Introduction
The purpose of this experiment was
to observe how the image changes based on the object distance. In this
experiment, a meter stick, a converging lens, and a socket lamp with filament,
a lens holder, and a cardboard. First, the focal length of the lens was
determined by measuring the distance between the lens and the focus of the sun
rays. Then the object distances varying from 1.5f to 5f were computed using the
focal length. These computed distances were used to position the lens distance
from the filament. The set up of the apparatus was shown in figure 2. The
height of the filament was also measured. After turning the power on to let the
light shine through the filament, the cardboard distance from the lens was
adjusted till a sharp image was obtained. This image distance and its height
were also measured. After recording all these data, the magnification of the
lens was computed, and two graphs were constructed to observe the relationship
between the image and object distance, and the focal length.
Figure 1: Measuring the focal length of the converging lens
Figure 2: Experimental set-up
Figure 3: Image forming through the converging lens
Data and Analysis
Focal length (f) = 9.5 ± 0.25 cm
Table 1: Recorded data of the
object and image distances and heights
Object distance as a multiple of f(cm)
|
Object distance(cm)
|
Image distance(cm)
|
Object height(cm)
|
Image height(cm)
|
Type of image
|
5f
|
47.5 ± 1.25
|
16.50 ± 0.25
|
8.80 ± 0.25
|
3.30 ± 0.25
|
Inverted, real
|
4f
|
38.0 ± 1.00
|
17.00 ± 0.25
|
4.40 ± 0.25
|
Inverted, real
|
|
3f
|
28.5 ± 0.75
|
18.00 ± 0.25
|
6.60 ± 0.25
|
Inverted, real
|
|
2f
|
19.0 ± 0.50
|
25.50 ± 0.25
|
14.30 ± 0.25
|
Inverted, real
|
|
1.5f
|
14.3 ± 0.38
|
23.25 ± 0.25
|
16.50 ± 0.25
|
Inverted, real
|
Table 2: Comparison
of magnification from distance ratios and height ratios
Object distance as a multiple of f(cm)
|
Md (di/d0)
|
Mh (hi/h0)
|
% difference between Md and Mh
(%)
|
5f
|
0.347 ± 0.011
|
0.375 ± 0.030
|
5.10
|
4f
|
0.447 ± 0.013
|
0.500 ± 0.032
|
7.33
|
3f
|
0.632 ± 0.019
|
0.750 ± 0.036
|
11.1
|
2f
|
1.34 ± 0.04
|
1.63 ± 0.05
|
12.6
|
1.5f
|
1.63 ± 0.05
|
1.88 ± 0.06
|
9.28
|
Graph 1: Object distance vs. Image distance
Graph 2: Inverse image distance vs. Negative inverse object distance
Conclusion
According to table 1 and graph 1,
as the object distance decreased, the image distance increased. Therefore, the
image and object distance had inverse relationship as shown in graph 1. However,
at 1.5f, even though the object distance decreased, the image distance
decreased. This was because the image became dimmer and unclearer as the object
distance decreased. Hence, uncertainty became greater since it became harder to
see the actual height of the image. Another relationship observed in this
experiment was that the image height increased as the object distance decreased.
This was because the image distance got smaller. Besides, the image observed
was always inverted. Since the image formed by the converging lens was
inverted, the image was real. This idea was explained in experiment 9. As shown
in table 2, the magnification obtained from distance ratio and height ratio increased
as the object distance decreased. This agreed with the observation since the
image got larger as the object was nearer to the lens. However, most of these
values were not within the uncertainties of each other. This was possibly
because the focus was not as accurate as it should have been. Unclear images at
small object distances also contributed to this error.
According to graph 2, the inverse
image distance and inverse object distance had linear relationship. This
relationship actually described the relationship between the image distance,
object distance, and the focal length, which was 1/d0 + 1/di
= 1/f. The y-intercept 0.08178cm-1, obtained from the graph was the
inverse of the focal length of the lens. By taking the reciprocal of the
y-intercept, the graphical focal length was computed to be 12.23cm. However,
the measured focal length was 9.5cm. This large difference in focal length was contributed
by the image distance at 1.5f. As mentioned earlier, this was the only data set
that deviated from the image-object distance relationship. This smaller image
distance with larger inverse value lower the slope, hence, smaller y-intercept
and larger focal length.
When half of the lens was covered, the image became dimmer since the light passed through the lens was decreased by a factor of 2 due to halved-lens. Besides, as the object distance became closer to the lens, the image size and distance became larger. At 0.5f, there was no image because the image was between the vertex and the focus; hence, the image became virtual.
When half of the lens was covered, the image became dimmer since the light passed through the lens was decreased by a factor of 2 due to halved-lens. Besides, as the object distance became closer to the lens, the image size and distance became larger. At 0.5f, there was no image because the image was between the vertex and the focus; hence, the image became virtual.
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