| Index of refraction lab: |
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PROBLEMS: 3, 4, 7, 8, 9, 10, 11, 12, 15, 16, 20, 24, 25, 30, 31, 32, 38, 39, 43, 44, 45, 46, 47, 48, 49, 52 |
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TURN IN: 4, 8, 10, 12 (EC), 16, 20(EC), 24, 30, 32, 38, 44(EC), 46(EC), 48, 52 |
| 4. You need the angle theta that the ray between
the mirror and the nearest point on the floor that can be seen reflected
in the mirror. Then you'd use tan (theta) = 0.43/x.
You can find theta from the horizontal distance 2.20 m and the vertical length of the mirror. The correct ratio of these lengths gives you tan (theta) which allows you to compute x. |
| 8. Use equation 23-2. You can get f from given R. Set di = infinity. Solve for do. |
| 10. An upright image occurs in the case of (i) a convex mirror or (ii) a concave mirror when the do < f. However, only in case (ii) can the magnification be greater than 1. Thus use: 1/di + 1/do =
1/f m = - di/do |
| 16. This seems to be a convex mirror since magnifications m < 1. di = - 0.18 m and do = infinity. Use 1/di + 1/do = 1/f to find f. From this, find R. |
| 24. v = c/n. |
| 30. (a) Use equation 23-5 to find the angle with the normal when the ray is in the glass assuming the first angle is 43.5 degrees. n1*sin(theta1) = n2*sin(theta2) where 1 denotes the ray's incidence and reflection medium and 2 denotes it's transmission medium. Solve for the second angle. See figure 23-22. (b) Use equation 23-5 to find the angle with the normal when the ray is in the water assuming the first angle i has the value of the second angle 2 you solved for in part (a). . ni*sin(theta_i) = nf*sin(theta_f) where i denotes the ray's incidence and reflection medium and f denotes it's transmission medium. Solve for the final angle f. (c) Use equation 23-5 to find the angle with the
normal when the ray passes directly from air into water assuming
the first angle is 43.5 degrees. See figure 23-19. |
| 32. You really need a picture for this but here
goes: You can easily find the second angle, theta2, shown using
Snell's law: n1*sin(theta1) = n2*sin(theta2) where 1 denotes the
ray's incidence and reflection medium and 2 denotes it's
transmission medium.
With theta 2, you must geometrically find the angle
with the opposite face's normal theta3. Here's a suggestion: Thus, we have: Solve for theta_f. |
| 38. Zoom in on figure 23-24. From the critical
angle you want to find other quantities geometrically. Let x
be the horizontal beam displacement between the exit point of a
vertically fired beam and actual exit point.
Clearly, x/0.62 = tan(theta_c) where theta_c is the critical angle for a water-air interface. |
| 48. f = -1/(5.5) m. Use 1/di + 1/do = 1/f. Find the image distance given do. Then find magnification m to compute hf from hi = 0.0040 m. Is the image virtual or real? Assuming the object is upright, is the image upright or inverted? |
| 52. Let m = -1. That means -1 = -di/do or 1 = di/do . That is, di = do. If the image is real, then do > f. Thus, di > f and di = do. Plug in symbols and solve for do in terms of f: 1/di + 1/do = = 1/do + 1/do = 1/f . What is do ? Is do > f ? |
| more hints later. |