/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q4CQ Question: Why might a flat-bott... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Question:Why might a flat-bottom finite well be a better approximation of the potential well confining nucleons than a Coulomb well tapering to a lowest energy in the middle

Short Answer

Expert verified

Answer

The answer is 1287.

Step by step solution

01

Given data

The strong force is much stronger than the Coulomb force within the nucleus.

02

Definition of Potential Well

The finite potential well (also known as the finite square well) is a concept from quantum mechanics.

A particle is contained in a "box" with finite potential "walls" as an extension of the infinite potential well.

03

Explain which is better approximation of potential well confining nucleons amongst flat bottom finite well and coulomb well.

The potential confining the nucleons have contribution from the strong interaction attractions between all nucleons and the coulomb repulsion between all pairs of protons.

The strong force is much stronger than the Coulomb force within the nucleus.

Thus, the potential is more like a fiat bottom well, which is a good approximation of the strong interaction attraction potential when nucleons are close, than a Coulomb well.

In fact, the nucleons would not keep together if only Coulomb force exists.

The repulsion will cause all the protons to fly apart.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

In both D-D reactions in equation (11-18). Two deuterons fuse to produce two particles, a nucleus ofA=3 and a free nucleon. Mass decreases because the binding energy of theA=3nucleus is greater than the combined binding energies of the two deuterons. The binding energy of helium-4is even greater still. Why can't the deuterons simply fuse into a helium-4nucleus and nothing else? Why must multiple particles be produced?

Equation (9-42) gives the Fermi energy for a collection of identical fermions packed into the lowest energies allowed by the exclusion principle. Argue that if applied to neutrons or protons (ignoring their repulsion) in a nucleus. the equation suggests that the Fermi energy is roughly the same for all nuclei. Making the rough approximation that the spacing between quantum levels is a constant in a given nucleus, argue that this spacing should vary from one nucleus to another in proportion toA-1 .

(a) Calculatethe binding energies per nucleon of the isobars boron- 12, carbon- 12, and nitrogen- 12.

(b) In which ofthe terms of the semiempirical binding energy formula do these binding energies differ, and how should these differences affect the binding energy per nucleon?

(c) Determine the binding energy per nucleon using the semiempirical binding energy formula and discuss the result.

The vast majority of measured nuclear spins are fairly small, between zero and nine times 12h . More to the point. Nuclear spin does not uniformly increases with A. Argue that if the assumptions in the shell model are valid then these observations are not unexpected.

Question:How is it that a high binding energy is a low energy?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.