Understanding Diffraction and Interference Patterns: Single, Double and Multiple Slits, Lab Reports of Physics

Detailed information on the concepts of diffraction and interference, focusing on single, double and multiple slits. It includes equations for calculating slit width, slit spacing, and ruling density, as well as instructions for observing and measuring diffraction patterns. The document also explains babinet's principle.

Typology: Lab Reports

Pre 2010

Uploaded on 07/28/2009

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DIFFRACTION AND INTERFERENCE
OBJECTIVES:
1) Observe Fraunhofer diffraction and interference from a single slit, double-slit and
multiple-slit (a diffraction grating).
2) Calculate the slit width, which produces the single-slit diffraction pattern, and observe
how the slit width affects the diffraction pattern.
3) Calculate the slit width and the slit spacing for double-slit, and compare the pattern to
that given by a single-slit.
4) Calculate the slit spacing of a diffraction grating and thereby determine the ruling
density.
5) Verify Babinet's Principle by observing the diffraction pattern from a thin wire.
CAUTION!
The laser is a device that can produce an intense, narrow beam of light at
one wavelength. NEVER look directly into the laser beam or its
reflection from a mirror, etc.
INTRODUCTION
Diffraction occurs when a portion of a wave passes through a slit. Interference occurs when two or
more coherent waves overlap. (Coherent means that the waves have a fixed phase relationship.)
Constructive interference takes place at certain locations where two waves are in phase (both
waves have maximum). Destructive interference takes place where two waves are out of phase
(one wave has maximum, the other has minimum).
In the case of a single-slit, diffraction is the only effect present. In the case of two or more slits, two
effects are present: a) diffraction from each individual slit; b) if the incident light is coherent and the
diffraction patterns of each slit overlap, then interference takes place in the region of the overlap,
(i.e., inside the diffraction envelope).
The simplest diffraction and interference patterns involve plane waves (collimated light beams).
Diffraction patterns associated with plane waves are called Fraunhofer patterns, named after the
German scientist who first explained the effect. In this experiment, we will use a laser as our light
source. A laser produces collimated and coherent light beams at one wavelength.
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DIFFRACTION AND INTERFERENCE

OBJECTIVES:

  1. Observe Fraunhofer diffraction and interference from a single slit, double-slit and multiple-slit (a diffraction grating).
  2. Calculate the slit width, which produces the single-slit diffraction pattern, and observe how the slit width affects the diffraction pattern.
  3. Calculate the slit width and the slit spacing for double-slit, and compare the pattern to that given by a single-slit.
  4. Calculate the slit spacing of a diffraction grating and thereby determine the ruling density.
  5. Verify Babinet's Principle by observing the diffraction pattern from a thin wire.

CAUTION!

The laser is a device that can produce an intense, narrow beam of light at

one wavelength. NEVER look directly into the laser beam or its

reflection from a mirror, etc.

INTRODUCTION

Diffraction occurs when a portion of a wave passes through a slit. Interference occurs when two or more coherent waves overlap. (Coherent means that the waves have a fixed phase relationship.) Constructive interference takes place at certain locations where two waves are in phase (both waves have maximum). Destructive interference takes place where two waves are out of phase (one wave has maximum, the other has minimum).

In the case of a single-slit, diffraction is the only effect present. In the case of two or more slits, two effects are present: a) diffraction from each individual slit; b) if the incident light is coherent and the diffraction patterns of each slit overlap, then interference takes place in the region of the overlap, (i.e., inside the diffraction envelope).

The simplest diffraction and interference patterns involve plane waves (collimated light beams). Diffraction patterns associated with plane waves are called Fraunhofer patterns, named after the German scientist who first explained the effect. In this experiment, we will use a laser as our light source. A laser produces collimated and coherent light beams at one wavelength.

Introductory Physics Experiments (Physics 252, v3.7)

Single-slit diffraction

D

w

θ^ n = 2

X

X- 1 n = + 1 n = + 2

X

  • 2

X = 0

Geometry and intensity distribution in single-slit diffraction Figure 1

Figure 1 shows the pattern of light intensity as a function of position, with x = 0 at the position the beam would have taken without the slit. The top pane of the drawing shows the physical arrangement, with a sketch indicating the intensity at different points. The bottom part of the figure is a blowup of the intensity sketch.

The intensity curve shows how much light appears as a function of position; the original beam of light is redistributed by diffraction. Maxima (peaks) of light intensity will be seen as bright spots if you look at the screen. Minima (valleys) of light intensity will be seen as dark spots. The principal maximum position, x=0, is the center of the central bright spot, which is where you might have thought all the light would go. To measure the location of a maximum, use the center of a bright spot. To measure the location of the minimum, use the center of a dark spot.

The pattern in figure 1 is what happens for light of a single wavelength. Superimposing diffraction patterns from different wavelengths of light would blur the pattern, because maxima for some wavelengths would land on minima for other wavelengths. This is one reason we use a laser in this experiment.

Introductory Physics Experiments (Physics 252, v3.7)

Double-slit diffraction and interference

D

d θ

X

maximum) minimum)

n = -2 m = -7 m = -4 n = + Figure 2: Geometry and intensity distribution in double-slit diffraction and interference. Arrows point to m = -7 interference maximum, and n = +1 diffraction minimum. The m = -5 maximum is not seen here as it coincides with the n = -1 minimum.

For two nearby slits (the double slit), the condition for interference maximum to occur is:

d sin θm = mλ Thus,

Here, d = slit spacing m = order number of interference maximum λ = wavelength of light D = distance from screen to slit xm =distance from the principal maximum to the m th interference maximum

sin tan^1  

D

x

m d m

λ

Diffraction and Interference (Version 3.7, 8/23/2002)

θm = angle from the center line to the m th interference maximum

Equation (2) is called the Interference Equation. The algebra looks the same as for the Diffraction equation except that xm refers to the location of maxima, not minima and d is the spacing between the two slits , not the width of the individual slits.

Multiple-slit interference and diffraction (a diffraction grating)

D

d θ n = 3

X

X^3

Intensity distribution of a diffraction grating Figure 3

The condition here for interference maximum is the same as for double-slits, but the pattern may be very different because d (the slit spacing) for gratings is very small. d sin θn = nλ

Thus d^ =^

sin tan−^1

xn D

Diffraction and Interference (Version 3.7, 8/23/2002)

Partners: ____________________ Name:______________________

____________________________ Section:_____________________

PROCEDURE

  1. Single-slit diffraction a) Place the panel that holds four single-slits in the laser (between the laser and the screen). The pattern is most easily seen with the slit near the laser and the screen far away (even perhaps on the wall). Try different slits and observe their diffraction patterns on the screen.

Q: How does the slit width affect the diffraction pattern?

b) Choose a slit that gives a diffraction pattern of reasonable size. Measure the distance from the slit to the screen (D) and record the labeled slit width. c) Tape a piece of paper across the screen where you see the diffraction pattern. Mark carefully the positions of the center at the principal maximum and the center of the diffraction minima of several orders on the paper. Remove the paper from the screen and attach it to your lab report. d) Measure and record the distance of each minimum from the principal maximum (xn) in the table below. Calculate the slit width (w) using equation (1). Use negative xn and n for the positions to the left of the principal maximum.

D (distance from the slit to the screen) = __________________ cm Labeled slit width = _____________ mm

Write down the equation you will use for calculating the slit width (w):

Note: The wavelength (λ) of He-Ne laser is 632.8 nm = 6.328 x 10-4^ mm

Order of Diffraction Minimum n

distance from principal maximum xn (cm)

calculated slit width w (mm)

Average slit width:

Q: Compare the average slit width with the labeled one. Comment:

Introductory Physics Experiments (Physics 252, v3.7)

  1. Double-slit interference and diffraction a) Place the panel that holds four double-slits in the laser beam. Try different double-slits. Q: What is the main difference between the single-slit and double-slit pattern?

Q: What causes the main difference from the single-slit pattern?

Q: How does the slit width affect the pattern?

Q: How does slit spacing affect the pattern?

b) Choose a double-slit that gives a reasonable pattern. Measure the distance from the slit to the screen (D) and record the labeled slit width and slit spacing. c) Tape a piece of paper across the screen where you see the pattern. Mark carefully the positions of the principal maximum, the interference maxima, and the diffraction minima on the paper. (You may want to distinguish the marks for each kind.) Remove the paper from the screen and attach it to your lab report. d) Measure and record the distance of each interference maximum and each diffraction minimum from the principal maximum (xn) in the following two tables respectively. Calculate and the slit width (w) using equation (1) and the slit spacing (d) using equation (2).

D (distance from slit to screen) = __________________ cm Labeled slit width = _____________ mm Labeled slit spacing = _____________ mm

e) Write down the equation you will use for calculating slit width (w):

order of diffraction minimum n

distance from principal maximum xn (cm)

calculated slit width w (mm)

Average slit width:

Q: Compare the average slit width with the labeled one. Comment:

f) Write down the equation you will use for calculating slit spacing (d):

Introductory Physics Experiments (Physics 252, v3.7)

order of minimum n

distance from principal maximum xn (cm)

calculated diameter w (mm) 1 2 3 4 5 Average wire diameter:

Q: Compare the average wire diameter with the labeled one. Comment:

Q: Is your hair thicker or thinner than the wire? How did you find out?

  1. Multiple-slit interference and diffraction: a diffraction grating a) Place the grating in the laser beam (close to the screen, not far away). b) Measure the distance from the plane of the grating to the screen (D) and record the labeled ruling density (grooves/mm). c) Tape a piece of paper across the screen. Mark carefully the positions of the principal maximum and the diffraction maxima. Remove the paper from the screen and attach it to your lab report. d) Measure and record the distance of each diffraction maximum from the principal maximum (xn). Calculate the slit spacing (d) using equation (2).

D (distance from the grating to the screen) = __________________ cm Labeled ruling density = _____________ grooves/mm

order of maximum n

distance from principal maximum xn (cm)

calculated slit spacing d (mm)

  • 1
  • 2
  • Average slit spacing:

e) Measured ruling density = 1 d

= _____________ grooves/mm

Compare the measured ruling density with the labeled one. Comment: