Ch. 42----2, 3, 4, 5, 8, 9, 10, 12, 13, 15, 18, 19, 22, 24, 26, 27, 28, 29, 30, 32 |
| CLICK HYPERPHYSICS FOR SUMMARIES OF ALL UNDERGRADUATE PHYSICS TOPICS INCLUDING RELATIVITY, ATOMS, NUCLEI AND COSMOLOGY. |
| SAMPLE EXAMS #2 |
| REAL EXAM 3 |
| REAL EXAM 4 |
| 2. (a) Find U. See example 42.1. (b) See page 1434 about the additional "net investment " in pulling molecule apart and returning electron to the sodium (Na) , which "donated" it to Cl when the two elements formed an ionic bond. Total binding energy is |U + 3.5 eV - 4.3 eV |; see page 1434. This is how much work you have to do to pull the molecule apart and separate the neutral atoms. - |
| 3. This transition is not consistent with photon selection rules. See Figure 42.5. 5*hbar2/I = hc/lambda; find I and find inter-atomic distance from I formula. |
| 4. This transition is more consistent with photon selection rules. hc/lambda = hbar2/I . Oven frequency should be near f you found for maximum absorption of heat. |
| 5. (a) Eqn 42.5 (b) They should agree. |
| 8. This transition is consistent with photon selection rules: change in n = 1. See Eqn 42.8. Set hc/lambda = expression for change in E. Find k'. |
| 9.(a) 4*hbar2/I Compute I to complete problem. (b) hc/lambda = 4*hbar2/I . |
| 10. (i) 2*hbar2/I
= hc/lambda = 8.841x10 -4 eV and (ii) hc/lambda' =
0.2560 eV = expression for change in E. Find k'.
From (i) get mass & use in (ii) for k'. |
| 12. Now E = E(l, n) is a function of two variables, l and n, given by equation 42.9. (a) Set hc/lambda = E(1, 2) - E(0,1) Use similar substitutions for part (b) and (c). |
| 13. (a) Equation 42.8. (b) Equation 42.8. (c ) E = E(n). Set hc/lambda = E(n + 1) - E(n) = right side of equation 42. 8 |
| 15. Use simple cubic: (atom mass/L3, where L is given. Use average of Na and Cl atom for atom mass |
| 18. (a), (b) , (c) based on hc/lambda = Eg. |
| 19. hc/lambda = n*(1.12 eV); find n. |
| 22. Review Ch. 18, equation 18.19, to get vrms then compare with v in example 42.9. |
| 24. Eliminate nrs by taking the square root of both sides of 42.13. Solve for nrs in terms of E. The substitute into equation 42.12 to get 42.14.. |
| 26. EF is derived on page
1450. It is given by the total number of electrons N . On page
1450 we integrate 42.18 to get N at T = 0 and get the
fermi energy EF0 at absolute zero.
(a) Now that you know EF0 is
use it to evaluate equation 42.22. (c) Set kT = EF. |
| 27. Evaluate equation 42.17. Remember T is in Kelvin. |
| DISCUSSIONS TO COME |