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1 Controlled Fission 235 U + n X + Y + (~ 2.4) n Moderation of second generation neutrons Chain reaction. Water, D 2 O or graphite moderator. Ratio of.

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Presentation on theme: "1 Controlled Fission 235 U + n X + Y + (~ 2.4) n Moderation of second generation neutrons Chain reaction. Water, D 2 O or graphite moderator. Ratio of."— Presentation transcript:

1 1 Controlled Fission 235 U + n X + Y + (~ 2.4) n Moderation of second generation neutrons Chain reaction. Water, D 2 O or graphite moderator. Ratio of number of neutrons (fissions) in one generation to the preceding k (neutron reproduction or multiplication factor). k 1 Chain reaction. k < 1 subcritical. k = 1 critical system. k > 1 supercritical. For steady release of energy (steady- state operation) we need k =1. Fast second generation neutrons Infinite medium (ignoring leakage at the surface). Chain reacting pile Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh).

2 Controlled Fission allAverage number of all neutrons released per fission (for thermal neutrons, eV). 233 U : U : Pu : Pu : absorbedReactor is critical ( k = 1): rate of neutrons produced by fission = rate of neutrons absorbed + leaked. Size and composition of the reactor. 2Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh).

3 3 Probability for a thermal neutron to cause fission on 235 U is Controlled Fission 235 U thermal cross sections fission 584 b. scattering 9 b. radiative capture 97 b. fast If each fission produces an average of neutrons, then the mean number of fast fission neutrons produced per thermal neutron = < Check numbers!

4 4 Controlled Fission 235 U 238 U Assume natural uranium: % 238 U, % 235 U. f / N = ( )(0) + (0.0072)(584) = 4.20 b. / N = ( )(2.75) + (0.0072)(97) = 3.43 b. Thermal f = 0 b584 b Thermal = 2.75 b97 b Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). Using the experimental elastic scattering data the radius of the nucleus can be estimated. Doppler effect? Why?

5 5 natural uranium Probability for a thermal neutron to cause fission in natural uranium If each fission produces an average of = 2.4 neutrons, then the mean number of fast fission neutrons produced per thermal neutron = = 2.4 x This is close to 1. If neutrons are still to be lost, there is a danger of losing criticality. (Heavy water?). enriched uranium For enriched uranium ( 235 U = 3%) = ????? (> 1.3). (Light water?). In this case is further from 1 and allowing for more neutrons to be lost while maintaining criticality. Controlled Fission Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). Compare to pure 235 U and to 3% enriched fuel.

6 Moderation (to compare x-section) 1H1H (n, ) (n,n) 2H2H Resonances? 3 H production. 6Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh).

7 7 Controlled Fission Verify Comment on the calculation for thermal neutrons and a mixture of fissile and non-fissile materials, giving an example. Comment for fast neutrons and a mixture of fissionable materials, giving an example. HW 11

8 8 Converters: Convert non-thermally-fissionable material to a thermally-fissionable material. f,th = 742 b Nuclear Reactors, BAU, 1 st Semester, (Saed Dababneh). f,th = 530 b Conversion and Breeding 8Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). India

9 9 If = 2 Conversion and fission. If > 2 Breeder reactor. 239 Pu : Thermal neutrons ( ~ 2.1) hard for breeding. Fast neutrons ( ~ 3) possible breeding fast breeder reactors. After sufficient time of breeding, fissile material can be easily (chemically) separated from fertile material. Compare to separating 235 U from 238 U. Reprocessing. Nuclear Reactors, BAU, 1 st Semester, (Saed Dababneh). Conversion and Breeding Delicate neutron economy…! 9Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh).

10 10 Controlled Fission Note that is greater than 2 at thermal energies and almost 3 at high energies. These extra neutrons are Used to convert fertile into fissile fuel. Plutonium economy. India and thorium. Efficiency of this process is determined by neutron energy spectrum. Variations in Variations in

11 Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). 11 Controlled Fission Conversion ratio Conversion ratio CR is defined as the average rate of fissile atom production to the average rate of fissile atom consumption. For LWR's CR 0.6. CR is called BR for values > 1. Fast breeder reactors have BR > 1. They are called fast because primary fissions inducing neutrons are fast not thermal, thus η > 2.5 but σ f is only a few barns. Moderator??

12 12 Controlled Fission thermalhave produced so far N fast neutrons. N thermal neutrons in one generation have produced so far N fast neutrons. fast fast fission factor Some of these fast neutrons can cause 238 U fission more fast neutrons fast fission factor = (= 1.03 for natural uranium). Now we have N fast neutrons. We need to moderate these fast neutrons use graphite as an example for 2 MeV neutrons we need ??? collisions. How many for 1 MeV neutrons? strong The neutron will pass through the eV region during the moderation process. This energy region has many strong 238 U capture resonances (up to ????? b) Can not mix uranium and moderator. resonance escape probability In graphite, an average distance of 19 cm is needed for thermalization the resonance escape probability p ( 0.9). Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). Reactor design.

13 13 Controlled Fission Now we have p N thermal neutrons. Moderator must not be too large to capture thermal neutrons; when thermalized, neutrons should have reached the fuel. Graphite thermal cross section = b, but there is a lot of it present. Capture can also occur in the material encapsulating the fuel elements (clad). thermal utilization factor The thermal utilization factor f ( 0.9) gives the fraction of thermal neutrons that are actually available for the fuel. Now we have fp N thermal neutrons Now we have fp N thermal neutrons, could be > or < N thus determining the criticality of the reactor. The four-factor formula. k = fp The four-factor formula. k = k eff = fp (1- l fast )(1- l thermal ) Fractions lost at surface Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh).

14 14 k = fp, Fast from thermal, as defined in HW 11. Fast from fast,. Thermal from fast, p. Thermal available for fuel Thinking QUIZ For each thermal neutron absorbed, how many fast neutrons are produced? Will need this when discuss two-group diffusion. Controlled Fission

15 15 x 1.03 Fast fission factor Fast fission factor x 0.9 Resonance escape probability p x 0.9 Thermal utilization factor f x What is: Migration length? Critical size? How does the geometry affect the reproduction factor? Neutron reproduction factor k = Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). Neutron Life Cycle

16 16Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). Neutron Life Cycle Why should we worry about these? How?

17 Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). 17 k = fp (1- l fast )(1- l thermal ) Controlled Fission Thermal utilization factor f can be changed, as an example, by adding absorber to coolant (PWR) (chemical shim, boric acid), or by inserting movable control rods in & out. Reactors can also be controlled by altering neutron leakages using movable neutron reflectors. f and p factors change as fuel is burned. f, p, η change as fertile material is converted to fissile material. Not fixed…!

18 Nuclear Reactor Theory, JU, Second Semester, (Saed Dababneh). 18 Controlled Fission Attention should be paid also to the fact that reactor power changes occur due to changes in resonance escape probability p. If Fuel T, p due to Doppler broadening of resonance peaks. Under-moderation and over-moderation.


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