To begin, one had to measure the focal length of the lense and this was accomplished by using an infinite light source--the sun. The focal length was distance between the lense and the sharp point on the surface where all the sun rays collected. The focal length was measured to be 20 +/-1 cm.
The lense was then moved to 2 focal lengths:
D-o = 40 +/- .5 cm H-o = 9 +/- .5 cm
D-i = 36 +/- .5cm H-i = 8.5+/- .05 cm
M = .94 +/- .058
*After flipping the lense again, nothing was changed--all numbers are the same and the image was still real and inverted.
The lense was then moved to 1.5 focal lengths:
D-o = 30 +/- .5 cm H-o = 9 +/- .5 cm
D -i = 52 +/- .5 cm H-i = 16 =/- .5 cm
M = 1.78 +/- .153
*Once again the image was real and inverted and numbers did not change after flipping the lense.
The next part of the experiment consisted of applying the same technique of moving the lense to various distances from the object. The object was no longer the fillament but a small key chain that had the form of a bear. The following data was obtained.
Object distance (cm) | Image distance (cm) | object height (cm) | image height (cm) | M | Type of image | |||
5f | 23 +/- .5 | 5.1 +/- .05 | 1.7 +/- .05 | 0.333 +/- .0131 | real,inverted | |||
4f | 24.5 +/- .5 | 5.1 +/- .05 | 2 +/- .05 | 0.392 +/- .0136 | real, inverted | |||
3f | 28 +/- .5 | 5.1 +/- .05 | 2.5 +/- .05 | 0.49 +/- .0057 | real, inverted | |||
2f | 32 +/- .5 | 5.1+/- .05 | 3.2 +/- .05 | 0.627 +/- .0159 | real, inverted | |||
The graph above is one over the image distance versus negative one over the object distance. The y-intercept represents one over the focal length 1/f. Initially the focal lenth was measured to be 20 +/- 1 cm. However with respect to the graph, the focal length is 19.69 cm. This yields a percent difference 1.5 percent which is within error range. More importantly the lab supports the idea that 1/D-i + 1/D-o = 1/f.
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