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Section 10.2 gives the energy and approximate proton separation of the H2+ molecule. What is the energy of the electron alone?

Short Answer

Expert verified

The energy of the electron in H2+ is 29.4 eV.

Step by step solution

01

Given data 

The distance between two protons is 0.11nm.

02

Concept of potential energy

The potential energy between the two protons is given by a relation, U=14πε0e2a.

Here, ε0 is permittivity of the free space,e is charge on each proton, and role="math" localid="1658384048724" ais the distance between the two protons.

03

Determine the potential energy between two protons

Substitute8.85×1012 C2/Nm2 forε0,1.6×1019 Cfore,0.11 nmfora in the equationU=14πε0e2aand solve forU.

U=(1.6×1019 C)2(4π)(8.85×1012 C2/Nm2)(0.11 nm)U=(1.6×1019 C)2(4π)(8.85×1012 C2/Nm2)(0.11×109 m)U=2.09×1018J

Convert joules to electron volte.

U=2.09×1018J1eV1.6×1019JU=13.1eV

04

Determine the energy of electron in  H2+

The energy of the electron is given by the difference of the total energy and the proton's energy, Ee=ETU.

Here, Ee is the energy of the electron, ET is the total energy, and U is the energy of the proton.

Substitute16.3eVforETand13.1eVforUin the equationEe=ETUand solve forEe.

Ee=16.3eV13.1eVEe=29.4eV

Therefore, the energy of the electron in H2+ is role="math" 29.4eV.

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Most popular questions from this chapter

Question:If electrical conductivity were determined by the mere static presence of positive ions rather than by their motion the collision time would be inversely proportional to the electron's average speed. If however, it were dominated by the motion of the ions, it should be inversely proportional to the “area" presented by a jiggling ion, which is in turn proportional to the square of its amplitude as an oscillator. Argue that only the latter view gives the correct temperature dependence in conductors of σT-1. Use the equipartition theorem (usually covered in introductory thermodynamics and also discussed in Section 9.9).

The effective force constant of the molecular “spring” in HCL is 480N/m, and the bond length is 0.13nm.

(a) Determine the energies of the two lowest-energy vibrational states.

(b) For these energies, determine the amplitude of vibration if the atoms could be treated as oscillating classical particles.

(c) For these energies, by what percentages does the atomic separation fluctuate?

(d) Calculate the classical vibrational frequencyωvh=k/μand rotational frequency for the rotational frequencyωrot=L/I, assume that L is the its lowest non zero value, 1(1+1)hand that the moment of inertia Iis μa2.

(e) Is is valid to treat the atomic separation as fixed for rotational motion while changing for vibrational?

The left diagram in FIGURE 10.1 might represent a two atom crystal with two bands. Basing your argument on the kinetic energy inside either individual well, explain why both energies in the lower band should be roughly equal to that of the n=1 atomic state and why both energies in the upper should roughly equal that of the n=2 atomic state

As we see in Figures 10.23, in a one dimensional crystal of finite wells, top of the band states closely resemble infinite well states. In fact, the famous particle in a box energy formula gives a fair value for the energies of the band to which they belong. (a) If for nin that formula you use the number of anitnodes in the whole function, what would you use for the box length L? (b) If, instead, the n in the formula were taken to refer to band n, could you still use the formula? If so, what would you use for L? (c) Explain why the energies in a band do or do not depend on the size of the crystal as a whole.

Of N2, O2 and F2, none has an electric dipole moment, but one does have a magnetic dipole moment, which one, and why?

(Refer to figure 10.10)

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