SP Unit 2.5

Practicals

Waves properties

SP Unit 2.5

Practicals

Waves properties

Learners should be able to demonstrate and apply their knowledge and understanding of:

1. Determination of wavelength using Young’s Double Slits
2. Determination of wavelength using Diffraction Grating
3. Determination of the speed of sound using Stationary Waves
  • 1. Determination of Wavelength Using Young’s Double Slit Experiment

  • ⇒  Objective:
  • Measure the wavelength of a monochromatic light source by analyzing the interference pattern produced by two closely spaced slits.
  • ⇒  Apparatus:

  • – Coherent light source (e.g., laser)
  • – Double slit plate with known slit separation (d)
  • – White screen or photographic plate
  • – Ruler or measuring tape
  • – Optical bench
  • ⇒  Procedure:

  • 1. Setup:
  • – Mount the light source so that its beam is incident on the double-slit plate.
  • – Place the screen at a known distance (L) from the slits.
  • – Ensure the setup is stable and aligned so that the interference pattern is clear.
  • Figure 1 Young’s Double slit experiment
  • 2. Observation:
  • – When light passes through the two slits, it produces an interference pattern of bright and dark fringes on the screen.
  • – Measure the distance between several adjacent bright fringes (or dark fringes) to determine the fringe spacing ([math]\Delta x[/math]).
  • 3. Calculation:
  • – For small angles, the fringe separation is related to the wavelength (λ) by:
  • [math]\Delta x = \frac{\lambda L}{d}[/math]
  • – Rearranging to solve for λ:
  • [math]\lambda = \frac{\Delta x \cdot L}{d}[/math]
  • Using your measured values of Δx, d, and L, compute the wavelength.
  • ⇒  Points to Consider:

  • Ensure that the distance L is large compared to d for small-angle approximations to be valid.
  • Take multiple measurements of fringe spacing to improve accuracy.
  • 2. Determination of Wavelength Using a Diffraction Grating

  • ⇒  Objective:

  • Determine the wavelength of light using a diffraction grating which produces multiple diffraction orders.
  • Figure 2 Wavelength using a diffraction grating
  • ⇒  Apparatus:

  • – Monochromatic light source (e.g., laser or filtered lamp)
  • – Diffraction grating with a known number of lines per millimeter (or known grating spacing, d).
  • – Rotating stage or goniometer to measure diffraction angles
  • – Screen or detector
  • ⇒  Procedure:

  • 1. Setup:
  • – Shine the monochromatic light on the diffraction grating
  • – The grating diffracts the light into several orders (bright spots) on either side of the central maximum.
  • – Place a screen at a distance or use a goniometer to measure the angle θ for a given order m (typically m=1).
  • 2. Measurement:
  • – Measure the angle θ between the central maximum (zeroth order) and one of the diffracted maxima.
  • 3. Calculation:
  • – Use the grating equation:
  • [math]d sin⁡θ = mλ[/math]
  • Where:
  • – d is the grating spacing (the reciprocal of the number of lines per unit length)
  • – m is the order of the maximum,
  • – λ is the wavelength.
  • Rearranging, solve for the wavelength:
  • [math]\lambda = \frac{d \sin \theta}{m}[/math]
  • – Insert the measured angle and known d to calculate λ.
  • ⇒  Points to Consider:

  • Use the first order maximum (m=1) for ease of measurement.
  • Ensure the grating is well aligned with the incident beam for accurate angle measurements.
  • 3. Determination of the Speed of Sound Using Stationary Waves

  • ⇒  Objective:

  • Measure the speed of sound by creating and analyzing standing (stationary) waves in a resonant tube.
  • ⇒  Apparatus:

  • – Resonance tube (open at one end and closed at the other, or both ends open)
  • – Tuning forks of known frequency, or a signal generator with a speaker
  • – Meter stick or measuring tape
  • – Water bath (if using a variable-length tube submerged in water)
  • – Microphone and oscilloscope or sound level meter (for precise detection of resonance)
  • ⇒   Procedure:

  • 1. Setup:
  • – Arrange the resonance tube vertically or horizontally. For a tube with one closed end and one open end, the resonant condition occurs when a node forms at the closed end and an antinode at the open end.
  • – If using a water-filled tube, adjust the water level to change the effective length of the air column.
  • 2. Generating Standing Waves:
  • – Strike a tuning fork with a known frequency (f) and hold it near the open end of the tube, or drive a speaker with the signal generator at a fixed frequency.
  • – Slowly adjust the length of the tube (or water level) until a strong resonance (maximum sound amplitude) is detected. The positions of resonant conditions can be identified by observing peaks in the sound amplitude (using an oscilloscope or sound level meter).
  • Figure 3 Speed of sound using stationary wave
  • 3. Determining Wavelength:
  • – For a tube open at one end, the fundamental mode of resonance occurs when the length LLL of the air column is approximately:
  • [math]L = \frac{λ}{4}[/math]
  • – For higher modes, the relation is:
  • [math]L = \frac{(2n – 1)\lambda}{4}, \quad n = 1, 2, 3, \ldots[/math]
  • – Measure the length L corresponding to a resonance and calculate the wavelength:
  • [math]L = \frac{4\lambda}{2n – 1}[/math]
  • (Use n=1 for the fundamental frequency.)
  • 4. Calculating the Speed of Sound:
  • – The speed of sound v is related to the wavelength and frequency by:
  • [math]v = fλ[/math]
  • – Substitute the measured frequency and calculated wavelength to obtain v.
  • ⇒  Points to Consider:
  • The accuracy of the speed of sound measurement depends on precise determination of the resonant length and the frequency of the tuning fork.
  • Temperature, humidity, and air pressure affect the speed of sound, so record environmental conditions if high precision is required.
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