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Published byDontae Doxey Modified over 2 years ago

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**Semi-Empirical Mass Formula Applications – II Nucleon Separation Energies and Fission**

[Sec Dunlap]

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**The Semi-Empirical Mass Formula**

Let us see how this equation can be applied to Neutron Separation Energies Alpha Particle Decay Energies Fission

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**Single neutron separation energies**

Fig PULLING NEUTRONS OUT OF ODD-A NUCLIDES The arrows show the transitions from the odd A parabola to the even (A-1) parabolas for the two cases of (e,o)(o,o) breaking pairing on neutron side (o,e)(e,e) breaking no pairing bond

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**Single neutron separation energies**

In an earlier lecture we found that the separation energy for a neutron was: This can be written in terms of mass of constituents and binding energies B to o-o Even Odd A 1 to e-e Apply the SEMF assuming B(A,Z) is continuous in A.

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**Single neutron separation energies**

Now apply the SEMF: This is an interesting result because it can give us an equation for the “neutron drip” line by putting Sn=0

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Mass Parabolas Z=N Proton number Neutron drip line Neutron number

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Alpha Particle Decay Q We saw in a previous lecture that the Q-value (energy released) in -decay is: where From which:

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Alpha Particle Decay Q

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**Energy released in Fission**

The diagram shows the Q (energy released) from the fission of 236U as a function of the A of one of the fragments (as obtained from the SEMF). Note that maximum energy release is 210MeV/Fission for the nucleus splitting into equal fragments.

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**Energy released in Fission**

This figure shows the prediction of the SEMF for the energy released in FISSION when two equal fragments are formed.

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**Energy released in Fission**

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**The Fission Barrier Fission barrier**

The origin of the fission barrier can be seen by reversing the fission process. Two fission fragments approach with (1/r) potential – consider the fragments equal. When r decreases until the two fragments are nearly touching the nuclear attractive strong force takes over – the potential energy is less than that calculated by Coulomb law.

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**Understanding the Fission Barrier**

Consider the stability of an Ellipsoidal Deformation, =eccentricity of ellipse How do BS and BC vary on deformation?

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**Understanding the Fission Barrier**

SURFACE ENERGY The surface area increases on deformation and so does BS. The nucleus becomes LESS bound Surface tenstion The mass energy increases with deformation – This produces a potential that seeks to keep =0, I.E. the nucleus in SPHERICAL condition

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**Understanding the Fission Barrier**

COULOMB ENERGY The Coulomb energy has the opposite tendency. On deformation the charge in the nucleus is less condensed – the electrostatic “blow apart” energy is less Nuclear deformation makes the nucleus MORE BOUND.

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**Understanding the Fission Barrier**

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**The fission barrier on the SEMF**

To calculate the height of the fission barrier using the SEMF is fairly complex, but can be done as seen in this study – Fig12.3 Dunlap. The dotted lines show variations that are understood on the shell model. Note that the barrier is only small ~3MeV for A>250.

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The Fissionability The Fissionability parameter Z2/A as a function of A. Note that the fastest decaying man-made transuranics still have F<45

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**The rate of spontaneous fission**

NOTE log of the decay rate (period) is approximately proportional to the fissionability Z2/A

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Nuclear Physics Lesson 13

Nuclear Physics Lesson 13

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