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What about the winding of the frauliens 32.42, and 52in the hydroponics O-7In what spectral range do these lie?

Short Answer

Expert verified

λ32=10.26nm;λ42=7.6nm;λ52=6.79nm

Step by step solution

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01

Step: 1 Given information

The given hydronics areO-7

02

Calculation

Wecanbeginbyexpressingenergylevelsasfollows:$$\begin{aligned}E_{n}&=-\frac{13.6Z^{2}(eV)}{n^{2}}E_{3}-E_{2}=-13.6Z^{2}(eV)\cdot\left(\frac{1}{3^{2}}-\frac{1}{2^{2}}\right)\\E_{3}-E_{2}=\frac{hc}{\lambda_{32}}\\\lambda_{32}=\frac{hc}{E_{3}-E_{2}}\\\lambda_{32}=\frac{-13.6\cdot8^{2}\cdot1.6\cdot10^{-19}\cdot\left(\frac{1}{3^{2}}-\frac{1}{2^{2}}\right)}{10.26\mathrm{~nm}}\\\lambda_{32}&=10^{-34}\cdot3\cdot10^{8}\end{aligned}Wecanbeginbyexpressingenergylevelsasfollows:$$\begin{aligned}E_{n}&=-\frac{13.6Z^{2}(eV)}{n^{2}}E_{3}-E_{2}=-13.6Z^{2}(eV)\cdot\left(\frac{1}{3^{2}}-\frac{1}{2^{2}}\right)\\E_{3}-E_{2}=\frac{hc}{\lambda_{32}}\\\lambda_{32}=\frac{hc}{E_{3}-E_{2}}\\\lambda_{32}=\frac{-13.6\cdot8^{2}\cdot1.6\cdot10^{-19}\cdot\left(\frac{1}{3^{2}}-\frac{1}{2^{2}}\right)}{10.26\mathrm{~nm}}\\\lambda_{32}&=10^{-34}\cdot3\cdot10^{8}\end{aligned}uncaught exception: Invalid chunk

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En=-13.6Z2(eV)n2E3-E2=-13.6Z2(eV)·132-122

E3-E2=hcλ32

λ32=hcE3-E2λ32=-13.6·82·1.6·10-19·132-12210.26nmλ32=10-34·3·108

In the same approach, we can determine out 42and 52transitions:

λ42=hcE4-E2λ42=6.63·10-34·3·108-13.6·82·1.6·10-19·142-122

λ42=7.6nmλ52=hcE5-E2λ52=6.63·10-34·3·108-13.6·82·1.6·10-19·152-122λ52=6.79nm

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Most popular questions from this chapter

20.What is the quantum number of an electron confined in a 3.0-nm-long one-dimensional box if the electron's de Broglie wavelength is1.0nm ?

In the atom interferometer experiment of Figure 38.13, laser cooling techniques were used to cool a dilute vapor of sodium atoms to a temperature of 0.0010K=1.0mK. The ultracold atoms passed through a series of collimating apertures to form the atomic beam you see circling the figure from the left. The standing light waves were created from a laser beam with a wavelength of 590nm.

a. What is the rms speed vmeof a sodium atom (A-23)in a gas at temperature 1.0mK?

b. By treating the laser beam as if it were a diffraction grating. Calculate the first-order diffraction angle of a sodium atom traveling at the rms speed of part a.

c. how far apart are the points Band Cif the second sanding wave is 10cmfrom the first?

d. Because interference is observed between the two paths, each individual atom is apparently present at both points Band point CDescribe, in your own words, what this experiment tells you about the nature of matter.

Determine the wavelengths of all the possible photons that can be emitted from the n=4state of a hydrogen atom.

In the atom interferometer experiment shown in Figure 38.13laser cooling techniques were used to cool a dilute vapor of sodium atoms to a temperature of 0.0010K=1.0mK. The ultracold atoms passed through a series of collimating apertures to form the atomic beam you see circling the figure from the left. The standing light waves were created from a laser beam with a wavelength of 590nm.

a. What is the rms speed vmeof a sodium atom (A-23)in a gas at this temperature 1.0mK?

b. By treating the laser beam as if it were a diffraction grating. cakculate the first-order diffraction angle of a sodium atom traveling with the rms speed of part a.

c. allow far apart are points Band Cif the second sanding wave is 10cmfrom the first?

d. Because interference is observed between the two paths, each individual atom is apparently present at both point Band point C. Describe, in your own words, what this experiment tells you about the nature of matter.

Draw an energy-level diagram, similar to Figure 38.21, for the He+ion. On your diagram:

a. Show the first five energy levels. Label each with the values of n andEn

b. Show the ionization limit.

c. Show all possible emission transitions from the n = 4 energy level.

d. Calculate the wavelengths (in nm) for each of the transitions in part c and show them alongside the appropriate arrow.

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