Chemical Principles
Chemical Principles
8th Edition
ISBN: 9781305581982
Author: Steven S. Zumdahl, Donald J. DeCoste
Publisher: Cengage Learning
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Chapter 12, Problem 165CP
Interpretation Introduction

Interpretation:Wavelength of light required to promote high energy ground state electron to lowest energy excited state is to be calculated.

Concept introduction:Wavefunction is defined as the function of wave that gives information about the properties of wave. For a particle in one dimension box energy is calculated as follows:

  E=n2h28mL2

Where,

  • E is energy of state.
  • n is energy level.
  • h isplanck’s constant.
  • m is mass of electron.
  • L is dimension of cubical box.

Expert Solution & Answer
Check Mark

Answer to Problem 165CP

Value of λ is 2470 nm .

Explanation of Solution

The expression to calculate energy of a cubical box is as follows:

  E=h28mL2(nx2+ny2+nz2)

Since eight electrons are occupied in allowed energy level and each level occupies two electrons. Therefore, energy for first four energy levels is calculated. The four energy levels are E1,1,1 , E1,1,2 , E1,2,1 and E2,1,1 . The energy of last three orbitals is same; therefore, it is a degenerate orbital. The expression to calculate energy of one level is as follows:

  E1,1,1=h28mL2(nx2+ny2+nz2)

Where,

  • E1,1,1 is energy of first level.
  • h isplanck’s constant.
  • m is mass of electron.
  • nx , ny and nz are energy levels in x , y and z direction respectively.
  • L is dimension of cubical box.

Value of nx is 1.

Value of ny is 1.

Value of nz is 1.

Substitute values in above equation.

  E=h28mL2(nx2+ny2+nz2)=h28mL2(1+1+1)=3h28mL2

Hence, energy of cubical box is 3h28mL2 .

Since energy of second, third and fourth level is same, therefore, expression used to calculate energy of highest energy level is as follows:

  E1,1,2=E1,2,1=E2,1,1=h28mL2(nx2+ny2+nz2)

Where,

  • E1,1,2 , E1,2,1 and E2,1,1 .is energy of second, third and fourth level.
  • h isplanck’s constant.
  • m is mass of electron.
  • nx , ny and nz are energy levels in x , y and z direction respectively.
  • L is dimension of cubical box.

Value of nx is 2 .

Value of ny is 2 .

Value of nz is 2 .

Substitute values in above equation.

  E1,1,2=E1,2,1=E2,1,1=h28mL2(nx2+ny2+nz2)=h28mL2((2)2+(2)2+(2)2)=6h28mL2

Hence, energy of second, third and fourth level in cubical box of is 6h28mL2 .

Excitation of electron from highest level to lowest excited state develops next energy levels. Thus, energy of energy levels that are also degenerate is as follows:

  E2,2,1=E1,2,2=E2,1,2=h28mL2(nx2+ny2+nz2)

Where,

  • E2,2,1 , E1,2,2 and E2,1,2 .is energies of excited level.
  • h isplanck’s constant.
  • m is mass of electron.
  • nx , ny and nz are energy levels in x , y and z direction respectively.
  • L is dimension of cubical box.

Value of nx is 3 .

Value of ny is 3 .

Value of nz is 3 .

Substitute values in above equation.

  E2,2,1=E1,2,2=E2,1,2=h28mL2(nx2+ny2+nz2)=h28mL2((3)2+(3)2+(3)2)=9h28mL2

Hence, energy of excited level in cubical box of is 9h28mL2 .

The transition of electron from high energy ground state electron to lowest energy excited state is calculated by difference in energy of degenerate levels. The expression for difference in energy is as follows:

  ΔE=9h28mL26h28mL2=3h28mL2

Where,

  • ΔE is energy change.
  • h isplanck’s constant.
  • m is mass of electron.
  • L is dimension of cubical box.

Value of h is 6.626×1034 Js .

Value of m is 9.1×1031 kg .

Value of L is 1.50 nm .

Substitute values in above equation.

  ΔE=3h28mL2=3(6.626×1034 Js)28(9.1×1031 kg)(1.50 nm)(1 nm109 m)=8.03×1020 J

Hence, change in energy is 8.03×1020 J .

The change in energy for transition is calculated is as follows:

  ΔE=hcλ

Rearrange above equation for λ .

  λ=hcΔE

Value of c is 2.998×108 m/s .

Value of ΔE is 8.03×1020 J .

Value of h is 6.626×1034 Js .

Substitute values in above equation.

  λ=hcΔE=(6.626×1034 Js)(2.998×108 m/s)8.03×1020 J(109 nm1 m)=2470 nm

Hence, value of λ is 2470 nm .

Conclusion

Value of λ is 2470 nm .

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Chapter 12 Solutions

Chemical Principles

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