CH 301 Ch12 notes part 2

# CH 301 Ch12 notes - CH301 Chapter 12 Notes Part 2 Solution to the Schrdinger Equation The Particle in a 1-Dimensional Box 1/2 sin(n x/L n(x =(2/L

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CH301 Chapter 12 Notes: Part 2: Solution to the Schrödinger Equation: The Particle in a 1-Dimensional Box < n (x) = (2/L) 1/2 sin(n 3 x/L) This equation summarizes a set of n sinusoidal curves: < 1 ± < 2 ± < 3 ± < 4 ± < 5 ……… Allowed energies of a particle in a 1-D box: E n = n 2 h 2 8mL 2 Each solution has its own specific energy: E 1 ± E 2 ± E 3 ± E 4 ± E 5 …………. n is known as a QUANTUM NUMBER. In this case, n is a positive, nonzero integer. Any other value of n would not work - it would not be a solution to the Schrödinger equation! What happens to E for any value of n if we let m or L increase? Figure 12.14 shows the energies, wavefunctions and square of the wavefunctions for the first three solutions (n=1, n=2, n=3). In class we'll discuss the third one in detail. Interpreting the solution for a particle in a 1-D box (Figure 12.14): Each wavefunction is equal to zero at x = 0 and x = L (as required by the boundary conditions) Note the energy level ‘ladder’ -- QUANTIZED energies. Sketch the plots of to < 3 and < ² 2 here and add the comments/notes: Remember < 2 gives the idea of WHERE the particle is likely to be! How does this compare to what you would expect for a macroscopic object? What do I need to know? Be able to sketch and interpret any of the first 8 or so solutions: e.g., < ² ± or < ³ 2 …. Where are the NODES. What is a Node? Where will you be most/least likely to find the particle? What does < 2 mean? Energy needed to jump from one level to another: (Figure 12.14) ' E = (n 2 2 -n 1 2 ) h 2 8mL 2 We can calculate the energy to go from < n 1 to level < n 2 : where n 1 and n 2 are two different values of n. We see that the gaps themselves, ' E, are also inversely proportional to L (actually L 2 ) and m. Example: A ball mass 0.5g in a 1D box 2m long: What energy is needed to go from n=4 to n=7 ? Zero Point Energy: Quantum Weirdness What about n=0? < 0 does NOT exist! The smallest allowed value of n is 1. The energy of a particle in a 1-D box can never be zero! To calculate ZPE use n=1 and your values of m and L. Example: Assume we confine all of these in 1-D boxes 100cm long: - an electron - a marble - a bowling ball Which do you think has the smallest ZERO POINT ENERGY?

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What do I need to know? Be able to sketch the energy level diagram and interpret it: (what happens as we change n,L) Be able to do calculations of values of E for a particular wavefunction given n,m,L Be able to calculate ' E for a particular wavefunction given two values of n, and m,L Be able to calculate the ZPE if given m,L (obviously you know what n is!!! ) Also the sort of qualitative examples we’ve done. Always remember that you should get very tiny numbers if your object is macroscopic. Why? The Schrodinger Equation for the H atom
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## This note was uploaded on 11/02/2010 for the course CH 50985 taught by Professor Sarasutcliffe during the Fall '10 term at University of Texas at Austin.

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CH 301 Ch12 notes - CH301 Chapter 12 Notes Part 2 Solution to the Schrdinger Equation The Particle in a 1-Dimensional Box 1/2 sin(n x/L n(x =(2/L

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