Edexcel A Level (IAL) Physics-2.20 Core Practical 6: Investigating Diffraction Gratings- Study Notes- New Syllabus
Edexcel A Level (IAL) Physics -2.20 Core Practical 6: Investigating Diffraction Gratings- Study Notes- New syllabus
Edexcel A Level (IAL) Physics -2.20 Core Practical 6: Investigating Diffraction Gratings- Study Notes -Edexcel A level Physics – per latest Syllabus.
Key Concepts:
CORE PRACTICAL 6: Determine the Wavelength of Light Using a Diffraction Grating
This experiment uses a diffraction grating to accurately measure the wavelength of a laser or monochromatic light source. It makes use of the diffraction grating equation:
\( n\lambda = d\sin\theta \)
Apparatus![]()
- Laser or monochromatic light source
- Diffraction grating (e.g., 300, 600, or 1000 lines/mm)
- Screen or white wall
- Metre ruler or measuring tape
- Protractor
- Retort stand and clamps
Method
- Fix the diffraction grating securely so that the laser passes perpendicularly through it.
- Place a screen several metres away to allow clear diffraction spots (fringes) to form.
- Mark the central (zero-order) bright spot.
- Mark the first-order and second-order spots on both sides.
- Measure the horizontal distance \( x \) from the central maximum to each side maximum.
- Measure the distance \( L \) from the grating to the screen.
- Calculate the diffraction angle using:
\( \theta = \tan^{-1}\left(\dfrac{x}{L}\right) \)
- Find the grating spacing \( d \) using:
\( d = \dfrac{1}{N} \)
where \( N \) = lines per metre.
- Substitute \( n \), \( d \), and \( \theta \) into:
\( n\lambda = d\sin\theta \)
Important Notes
- Ensure laser hits the grating perpendicular to its surface.
- Use measurements for left and right orders and average them.
- Higher orders increase accuracy but may be dimmer.
- Use a dark room for clearer fringes.
- Always follow laser safety precautions (never look directly into the beam).
Sample Data Table (Typical Format)
- Distance to screen: \( L = 2.50\ \mathrm{m} \)
- Measured for first order:
- \( x_{\text{left}} = 0.82\ \mathrm{m} \)
- \( x_{\text{right}} = 0.80\ \mathrm{m} \)
- Average \( x = 0.81\ \mathrm{m} \)
- Diffraction grating: 600 lines/mm → \( N = 600\times10^3 = 6.00\times10^5\ \mathrm{m^{-1}} \) → \( d = \dfrac{1}{6.00\times10^5} = 1.67\times10^{-6}\ \mathrm{m} \)
Example Calculation
Using the diffraction formula:
- Order: \( n = 1 \)
- \( d = 1.67\times10^{-6}\ \mathrm{m} \)
- \( \theta = \tan^{-1}\left(\dfrac{0.81}{2.50}\right) = 17.8^\circ \)
\( \lambda = \dfrac{d\sin\theta}{n} = \dfrac{1.67\times10^{-6} \sin 17.8^\circ}{1} = \dfrac{1.67\times10^{-6} \times 0.306}{1} = 5.11\times10^{-7}\ \mathrm{m} \)
The wavelength of the laser ≈ \( 510\ \mathrm{nm} \).
Evaluation and Sources of Error
- Ensure grating is perpendicular to laser beam.
- Screen must be flat and directly in line with beam.
- Avoid parallax error when marking fringe positions.
- Use a longer distance \( L \) to reduce percentage uncertainty.
- Avoid stray light and reflections.
Results & Conclusion
- Using a diffraction grating gives very accurate wavelength measurements.
- More lines/mm → sharper fringes → better accuracy.
- Higher order maxima improve precision if visible.
