Using Egs=-79.0eV for the ground state energy of helium, calculate the ionization energy (the energy required to remove just one electron). Hint: First calculate the ground state energy of the helium ion, He+, with a single electron orbiting the nucleus; then subtract the two energies.

Short Answer

Expert verified

The first ionization energy is 24.6eV.

Step by step solution

01

Definition of the hyperfine harmonic oscillator

A harmonic oscillator is a system that experiences a restoring forceFproportionate to the displacement xwhen it is moved from its equilibrium position, where k is a positive constant.

02

The ionization energy

Subtract Helium's ground state energy from its first excited state yields the first ionization energy (energy necessary to remove one electron).

The energy of the Helium ion'sHe+ground state is equal to the energy of the first excited state.

So, calculate the ground state energy ofHe+as:

He+ is a Hydrogen like atom. It contains just one electron but two protons in its nucleus, which indicates it has only one electron.

Hydrogen atom energy,

EH=-13.6eVZ2n2

ForHydrogen ground state n = 1 , and Z = 1.

For helium, Z = 2, then the expression will be :

EHe=-13.6eV2212EHe=-54.4eV

Ground state energy for helium is:

Egs=-79.0eV

SubtractingEHe andEgs ground state energy as:

Ejoin=-54eV--79eV=24.6eV

Thus, the first ionization energy is 24.6eV.

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Most popular questions from this chapter

Apply the techniques of this Section to the H-and Li+ions (each has two electrons, like helium, but nuclear charges Z=1and Z=3, respectively). Find the effective (partially shielded) nuclear charge, and determine the best upper bound on Egs, for each case. Comment: In the case of H- you should find that (H)>-13.6eV, which would appear to indicate that there is no bound state at all, since it would be energetically favourable for one electron to fly off, leaving behind a neutral hydrogen atom. This is not entirely surprising, since the electrons are less strongly attracted to the nucleus than they are in helium, and the electron repulsion tends to break the atom apart. However, it turns out to be incorrect. With a more sophisticated trial wave function (see Problem 7.18) it can be shown that Egs<-13.6eVand hence that a bound state does exist. It's only barely bound however, and there are no excited bound states, soH- has no discrete spectrum (all transitions are to and from the continuum). As a result, it is difficult to study in the laboratory, although it exists in great abundance on the surface of the sun.

Although the Schrödinger equation for helium itself cannot be solved exactly, there exist “helium-like” systems that do admit exact solutions. A simple example is “rubber-band helium,” in which the Coulomb forces are replaced by Hooke’s law forces:

H=-ħ22m(12+22)+12mω2|r1-r1|2(8.78).

(a) Show that the change of variables from

r1,r2,tor1,r2,tou12(r1+r2),v12(r1+r2) (8.79).

turns the Hamiltonian into two independent three-dimensional harmonic oscillators:

H=[-ħ2mu2+12mω2u2]+[-ħ2mu2+121-λmω2u2](8.80)

(b) What is the exact ground state energy for this system?

(c) If we didn’t know the exact solution, we might be inclined to apply the method of Section 7.2 to the Hamiltonian in its original form (Equation 7.78). Do so (but don’t bother with shielding). How does your result compare with the exact answer? Answer:(H)=3ħω(1-λ/4)a.

If the photon had a nonzero mass mγ0, the Coulomb potential would be replaced by the Yukawa potential,

V(r)=-e24π0e-μrr (8.73).

Whereμ=mγc/ . With a trial wave function of your own devising, estimate the binding energy of a “hydrogen” atom with this potential. Assumeμa1 , and give your answer correct to order(μa)2 .

The fundamental problem in harnessing nuclear fusion is getting the two particles (say, two deuterons) close enough together for the attractive (but short-range) nuclear force to overcome the Coulomb repulsion. The “bulldozer” method is to heat the particles up to fantastic temperatures and allow the random collisions to bring them together. A more exotic proposal is muon catalysis, in which we construct a “hydrogen molecule ion,” only with deuterons in place of protons, and a muon in place of the electron. Predict the equilibrium separation distance between the deuterons in such a structure, and explain why muons are superior to electrons for this purpose.

Find the best bound on Egsfor the one-dimensional harmonic oscillator using a trial wave function of the form role="math" localid="1656044636654" ψ(x)=Ax2+b2.,where A is determined by normalization and b is an adjustable parameter.

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