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Optics
Presented to: Dr. Kamran sb.
Presented by: Tahir Younus
Reg. No. BS-PHYS-18-44 (E)
Semester: 2018-22 5th
Department of Physics
Ghazi University Dera Ghazi
Khan
β€’Introduction
β€’Performed by Young in 1801 to demonstrate wave behavior of light.
β€’In this experiment, Young identified the phenomenon called interference
β€’The double-slit experiment is a demonstration that light and matter can display
characteristics of both waves and particles.
Interference occurred during experiment is of two types
οƒ˜ Constructive Interference
οƒ˜ Destructive Interference
Experiment
 A screen having two narrow
slits is illuminated by
monochromatic light.
 Superposition of wavelets
result in series of bright and
dark fringes.
 The bright fringes are termed
as maxima and dark fringes
are termed as minima.
Derivation of
Equation for
Maxima and
Minima
Maxima
If the point P is to have a bright fringe, the path difference must be an integral multiple of πœ†.
BD = mπœ†
m = 0,1,2,3,4,….
From βˆ†π΄π΅π·.
BD = d sinπœƒ
So, d sinπœƒ= mπœ† … . . 1)
Distance between Adjacent Bright Fringes
Since angle β€˜πœƒβ€™ is very small,
Sin πœƒ β‰ˆ π‘‡π‘Žπ‘›πœƒ
So, Equation 1 becomes
dπ‘‡π‘Žπ‘›πœƒ=m πœ† … . . 2)
From figure
Tanπœƒ=
π‘Œ
𝐿
So, equation 2 can be written as
d
π‘Œ
𝐿
= m πœ†
Y=m
πœ†πΏ
𝑑
… . . 3)
If there would be a dark fringe at point P then,
Y=(π‘š +
1
2
)
πœ†πΏ
𝑑
…. 4)
That’s the distance between two adjacent bright fringes, mth and (m+1) fringes are considered.
For mth bright fringe
π‘¦π‘š = π‘š
πœ†πΏ
𝑑
For (m+1) bright fringe,
π‘¦π‘š+1 = (π‘š + 1)
πœ†πΏ
𝑑
Let β€˜βˆ†π‘Œβ€²
be the distance between these two adjacent fringes, then
βˆ†Y=π‘Œπ‘š+1 βˆ’ π‘Œπ‘š= π‘š +
1
2
πœ†πΏ
𝑑
βˆ’ π‘š
πœ†πΏ
𝑑
βˆ†Y=
πœ†πΏ
𝑑
Minima (Dark fringes)
If the point P is to have a dark fringe, the path difference BD must be half integral number of wavelength
πœ†.
𝐡𝐷 = (π‘š +
1
2
)πœ† m=0,1,2,….
From βˆ†π΄π΅π·.
BD = d sinπœƒ
d sinπœƒ = (π‘š +
1
2
)πœ†
First dark fringe is obtained at m=0 and second dark for m=1.
Distance between adjacent dark fringes
Since angle β€˜πœƒβ€™ is very small,
Sin πœƒ β‰ˆ π‘‡π‘Žπ‘›πœƒ
dπ‘‡π‘Žπ‘›πœƒ = (π‘š +
1
2
)πœ†
From figure,
Tanπœƒ=
π‘Œ
𝐿
d
π‘Œ
𝐿
= (π‘š +
1
2
)πœ†
If there would be a dark fringe at β€˜p’ then
Y=(π‘š +
1
2
)
πœ†πΏ
𝑑
Now distance between to adjacent dark fringes,
βˆ†Y=
πœ†πΏ
𝑑
Dark and bright fringes are of equal width and are equally spaced.
Fringe spacing is directly proportional to β€˜πœ†β€™ and distance between slits β€˜L’.
Inversely to separation of slits β€˜d’.

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Youngs double slit experiment

  • 1. Optics Presented to: Dr. Kamran sb. Presented by: Tahir Younus Reg. No. BS-PHYS-18-44 (E) Semester: 2018-22 5th Department of Physics Ghazi University Dera Ghazi Khan
  • 2. β€’Introduction β€’Performed by Young in 1801 to demonstrate wave behavior of light. β€’In this experiment, Young identified the phenomenon called interference β€’The double-slit experiment is a demonstration that light and matter can display characteristics of both waves and particles.
  • 3. Interference occurred during experiment is of two types οƒ˜ Constructive Interference οƒ˜ Destructive Interference
  • 4. Experiment  A screen having two narrow slits is illuminated by monochromatic light.  Superposition of wavelets result in series of bright and dark fringes.  The bright fringes are termed as maxima and dark fringes are termed as minima.
  • 5.
  • 7. Maxima If the point P is to have a bright fringe, the path difference must be an integral multiple of πœ†. BD = mπœ† m = 0,1,2,3,4,…. From βˆ†π΄π΅π·. BD = d sinπœƒ So, d sinπœƒ= mπœ† … . . 1)
  • 8. Distance between Adjacent Bright Fringes Since angle β€˜πœƒβ€™ is very small, Sin πœƒ β‰ˆ π‘‡π‘Žπ‘›πœƒ So, Equation 1 becomes dπ‘‡π‘Žπ‘›πœƒ=m πœ† … . . 2) From figure Tanπœƒ= π‘Œ 𝐿 So, equation 2 can be written as d π‘Œ 𝐿 = m πœ† Y=m πœ†πΏ 𝑑 … . . 3)
  • 9. If there would be a dark fringe at point P then, Y=(π‘š + 1 2 ) πœ†πΏ 𝑑 …. 4) That’s the distance between two adjacent bright fringes, mth and (m+1) fringes are considered. For mth bright fringe π‘¦π‘š = π‘š πœ†πΏ 𝑑 For (m+1) bright fringe, π‘¦π‘š+1 = (π‘š + 1) πœ†πΏ 𝑑 Let β€˜βˆ†π‘Œβ€² be the distance between these two adjacent fringes, then βˆ†Y=π‘Œπ‘š+1 βˆ’ π‘Œπ‘š= π‘š + 1 2 πœ†πΏ 𝑑 βˆ’ π‘š πœ†πΏ 𝑑 βˆ†Y= πœ†πΏ 𝑑
  • 10. Minima (Dark fringes) If the point P is to have a dark fringe, the path difference BD must be half integral number of wavelength πœ†. 𝐡𝐷 = (π‘š + 1 2 )πœ† m=0,1,2,…. From βˆ†π΄π΅π·. BD = d sinπœƒ d sinπœƒ = (π‘š + 1 2 )πœ† First dark fringe is obtained at m=0 and second dark for m=1.
  • 11. Distance between adjacent dark fringes Since angle β€˜πœƒβ€™ is very small, Sin πœƒ β‰ˆ π‘‡π‘Žπ‘›πœƒ dπ‘‡π‘Žπ‘›πœƒ = (π‘š + 1 2 )πœ† From figure, Tanπœƒ= π‘Œ 𝐿 d π‘Œ 𝐿 = (π‘š + 1 2 )πœ† If there would be a dark fringe at β€˜p’ then Y=(π‘š + 1 2 ) πœ†πΏ 𝑑 Now distance between to adjacent dark fringes, βˆ†Y= πœ†πΏ 𝑑
  • 12. Dark and bright fringes are of equal width and are equally spaced. Fringe spacing is directly proportional to β€˜πœ†β€™ and distance between slits β€˜L’. Inversely to separation of slits β€˜d’.