Estimate the probability that a hydrogen atom at room temperature is in one of its first excited states (relative to the probability of being in the ground state). Don't forget to take degeneracy into account. Then repeat the calculation for a hydrogen atom in the atmosphere of the starγ UMa, whose surface temperature is approximately 9500 K.

Short Answer

Expert verified

As a result, no Hydrogen atoms can be found in the first excited state.

On this star, there is one atom in the first excited state out of 64500 hydrogen atoms.


Step by step solution

01

Given information

A hydrogen atom at room temperature is in one of its first excited states (relative to the probability of being in the ground state).

02

Explanation

With n = 2, assuming E1 is ground state energy and E2 is first excited state energy, the chance of finding the atom in either of the first excited states is:

Ps2=1Ze-E2/kT

The partition function is equal to the sum of the Boltzmann factors, but because the initial state has the greatest energy magnitude, we can approximate it as follows:

Z=se-E(s)/kTe-E1/kT

Substitute in the above equation

Ps2=eE1/kTe-E2/kTPs2=e-E2-E1/kT

There are four such states, therefore the probability of E2 equals Ps2multiplied by 4, so:

PE2=4e-E2-E1/kT

Substitute the energies and Boltzmann constant in eV (k = 8.617 x 10-5 eV/K) at room temperature T = 300 K for the energy of the ground state E1=-13.6 eV and the energy of the first excited state B2 =-3.4 eV.

PE2=4e-(-3.4eV-(-13.6eV))/8.617×10-5eV/K(300K)PE2=1.75×10-171

As a result, no Hydrogen atoms can be found in the first excited state.

03

Explanation

We must now calculate this probability for the star γUMa, which has a surface temperature of 9500 K, as follows:

PE2=4e-(-3.4eV-(-13.6eV))/8.617×10-5eV/K(9500K)PE2=1.55×10-5

On this star, there is one atom in the first excited state out of 64500 hydrogen atoms.

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Most popular questions from this chapter

Equations 6.92 and 6.93 for the entropy and chemical potential involve the logarithm of the quantity VZintNvQ. Is this logarithm normally positive or negative? Plug in some numbers for an ordinary gas and discuss.

Each of the hydrogen atom states shown in Figure 6.2 is actually twofold degenerate, because the electron can be in two independent spin states, both with essentially the same energy. Repeat the calculation given in the text for the relative probability of being in a first excited state, taking spin degeneracy into account. Show that the results are unaffected.

Consider an ideal gas of highly relativistic particles ( such as photons or fast-moving electrons) whose energy-momentum relation is E=pcinstead of E=p22m. Assume that these particles live in a one-dimensional universe. By following the same logic as above, derive a formula for the single particle partition function,Z1, for one particle in the gas.

This problem concerns a collection of N identical harmonic oscillators (perhaps an Einstein solid or the internal vibrations of gas molecules) at temperature T. As in Section 2.2, the allowed energies of each oscillator are 0, hf, 2hf, and so on. (

a) Prove by long division that

11-x=1+x+x2+x3+

For what values of x does this series have a finite sum?

(b) Evaluate the partition function for a single harmonic oscillator. Use the result of part (a) to simplify your answer as much as possible.

(c) Use formula 6.25 to find an expression for the average energy of a single oscillator at temperature T. Simplify your answer as much as possible.

(d) What is the total energy of the system of N oscillators at temperature T? Your result should agree with what you found in Problem 3.25.

(e) If you haven't already done so in Problem 3.25, compute the heat capacity of this system and check t hat it has the expected limits as T0 and T.

Consider a large system of Nindistinguishable, noninteracting molecules (perhaps an ideal gas or a dilute solution). Find an expression for the Helmholtz free energy of this system, in terms of Z1, the partition function for a single molecule. (Use Stirling's approximation to eliminate the N!.) Then use your result to find the chemical potential, again in terms ofZ1.

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