Ch. 40----2, 4, 6, 8, 9, 15, 16, 20, 22, 23, 26, 28, 29, 32, 33, 34, 35 (DUE MAY 4TH) |
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| SAMPLE EXAMS #2 |
| REAL EXAM 3 |
| REAL EXAM 4 |
| We start with # 15 and continue to the end of the set. Note: hbar = h/(2*pi). |
| 15. For the so-called squared well potential of section 40.2, 2.00 eV = E1 = 0.625E1box, where E1box is the ground state of the electron confined to box given by equation 40.10, with n = 1. Find L. |
| 16. To escape, the energy needed is hc/lambda = Uo - E1 = Uo - 0.625E1box |
| 20. The longest wavelength lambda means the smallest change in energy: hc/lambda = E2 - E1 = 2.43E1box - 0.625E1box. Given lambda, find L. E1box is the ground state of the electron confined to box given by equation 40.10, with n = 1. Find L. |
| 22. T = Ge-2KL , where G is within equation 40.21. Evaluate for ratios E/Uo = 5/7, 5/9 and 5/13. |
| 23. We use the phonetic symbol Psi to
rep wave function. Note: hbar = h/(2*pi). 2
equations: (A) -(hbar /2m)*d2Psi/dx2 = E*Psi, with Psi = A*eikx + B*e-ikx . (B) -(hbar /2m)*d2Psi/dx2
+ Uo*Psi = E*Psi or |
| 26. See 22, applying Uo - E twice. |
| 28. Substitute into -(hbar /2m)*d2Psi/dx2 + (1/2)*k*x2*Psi = E*Psi where C*e-alpha*x2 , alpha = sqrt(mk')/(2hbar). Show E = published ground state energy. |
| 29. (a) hc/lambda = hc/(5.8x10 -6 m) (b) hbar *w = hbar*sqrt( k'/m) to find k'. |
| 32. Ratios: (a) C*e-alpha*x2
, alpha = sqrt(mk')/(hbar) and x2 = A2
= (hbar/k')*w. (b) C*e-alpha*x2 , alpha = sqrt(mk')/(hbar) and x2 = 4A2 =4* (hbar/k')*w. |
| 33. (a) m = 3.82x10 -26
and (1/2)*k'*(0.014 x10 -9)2 =
0.0075 eVx1.6x10-19 J. Find k' and w. From that
get ground state energy. (b) hbar*w = hbar*sqrt( k'/m). (c) hc/lambda = hbar*w |
| 34.
-(hbar /2m)*d2Psi/dx2 + Uo*Psi
= E*Psi or |
| 35. Continuous Psi leads to (A) A+ B = C and continuous derivative leads to (B) ik*(A - B) = ik'*C, where k and k' are the wave numbers x < 0 and x > 0, respectively. Solve for B and C in terms of A. Reproduce the answer in back of book. |