DP IB Physics: HL

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First teaching 2014

Last exams 2024

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9.3.2 Two-Slit Interference Patterns

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Two-Slit Interference Patterns

  • For two-source interference fringes to be observed, the sources of the wave must be:
    • Coherent (constant phase difference)
    • Monochromatic (single wavelength)

  • When two waves interfere, the resultant wave depends on the phase difference between the two waves
    • This is proportional to the phase difference between the waves which can be written in terms of the wavelength λ of the wave

  • As seen from the diagram, the wave from slit S2 has to travel slightly further than that from S1 to reach the same point on the screen
    • The difference in this distance is the path difference

Path difference equations, downloadable AS & A Level Physics revision notes

Interference is caused by the variation in path length between the two slits

 

  • For constructive interference (where there are bright fringes or maxima), the difference in wavelengths will be an integer number of whole wavelengths
  • The condition for constructive interference can be written as:

path difference = n lambda (where n = 0, 1, 2, 3 ...)

  • When waves undergo constructive interference their amplitudes add to form a bigger resultant combined wave at the point where they meet

  • For destructive interference (where there are dark fringes or minima) it will be an integer number of whole wavelengths plus a half wavelength
  • The condition for destructive interference can be written as:

path difference = open parentheses n plus 1 half close parentheses lambda (where n = 0, 1, 2, 3 ...)

  • n is the order of the maxima (bright fringes) / minima (dark fringes)
    • n = 0 is taken from the middle, n = 1 is the next peak and so on
  • When waves undergo destructive interference their amplitudes add to form a smaller resultant combined wave at the point where they meet

Max and min interference pattern, downloadable AS & A Level Physics revision notes

Interference pattern of light waves shown with orders of maxima and minima

  • An interference pattern shows the intensity of light at different distances away from the central maxima
    • For a double-slit interference pattern the intensity of the light is the same for all maxima
  • This is different to the double-slit diffraction pattern that is observed on a screen (These are explained in 9.3.3 Diffraction Grating Patterns)

Double-Slit Diffraction Geometry

  • The diffraction pattern made by waves passing through two slits of separation d can be observed on a screen placed a large distance, D, away

9-3-2-double-slit-geometry

  • If the distance, D, between the slits and the screen, is considerably larger than the slit separation, D greater than greater than d:
    • This means the light rays coming from the slits can be considered as a set of plane wavefronts that are parallel to each other

physics-hl-rn-april-2022

  • For two paths, r1 and r2, travelling parallel to each other at an angle, θ, between the normal and the slit, the path difference will be:

path difference = r2 − r1d space sin space theta

  • For constructive interference:

path difference = n lambda

  • Therefore, bright fringes will occur when:

n lambda equals d sin space theta

  • For destructive interference:

path difference = open parentheses n plus 1 half close parentheses lambda

  • Therefore, dark fringes will occur when:

open parentheses n plus 1 half close parentheses lambda equals d sin space theta

9-3-2-double-slit-geometry-2

  • The distance between fringes, s, can be related to the distance to the screen, D, using trigonometry:

tan space theta equals s over D

  • Since the angle θ is small, the small-angle approximation may be used: tan space theta almost equal to sin space theta almost equal to theta

theta equals s over D

  • Using the condition for constructive interference and the small-angle approximation:

n lambda equals d sin space theta

n lambda equals d theta

  • Rearrange the equation for θ:

theta equals fraction numerator n lambda over denominator d end fraction

  • Combining the two equations gives:

fraction numerator n lambda over denominator d end fraction equals s over D

  • Rearranging for s gives an equation for the distance between two maxima:

s equals fraction numerator n lambda D over denominator d end fraction

Exam Tip

The equations for constructive and destructive interference above are the same versions as found in your data booklet - don't let other versions of these equations confuse you!

Constructive and destructive interference can be calculated with alternative equations for specific values of n

Intensity Graphs

  • In single slit diffraction, the observed interference pattern shows:
    • A central maximum with the highest intensity
    • Subsequent maxima with half the width of the central maximum
    • The intensity of each subsequent maxima decreases
  • In double slit diffraction, the observed interference pattern shows: 
    • The fringes are equally bright, meaning they have equal intensity
    • The angle increases by a constant amount, as the fringes are equally separated
  • Note: this is only the case for double slit diffraction for slit widths of negligible size

9-3-2-interference-intensity-graphs

Intensity graphs for single and double slit interference when the slit is infinitely narrow compared to a slit of finite width

  • The fringes due to the double slits are much closer together than in the single slit case
    • This is because the distance between the slits is greater than their widths

  • The resulting interference pattern is a combination of the double-slit and single slit interference patterns 
    • This is known as modulation

 

9-3-2-double-slit-diffraction

A modulated double-slit interference pattern with the single slit diffraction pattern is still visible in the "envelope" (shown by the dotted line). This occurs when the slit width is significant. 

  • The intensity of the resulting fringe pattern has been modulated by the interference of the two diffracted beams, as the effect of the single slits is significant
  • This is assuming that:
    • The slit width is not negligible
    • The distance between the slits is much greater than their width 

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Lindsay Gilmour

Author: Lindsay Gilmour

Lindsay graduated with First Class Honours from the University of Greenwich and earned her Science Communication MSc at Imperial College London. Now with many years’ experience as a Head of Physics and Examiner for A Level and IGCSE Physics (and Biology!), her love of communicating, educating and Physics has brought her to Save My Exams where she hopes to help as many students as possible on their next steps.