• Diffraction is the bending or spreading of waves when they encounter an obstacle or pass through an aperture

    • It is observed in various wave phenomena, such as light, sound, and water waves
  • Today, we will discuss “Diffraction Patterns Due to a ‘Single-Slit’ and a ‘Circular Aperture'”

  • Single-slit diffraction:

    • When light passes through a narrow slit, it diffracts and creates a pattern of bright and dark bands on a screen
    • The central bright band is the widest, and each subsequent band is narrower and less intense
    • The pattern is characterized by the central maximum and secondary maxima and minima
  • Single-slit diffraction equation:

    • For a single-slit of width ‘a’, the angle at which the first minimum is formed is given by:
    • sinθ = λ / a
      • θ: angle between the line perpendicular to the slit and the first minimum
      • λ: wavelength of light used
      • a: width of the slit
  • Circular aperture diffraction:

    • When light passes through a circular aperture, it produces a diffraction pattern with concentric bright and dark rings
    • The central bright spot is called the Airy disk, and subsequent rings are less intense
    • The pattern is characterized by the central maximum and rings of decreasing intensity
  • Circular aperture diffraction equation:

    • The angle at which the first minimum is formed can be determined using the equation:
    • sinθ = 1.22 * λ / D
      • θ: angle between the line perpendicular to the aperture and the first minimum
      • λ: wavelength of light used
      • D: diameter of the aperture
  • Intensity function in double-slit experiment (with slit of finite width):

    • In the double-slit experiment, when the slits have a finite width, the intensity at a point in the interference pattern depends on the superposition of waves diffracted from each slit
    • The intensity at a point on the screen can be calculated using the intensity function:
    • I = I₁ + I₂ + 2√(I₁ * I₂) * cos(δ)
      • I₁ and I₂: intensities of light from each slit individually
      • δ: phase difference between the waves from each slit
  • Diffraction patterns can be seen in various natural phenomena and applications:

    • Rainbows, where sunlight undergoes diffraction and dispersion
    • Sunsets, where the Sun’s light is scattered and diffracted as it passes through the Earth’s atmosphere
    • CD or DVD discs, where diffraction patterns are encoded to store information
    • Microscopic imaging techniques, such as diffraction-limited microscopy, utilize diffraction patterns to enhance resolution
  • Examples of diffraction patterns:

    • The diffraction grating, consisting of parallel slits, produces a pattern of multiple order maxima and minima
    • X-ray crystallography uses the diffraction pattern generated by x-rays passing through a crystal to determine its atomic structure
    • Ultrasonic waves diffracting around obstacles or through narrow openings produce characteristic diffraction patterns
  • Applications of diffraction in everyday life:

    • The principle of diffraction is applied in the design of audio speakers, which use diffraction to disperse sound waves evenly
    • Diffraction gratings are used in spectrophotometers and monochromators for precise wavelength selection and analysis of light
    • Holography relies on the interference and diffraction of light to create three-dimensional images
  • In conclusion:

    • Diffraction is an important wave phenomenon observed in various fields, including optics, acoustics, and water waves
    • Single-slit diffraction and circular aperture diffraction produce characteristic patterns of bright and dark regions
    • The intensity at a point in a double-slit experiment with finite slit width is determined by the interference and diffraction of waves
    • Diffraction patterns have practical applications in technology and are widely observed in nature Sure! Here are slides 11 to 20:

Slide 11:

  • Diffraction Patterns Due to a ‘Single-Slit’ and a ‘Circular Aperture - Intensity function in double-slit experiment (with slit of finite width)’
  • In a double-slit experiment, when the slits have a finite width, the intensity at a point in the interference pattern depends on the superposition of waves diffracted from each slit
  • The intensity at a point on the screen can be calculated using the intensity function:
    • I = I₁ + I₂ + 2√(I₁ * I₂) * cos(δ)
    • Here, I₁ and I₂ are the intensities of light from each slit individually, and δ is the phase difference between the waves from each slit

Slide 12:

  • Diffraction Patterns Due to a ‘Single-Slit’ and a ‘Circular Aperture - Intensity function in double-slit experiment (with slit of finite width)'
  • The intensity function equation shows that the interference pattern is modified by the diffraction of light at the slits
  • The term 2√(I₁ * I₂) * cos(δ) represents the interference fringes resulting from the superposition of waves

Slide 13:

  • Diffraction Patterns Due to a ‘Single-Slit’ and a ‘Circular Aperture - Intensity function in double-slit experiment (with slit of finite width)'
  • When the phase difference δ is zero or a multiple of 2π, the waves from each slit are in phase, resulting in constructive interference and a bright fringe
  • When the phase difference δ is an odd multiple of π, the waves from each slit are out of phase, resulting in destructive interference and a dark fringe

Slide 14:

  • Examples of diffraction and interference patterns:
    • Interference fringes in soap bubbles, where light is reflected and undergoes constructive and destructive interference
    • Interference patterns in thin films, such as oil slicks, where light reflects at different layers and interferes
    • Interference patterns in Newton’s rings, where light is reflected between a glass and a lens, creating concentric bright and dark rings

Slide 15:

  • Examples of diffraction and interference patterns:
    • The phenomenon of moiré patterns, where two similar patterns overlap and create a new, distinct pattern
    • The rings observed when laser light is scattered by small particles, known as Mie scattering, which result from the interference and diffraction of light waves

Slide 16:

  • Applications of diffraction in technology:
    • CD or DVD discs use diffraction patterns encoded onto the surface to store and read data
    • Diffraction gratings are used in spectrophotometers to separate light into its different component wavelengths for analysis

Slide 17:

  • Applications of diffraction in technology:
    • X-ray crystallography uses the diffraction pattern generated by x-rays passing through a crystal to determine its atomic structure
    • Diffraction patterns are used in various microscopy techniques, such as electron microscopy and X-ray microscopy, to enhance resolution and visualize small-scale structures

Slide 18:

  • Applications of diffraction in nature:
    • Rainbows are formed when sunlight refracts, reflects, and undergoes diffraction and dispersion in water droplets
    • Sunsets exhibit diffraction and scattering of sunlight as it passes through the Earth’s atmosphere, resulting in vibrant and colorful skies

Slide 19:

  • Applications of diffraction in nature:
    • The diffraction of sound waves around obstacles or through narrow openings can create acoustic shadows or diffraction patterns, which are utilized in noise reduction and sound engineering techniques
    • Diffraction of water waves around piers, breakwaters, and islands can result in wave patterns and interference effects

Slide 20:

  • Summary of key points:
    • The intensity in a double-slit experiment with finite slit width can be calculated using the intensity function
    • The intensity function incorporates both interference and diffraction effects
    • Diffraction and interference patterns are observed in various natural phenomena, such as rainbows and sunsets, as well as in technological applications like CD and DVD discs, spectrophotometers, and microscopy techniques

Slide 21:

  • Diffraction Patterns Due to a ‘Single-Slit’ and a ‘Circular Aperture - Summary'
  • Diffraction is the bending or spreading of waves when they encounter an obstacle or pass through an aperture
  • Single-slit diffraction produces a pattern of bright and dark bands, with the central maximum being the widest and subsequent bands narrowing
  • Circular aperture diffraction creates concentric bright and dark rings, with the central spot known as the Airy disk

Slide 22:

  • Diffraction Patterns Due to a ‘Single-Slit’ - Factors affecting the pattern:
    • Wavelength of light: Shorter wavelengths produce narrower diffraction patterns
    • Slit width: Narrower slits create wider diffraction patterns
    • Distance from the screen: Closer distances result in wider patterns

Slide 23:

  • Diffraction Patterns Due to a ‘Single-Slit’ - Example:
    • A single slit with a width of 0.1 mm is illuminated by monochromatic light with a wavelength of 600 nm
    • Calculate the angle at which the first minimum will occur in the diffraction pattern
    • Using the single-slit diffraction equation: sinθ = λ / a
    • sinθ = (600 x 10^-9 m) / (0.1 x 10^-3 m) = 0.006

Slide 24:

  • Diffraction Patterns Due to a ‘Single-Slit’ - Example continued:
    • Find the angle using inverse sine function: θ = sin^(-1)(0.006)
    • θ ≈ 0.345 degrees
    • This angle represents the position of the first minimum in the diffraction pattern

Slide 25:

  • Circular Aperture Diffraction - Factors affecting the pattern:
    • Wavelength of light: Shorter wavelengths produce narrower rings
    • Diameter of the aperture: Larger apertures create wider rings
    • Distance from the screen: Closer distances result in wider rings

Slide 26:

  • Circular Aperture Diffraction - Example:
    • Light with a wavelength of 500 nm passes through a circular aperture with a diameter of 1 mm
    • Calculate the angle at which the first minimum will occur
    • Using the circular aperture diffraction equation: sinθ = 1.22 * λ / D
    • sinθ = 1.22 * (500 x 10^-9 m) / (1 x 10^-3 m) = 0.61

Slide 27:

  • Circular Aperture Diffraction - Example continued:
    • Find the angle using inverse sine function: θ = sin^(-1)(0.61)
    • θ ≈ 37.4 degrees
    • This angle represents the position of the first minimum in the diffraction pattern

Slide 28:

  • Diffraction Patterns - Interference and Diffraction:
    • Diffraction involves the bending/spreading of waves when they encounter an obstacle or pass through an aperture
    • Interference occurs when waves superpose on each other, resulting in constructive or destructive interference
    • In the double-slit experiment, interference and diffraction contribute to the observed patterns

Slide 29:

  • Diffraction Patterns - Applications:
    • Audio speakers use diffraction to disperse sound waves evenly, enhancing sound quality
    • Spectrophotometers utilize diffraction gratings to separate and analyze different wavelengths of light
    • X-ray crystallography relies on diffraction patterns to determine the atomic structure of crystals

Slide 30:

  • Diffraction Patterns - Applications continued:
    • Holography utilizes interference and diffraction to create three-dimensional images
    • Various microscopy techniques, such as electron microscopy and X-ray microscopy, use diffraction patterns to achieve high-resolution imaging