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Question: A particle is trapped in a spherical infinite well. The potential energy is 0for r < a and infinite for r > a . Which, if any, quantization conditions would you expect it to share with hydrogen, and why?

Short Answer

Expert verified

Answer:

The particle will have the same quantization which is found in hydrogen.

Step by step solution

01

Identification of the given data 

The given data is listed as follows,

Potential Energy=0r<a1r>a
02

Significance of infinite potential well

The infinite potential well also called a particle in a box model describes a particle in such a state that, it is free to move in a determined space but surrounded by barriers that are impossible to penetrate.

03

Determination of the quantization conditions of particles related to that of hydrogen 

The potential energy defined in the given is a radial force, because it depends only on. So, all the angular parts of the Schrodinger Equation and the angular momentum quantization resulting from that will have the same quantization which is found in the hydrogen.

Thus, the particle will have the same quantization which is found in hydrogen.

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Most popular questions from this chapter

Exercise 80 discusses the idea of reduced mass. When two objects move under the influence of their mutual force alone, we can treat the relative motion as a one particle system of mass ฮผ=m1v2/(m1+m2). Among other things, this allows us to account for the fact that the nucleus in a hydrogen like atom isnโ€™t perfectly stationary, but in fact also orbits the centre of mass. Suppose that due to Coulomb attraction, an object of mass m2and charge -eorbits an object of mass m1 and charge +Ze . By appropriate substitution into formulas given in the chapter, show that (a) the allowed energies are Z2ฮผmE1n2, where is the hydrogen ground state, and (b) the โ€œBohr Radiusโ€ for this system is mzฮผa0 ,where a0is the hydrogen Bohr radius.

Question: Verify the correctness of the normalization constant of the radial wave function given in Table 7.4 as

1(2a0)3/23a0

Consider two particles that experience a mutual force but no external forces. The classical equation of motion for particle 1 is vห™1=F2on1/m1, and for particle 2 is vห™2=F1on2/m2, where the dot means a time derivative. Show that these are equivalent to vห™cm=constant, and vห™rel=FMutual/ฮผ .Where, vห™cm=(m1vห™1+m2vห™2)/(m1m2),FMutual=-Fion2andฮผ=m1m2(m1+m2).

In other words, the motion can be analyzed into two pieces the center of mass motion, at constant velocity and the relative motion, but in terms of a one-particle equation where that particle experiences the mutual force and has the โ€œreduced massโ€ ฮผ.

Taking then=3states as representative, explain the relationship between the complexity numbers of nodes and antinodes-of hydrogen's standing waves in the radial direction and their complexity in the angular direction at a given value of n. Is it a direct or inverse relationship, and why?

At heart, momentum conservation is related to the universe being "translationally invariant," meaning that it is the same if you shift your coordinates to the right or left. Angular momentum relates to rotational invariance. Use these ideas to explain at least some of the differences between the physical properties quantized in the cubic three-dimensional box versus the hydrogen atom.

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