even after complete shutdown, such as was the case of the [[Fukushima Daiichi nuclear disaster]]. In such cases, residual [[decay heat]] from the core may cause high temperatures if there is loss of coolant flow, even a day after the chain reaction has been shut down (see [[SCRAM]]). This may cause a chemical reaction between water and fuel that produces hydrogen gas which can explode after mixing with air, with severe contamination consequences, since fuel rod material may still be exposed to the atmosphere from this process. However, such explosions do not happen during a chain reaction, but rather as a result of energy from radioactive [[beta decay]], after the fission chain reaction has been stopped.
 
== See also ==
* [[Chain reaction]]
* [[Critical mass (nuclear)|Critical mass]]
* [[Criticality accident]]
* [[Four factor formula]]
* [[Nuclear criticality safety]]
* [[Nuclear physics]]
* [[Nuclear reaction]]
* [[Nuclear reactor physics]]
* [[Nuclear weapon design]]
 
== References ==
<references />
 
== External links ==
* [http://www.atomicarchive.com/Movies/Movie1.shtml Nuclear Chain Reaction Animation]
* [http://alsos.wlu.edu/adv_rst.aspx?query=nuclear+chain+reaction&method=exact&source=all&genre=all&disc=all&level=all&selection=keyword&sortby=creator&results=10&period=15 Annotated bibliography on nuclear chain reactions from the Alsos Digital Library]
* [http://chair.pa.msu.edu/applets/chain/a.htm Stochastic Java simulation of nuclear chain reaction] by Wolfgang Bauer
 
{{DEFAULTSORT:Nuclear Chain Reaction}}
[[Category:Nuclear physics|Chain reaction, nuclear]]
 
[[ml:ആണവ ചെയിന്‍ റിയാക്ഷന്‍]]

Latest revision as of 11:37, 15 November 2014


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