beautypg.com

Exp 12: image formation from spherical mirrors – PASCO OS-8500 INTRODUCTORY OPTICS SYSTEM User Manual

Page 66

background image

Introductory Optics System

012-02744K

®

60

Exp 12: Image Formation from Spherical Mirrors

Focal Length

60 mm

Remove the viewing screen and focus an image of
the crossed arrow target on itself. In this position,
the focal length will be half of the distance be-
tween the target and the mirror. This method gives
a focal length of 49.5 mm

Magnification

f = -50

ho = 32

do (mm)

di

hi

1/di + 1/d

1/f

hi/ho

-di/do

% f

% m

500

N/A

N/A

N/A

N/A

N/A

N/A

N/A

N/A

450

N/A

N/A

N/A

N/A

N/A

N/A

N/A

N/A

400

N/A

N/A

N/A

N/A

N/A

N/A

N/A

N/A

350

N/A

N/A

N/A

N/A

N/A

N/A

N/A

N/A

300

-37

3.0

-0.02

-0.02

0.09

0.12

15.59%

-31.56%

250

-52

3.5

-0.02

-0.02

0.11

0.21

-31.31%

-90.17%

200

-46

4.5

-0.02

-0.02

0.14

0.23

-19.48%

-63.56%

150

-35

5.5

-0.02

-0.02

0.17

0.23

8.70%

-35.76%

100

-30

7.0

-0.02

-0.02

0.22

0.30

14.29%

-37.14%

75

-23

9.5

-0.03

-0.02

0.30

0.31

33.65%

-3.30%

50

-21

12.0

-0.03

-0.02

0.38

0.42

27.59%

-12.00%

f = 50

ho = 19

do (mm)

di

hi

1/di+1/do

1/f

hi/ho

-di/do

% f

% m

500

55

-2.0

0.02

0.02

-0.11

-0.11

0.90%

-4.50%

450

56

-2.5

0.02

0.02

-0.13

-0.12

0.40%

5.42%

400

57

-3.0

0.02

0.02

-0.16

-0.14

0.22%

9.75%

350

58

-3.5

0.02

0.02

-0.18

-0.17

0.49%

10.04%

300

60

-4.0

0.02

0.02

-0.21

-0.20

0.00%

5.00%

250

62

-4.5

0.02

0.02

-0.24

-0.25

0.64%

-4.71%

200

66

-6.0

0.02

0.02

-0.32

-0.33

0.75%

-4.50%

150

76

-10.0

0.02

0.02

-0.53

-0.51

-0.88%

3.73%

100

100

-19.0

0.02

0.02

-1.00

-1.00

0.00%

0.00%

Virtual Images

Note: It is difficult to accurately locate the
virtual images. Because of this difficulty, the
accuracy of the second part of this lab does not
compare to the accuracy of the first. In addition,
the image of the virtual image finder is too small
to use at longer distances, so only the shorter
ones should be used.

Note: The final two data points are not
available because the image is located on the
opposite side of the target from the mirror. In
other words, the view of the image is blocked by
the object.

The results are in very good agreement with the
fundamental lens equation. The magnifications are
not as accurate, due to the difficulty in measuring
the size of the image accurately.