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A water molecule can vibrate in various ways, but the easiest type of vibration to excite is the "flexing' mode in which the hydrogen atoms move toward and away from each other but the HO bonds do not stretch. The oscillations of this mode are approximately harmonic, with a frequency of 4.8 x 1013Hz. As for any quantum harmonic oscillator, the energy levels are 12hf,32hf,52hf, and so on. None of these levels are degenerate.

(a) state and in each of the first two excited states, assuming that it is in equilibrium with a reservoir (say the atmosphere) at 300 K. (Hint: Calculate 2 by adding up the first few Boltzmann factors, until the rest are negligible.) Calculate the probability of a water molecule being in its flexing ground

(b) Repeat the calculation for a water molecule in equilibrium with a reservoir at 700 K (perhaps in a steam turbine).

Short Answer

Expert verified

The probability of water molecule is:

P1=0.9997P2=4.618×10-4P3=2.133×10-7

Step by step solution

01

Given information

A water molecule can vibrate in various ways, but the easiest type of vibration to excite is the "flexing' mode in which the hydrogen atoms move toward and away from each other but the HO bonds do not stretch. The oscillations of this mode are approximately harmonic, with a frequency of 4.8 x 1013Hz. As for any quantum harmonic oscillator, the energy levels are 12hf,32hf,52hf, and so on. None of these levels are degenerate.

02

Explanation

(a) The partition function is: because none of the levels are degenerate.

Z=∑se-E(s)/kT

Where,

E(s)=s+12hfs=0,1,2,…

So,

Z=e-hf/2kT+e-3hf/2kT+e-5hf/2kT+…

Let x=hf/kT, so

Z=e-x/2+e-3x/2+e-5x/2+…(1)

As a result, the value of z is (at T = 300 K, we substitute the Boltzmann constant in eV, k = 8.617x 10-5 eV/K, and the Planck constant in eV, h = 4.136 x 10-15 eV s):

x=4.136×10-15eV·s4.8×1013Hz8.617×10-5eV(300K)=7.68

Substitute x into (1)

Z=e-(7.68)/2+e-3(7.68)/2+e-5(7.68)/2Z=0.0215

Probability of first state is:

P=1Ze-x/2

Substitute with x and z:

role="math" localid="1647366550518" P1=10.0215e-7.68/2P1=0.9997

Probability of second state is:

P2=1Ze-3x/2

Substitute x and z:

role="math" localid="1647366573852" P2=10.0215e-3(7.68)/2P2=4.618×10-4

Probability of third state:

P3=1Ze-3x/2

Substitute x and z:

role="math" localid="1647366591263" P3=10.0215e-5(7.68)/2P3=2.133×10-7

03

Explanation

We have temperature value, T=300k, so

x=4.136×10-15eV·s4.8×1013Hz8.617×10-5eV(700K)=3.2913

Substitute x into (1):

role="math" localid="1647366281815" Z=e-(3.2913)/2+e-3(3.2913)/2+e-5(3.2913)/2Z=0.20033

Substitute the value of x and z to get the probabilities:

P1=10.20033e-3.2913/2P1=0.962847P2=10.20033e-3(3.2913)/2P2=0.035823P3=10.20033e-5(3.2913)/2P3=0.001333

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Most popular questions from this chapter

Carefully plot the Maxwell speed distribution for nitrogen molecules at T=300K and atT=600K. Plot both graphs on the same axes, and label the axes with numbers.

The most common measure of the fluctuations of a set of numbers away from the average is the standard deviation, defined as follows.

(a) For each atom in the five-atom toy model of Figure 6.5, compute the deviation of the energy from the average energy, that is, Ei-E¯,fori=1to5. Call these deviations ΔEi.

(b) Compute the average of the squares of the five deviations, that is, ΔEi2¯. Then compute the square root of this quantity, which is the root-mean- square (rms) deviation, or standard deviation. Call this number σE. Does σEgive a reasonable measure of how far the individual values tend to stray from the average?

(c) Prove in general that

σE2=E2¯-(E¯)2

that is, the standard deviation squared is the average of the squares minus the square of the average. This formula usually gives the easier way of computing a standard deviation.

(d) Check the preceding formula for the five-atom toy model of Figure 6.5.

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 T→0 and T→∞.

Use a computer to sum the rotational partition function (equation 6.30) algebraically, keeping terms through j = 6. Then calculate the average energy and the heat capacity. Plot the heat capacity for values ofkT/ϵ ranging from 0 to 3. Have you kept enough terms in Z to give accurate results within this temperature range?

Suppose you have 10 atoms of weberium: 4 with energy 0 eV, 3 with energy 1 eV, 2 with energy 4 eV, and 1 with energy 6 eV.

(a) Compute the average energy of all your atoms, by adding up all their energies and dividing by 10.

(b) Compute the probability that one of your atoms chosen at random would have energy E, for each of the four values of E that occur.

(c) Compute the average energy again, using the formulaE¯=∑sE(s)P(s)

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