Presentation is loading. Please wait.

Presentation is loading. Please wait.

Chapter 5: Quantum Mechanics

Similar presentations


Presentation on theme: "Chapter 5: Quantum Mechanics"— Presentation transcript:

1 Chapter 5: Quantum Mechanics
Limitations of the Bohr atom necessitate a more general approach de Broglie waves –> a “new” wave equation “probability” waves classical mechanics as an approximation Wave Function Y probability amplitude

2 Mathematical properties of the wave function

3 More mathematical properties of the wave function

4 The classical wave equation as an example of a wave equation:

5

6 Time dependent Schrödinger Equation
linear (in Y) partial differential equation

7 Expectation values (average values)

8 If the potential energy U is time independent,
Schrödinger equation can be simplified by “factoring” separation of variables Total energy can have a constant (and well defined) value Consider plane wave: An eigenvector, eigenvalue problem!

9 The time independent Schrödinger equation
Allowed values for (some) physical quantities such as energy are related to the eigenvalues/eigenvectors of differential operators eigenvalues will depend on the details of the wave equation (especially in U) and on the boundary conditions

10 Particle in a box: (infinite) potential well
U Particle in a box: (infinite) potential well L V0 x

11 Wavefunction normalization

12 Example Find the probability that a particle trapped in a box L wide can be found between .45L and .55L for the ground state and for the first excited state. Example 5.4 Find <x> for a particle trapped in a box of length L

13 Particle in a box: finite potential well
U Particle in a box: finite potential well L V0 E x I II III

14 U Boundary Conditions L V0 E x I II III

15

16 c = 4 c = 100 c = 1600

17 Tunneling U L V0 E x I II III

18 U Boundary Conditions L V0 E x I II III

19

20 Example 5. 5: Electrons with 1. 0 eV and 2
Example 5.5: Electrons with 1.0 eV and 2.0 eV are incident on a barrier 10.0 eV high and 0.50 nm wide. (a) Find their respective transmission probabilities. (b) How are these affected if the barrier is doubled in width?

21 Harmonic Oscillator: classical treatment

22 Quantum Oscillator

23

24 Quantum Harmonic Oscillator Solutions

25 Operators

26 Example 5. 6: An eigenfunction of the operator d 2 /dx 2 is y = e2x
Example 5.6: An eigenfunction of the operator d 2 /dx 2 is y = e2x. Find the corresponding eigenvalue.

27 Chapter 5 exercises: 4, 5, 6, 11, 23


Download ppt "Chapter 5: Quantum Mechanics"

Similar presentations


Ads by Google