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Analysis of Intensity of CD
         Diffraction Pattern using
Fraunhofer Single Slit Diffraction
Karl Arwen Cereno1, Leomark Responde1, Mark Joshua Salvacion2 and Jan
                                        Carlo Frayre3
                   1 Institute   of Civil Engineering, College of Engineering
              2 Department       of Geodetic Engineering, College of Engineering
             3Department    of Curriculum and Instruction, College of Education
            University of the Philippines, Diliman, Quezon City 1101 Philippines
Abstract
     In this experiment, the consistency of the
formula for intensity will be analyzed. The
method to be used includes calculating the
angle of diffraction given that there is a prior
value for a given intensity. The intensity is then
plotted and the graph is compared to the
theoretical plot of the Fraunhofer Single Slit
Diffraction. The result shows that the data
follows the theory. Because of the
approximation method used in calculating for a
given intensity, errors and deviations will be
accounted accordingly.
Introduction
     The wave nature of light can be demonstrated
clearly by observing the interference and diffraction of
light as it passes through slits. Diffraction manifests
itself in the apparent bending of waves around small
obstacles and the spreading out of waves past small
openings. (Include fraunhofer equation, and graph)
     For single-slit diffraction, the slit width can be
measured using the measurements of the diffraction
pattern. If a monochromatic light approaching the
diffracting object is parallel and the image plane is at a
distance large enough compared to the diffracting
object, the situation is of the Fraunhofer Diffraction. The
intensity of the mth fringe can then be calculated.
METHODOLOGY
Materials:

1. Laser Source

2. Blank CD

3. Light sensor

4. Vernier LabProTM

5. Optical Bench

6. Meter stick
METHODOLOGY

 This experiment was conducted to verify the
  functionality of the Franhoufer diffraction
  equation that relates the intensity of light on the
  mth order bright band and its angular distance
  from the central bright band.


 Figure 1 shows the experimental set up
METHODOLOGY




    Figure 1
METHODOLOGY

 The angle of incidence of the incoming light is roughly
  normal to the CD.

 The plane of the screen is set parallel to the plane of the
  CD.

 The intensity of the bright bands on the diffraction
  pattern was measured using a light sensor.

 Measurements are recorded in Data Table 1.
RESULTS
 Data Table 1
                          y
 m
                        (cm)

 -2           -           -             -             -

 -1          345        30.8           26.42

 0           1361   (Gauge the ‘D’ value. Does it fit the Fraunhofer
                    equation????)
 1           273        30.8           26.42

 2            -           -              -            -


D = 62 cm              a = 1.67 μm
λ = 650 nm             Io = 1361 lux
RESULTS

 There is a significant difference between the
  measured Intensity on the m=1 band and the m=-1
  band.



 The 2nd order bright bands are observable but the
  intensities are not measurable using the light
  sensor.
CONCLUSION

 The behavior of the plotted graph follows the theoretical
  behavior of the I/Io vs β (figure 3).



 The function that will best fit the data points cannot be
  derived due to the limits of the graphing tool (Microsoft
  Excel).
Conclusion

(Use the measurements
to generate a plot
following the Fraunhofer
equation)




               Figure 3 Intensity of the Single slit
               Fraunhofer diffraction pattern
RESULTS
 Graph of the ratio of the mth intensity/maximum
  intensity versus β/2 (phase difference)

                                    1.2
                                                         (Superimpose the
                                      1
                                                          Experimental and
                                    0.8                   Theoretical graphs)
                                    0.6
     I/Io
                                    0.4


                                    0.2


                                      0
            -2   -1.5   -1   -0.5          0    0.5   1      1.5   2   (Factor: π)
                                    -0.2
                                           mπ
                                Figure 2
CONCLUSION
The values of the measured intensity was highly
  affected by the following errors.

 Instrument error

 Procedural error

 Human error
Acknowledgements

     The researchers would like to express utmost
gratitude to the National Institute of Physics of the
University of the Philippines – Diliman for the academic
support and the privilege that they have
given, especially on the use of the laboratory and the
Lab Manuals that were provided. And ultimately, the
researchers would like express gratitude to Professor
Gerold Pidemonte for his support, encouragement and
assistance in this experiment.
(Change ‘Pidemonte’ to ‘P-E-demonte’ and Add Romy
Abaniel)
References
1. Lab Manual Authors, Physics 72.1 Laboratory Manual, 2007

2. Young, H., Freedman, R., “Sears and Zemansky’s University
   Physics: with Modern Physics” 12th ed, Chapter 36, Pearson
   Addison-Wesley, 1301 Sansome St., San Francisco, CA
   94111, 2008

3. Nave,C.R., “HyperPhysics”, hyperphysics.phy-astr.gsu.edu, 2010

4. Department of Physics and Astronomy, “Fraunhofer Diffraction
   with a Laser Source”, The University of
   Sheffield, Sheffield.ac.uk, 2008

5. Tippie, A., Lee, T., “Experiment with Diffraction”, 2008

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73.1 s

  • 1. Analysis of Intensity of CD Diffraction Pattern using Fraunhofer Single Slit Diffraction Karl Arwen Cereno1, Leomark Responde1, Mark Joshua Salvacion2 and Jan Carlo Frayre3 1 Institute of Civil Engineering, College of Engineering 2 Department of Geodetic Engineering, College of Engineering 3Department of Curriculum and Instruction, College of Education University of the Philippines, Diliman, Quezon City 1101 Philippines
  • 2. Abstract In this experiment, the consistency of the formula for intensity will be analyzed. The method to be used includes calculating the angle of diffraction given that there is a prior value for a given intensity. The intensity is then plotted and the graph is compared to the theoretical plot of the Fraunhofer Single Slit Diffraction. The result shows that the data follows the theory. Because of the approximation method used in calculating for a given intensity, errors and deviations will be accounted accordingly.
  • 3. Introduction The wave nature of light can be demonstrated clearly by observing the interference and diffraction of light as it passes through slits. Diffraction manifests itself in the apparent bending of waves around small obstacles and the spreading out of waves past small openings. (Include fraunhofer equation, and graph) For single-slit diffraction, the slit width can be measured using the measurements of the diffraction pattern. If a monochromatic light approaching the diffracting object is parallel and the image plane is at a distance large enough compared to the diffracting object, the situation is of the Fraunhofer Diffraction. The intensity of the mth fringe can then be calculated.
  • 4. METHODOLOGY Materials: 1. Laser Source 2. Blank CD 3. Light sensor 4. Vernier LabProTM 5. Optical Bench 6. Meter stick
  • 5. METHODOLOGY  This experiment was conducted to verify the functionality of the Franhoufer diffraction equation that relates the intensity of light on the mth order bright band and its angular distance from the central bright band.  Figure 1 shows the experimental set up
  • 6. METHODOLOGY Figure 1
  • 7. METHODOLOGY  The angle of incidence of the incoming light is roughly normal to the CD.  The plane of the screen is set parallel to the plane of the CD.  The intensity of the bright bands on the diffraction pattern was measured using a light sensor.  Measurements are recorded in Data Table 1.
  • 8. RESULTS Data Table 1 y m (cm) -2 - - - - -1 345 30.8 26.42 0 1361 (Gauge the ‘D’ value. Does it fit the Fraunhofer equation????) 1 273 30.8 26.42 2 - - - - D = 62 cm a = 1.67 μm λ = 650 nm Io = 1361 lux
  • 9. RESULTS  There is a significant difference between the measured Intensity on the m=1 band and the m=-1 band.  The 2nd order bright bands are observable but the intensities are not measurable using the light sensor.
  • 10. CONCLUSION  The behavior of the plotted graph follows the theoretical behavior of the I/Io vs β (figure 3).  The function that will best fit the data points cannot be derived due to the limits of the graphing tool (Microsoft Excel).
  • 11. Conclusion (Use the measurements to generate a plot following the Fraunhofer equation) Figure 3 Intensity of the Single slit Fraunhofer diffraction pattern
  • 12. RESULTS  Graph of the ratio of the mth intensity/maximum intensity versus β/2 (phase difference) 1.2  (Superimpose the 1 Experimental and 0.8 Theoretical graphs) 0.6 I/Io 0.4 0.2 0 -2 -1.5 -1 -0.5 0 0.5 1 1.5 2 (Factor: π) -0.2 mπ Figure 2
  • 13. CONCLUSION The values of the measured intensity was highly affected by the following errors.  Instrument error  Procedural error  Human error
  • 14. Acknowledgements The researchers would like to express utmost gratitude to the National Institute of Physics of the University of the Philippines – Diliman for the academic support and the privilege that they have given, especially on the use of the laboratory and the Lab Manuals that were provided. And ultimately, the researchers would like express gratitude to Professor Gerold Pidemonte for his support, encouragement and assistance in this experiment. (Change ‘Pidemonte’ to ‘P-E-demonte’ and Add Romy Abaniel)
  • 15. References 1. Lab Manual Authors, Physics 72.1 Laboratory Manual, 2007 2. Young, H., Freedman, R., “Sears and Zemansky’s University Physics: with Modern Physics” 12th ed, Chapter 36, Pearson Addison-Wesley, 1301 Sansome St., San Francisco, CA 94111, 2008 3. Nave,C.R., “HyperPhysics”, hyperphysics.phy-astr.gsu.edu, 2010 4. Department of Physics and Astronomy, “Fraunhofer Diffraction with a Laser Source”, The University of Sheffield, Sheffield.ac.uk, 2008 5. Tippie, A., Lee, T., “Experiment with Diffraction”, 2008