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In high-temperature sources, sodium atoms emit a doublet with an average wavelength of 1139 nm. The transition responsible is from the 4s to 3p state. Set up a spreadsheet to calculate the ratio of the number of excited atoms in the 4s state to the number in the ground 3s state over the temperature range from an acetylene-oxygen flame (3000°C) to the hottest part of an inductively coupled plasma source 8750°C).

Short Answer

Expert verified

The ratio of sodium atom at the acetylene-oxygen flame,3000C=0.063128709

The ratio of sodium atom at an inductively coupled plasma source,data-custom-editor="chemistry" 8750°C=0.739341631

Step by step solution

01

Given information

In high-temperature sources, sodium atoms emit a doublet with an average wavelength of 1139 nm. The transition responsible is from the 4s to 3p state.

02

Explanation

Boltzmann equation is used for the calculation of the ratio. This equation tells that how much an atom or ion is populated as a function of temperature. This equation is given as-

NjN0=gjg0exp-EjKT

03

Calculation of Energy

And the calculation of the energy of atom and ion is done by the following formula-

Ej=hcλ

The wavelength for the Na atom when the transition of an atom occurs from 4s to 3p = 1139nm, Planck’s constant = 6.62607×10-34J.s, c=3×108m/s


localid="1645797748501" Ej=6.6207×10-34J.s×3×108m/s1139×10-9mEj=1.744×10-19J

For 4s is 2 and for 3p is 6. Thus, the ratio can be given as:

gjg0=62=3

04

Data on spreadsheet

Calculation of the ratio of excited state 4s to the ground state 3s for sodium atom is done by plotting a spreadsheet. Therefore, from the spreadsheet-

gjg0

3



1.74E-19


k

1.38E-19


T (℃)

T(K)

NjN0

3000

3273

0.063128709

3250

3523

0.083027718

3500

3773

0.105305209

3750

4023

0.129672246

4000

4273

0.155835534

4250

4523

0.183511052

4500

4773

0.212432389

4750

5023

0.242355284

5000

5273

0.273059559

5250

5523

0.304349331

5500

5773

0.336052158

5750

6023

0.368017546

6000

6273

0.400115144

6250

6523

0.43223281

6500

6773

0.464274679

6750

7023

0.496159323

7000

7273

0.527818022

7250

7523

0.559193195

7500

7773

0.590236979

7750

8023

0.620909954

8000

8273

0.651180024

8250

8523

0.681021421

8500

8773

0.71041383

8750

9023

0.739341631

9000

9273

0.767793232

05

Conclusion

The ratio of sodium atoms at 3000C=0.063128709

The ratio of sodium atom atdata-custom-editor="chemistry" 8750°C=0.739341631

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Most popular questions from this chapter

For Na atoms and Mg+ ions, compare the ratios of the number of atoms or ions in the 3p excited state to the number in the ground state in

(a) a natural gas–air flame (1800 K).

(b) a hydrogen-oxygen flame (2950 K).

(c) an inductively coupled plasma source (7250 K).

The Doppler effect is one of the sources of the line broadening in atomic absorption spectroscopy. Atoms moving toward the light source encounter higher-frequency radiation than atoms moving away from the

source. The difference in wavelength λexperienced by an atom moving at speed v (compared to one at rest) is λ/λ=v/c, where c is the velocity of light. Estimate the line width (in nanometers) of the lithium

line at 670.776 (6707.76 Å) when the absorbing atoms are at a temperature of (a) 2000 K and (b) 3120 K. The average speed of an atom is given by v=8KT/πm, where k is Boltzmann’s constant, T is the absolute temperature, and m is its mass.

The intensity of a line for atomic Li is much lower in a natural gas flame, which operates at 1800°C, than in a hydrogen-oxygen flame, whose temperature is 2700°C. Explain.

Why is the CaOH spectrum in Figure 8-8 so much broader than the sodium emission line shown in Figure 8-4?

In a study of line broadening mechanisms in low-pressure laser-induced plasmas, Gornushkina et al.10 present the following expression for the half width for Doppler broadening λDof an atomic line.

∆λD(T)=λ08kTln2Mc2

where λ0is the wavelength at the center of the emission line, k is Boltzmann’s constant, T is the absolute temperature, M is the atomic mass, and c is the velocity of light. Ingle and Crouch11 present a similar

equation in terms of frequencies.

vD=22(ln2)kTM1/2vmc

where vDis the Doppler half width and vmis the frequency at the line maximum.

(a) Show that the two expressions are equivalent.

(b) Calculate the half width in nanometers for Doppler broadening of the 4s4p transition for atomic nickel at 361.939 nm (3619.39 Å) at a temperature of 20,000 K in both wavelength and frequency units.

(c) Estimate the natural line width for the transition in (b) assuming that the lifetime of the excited state is 5×10-8s.

(d) The expression for the Doppler shift given in the chapter and in Problem 8-8 is an approximation that works at relatively low speeds. The relativistic expression for the Doppler shift is

λλ=1c-vc+v-1

Show that the relativistic expression is consistent with the equation given in the chapter for low atomic

speeds.

(e) Calculate the speed that an iron atom undergoing the 4s 4p transition at 385.9911 nm (3859.911 Å) would have if the resulting line appeared at the rest wavelength for the same transition in nickel.

(f) Compute the fraction of a sample of iron atoms at 10,000 K that would have the velocity calculated in (e).

(g) Create a spreadsheet to calculate the Doppler half width λDin nanometers for the nickel and iron lines cited in (b) and (e) from 3000–10,000 K.

(h) Consult the paper by Gornushkin et al. (note 10) and list the four sources of pressure broadening that they describe. Explain in detail how two of these sources originate in sample atoms.

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