OCR · A-Level · Physics
Course version: H556 · Version from Sept 2015
(h) the condition for maxima d sin θ = nλ, where d is the grating spacing
Full specification wording
Electromagnetic radiation from stars: (h) the condition for maxima d sin θ = nλ, where d is the grating spacing
For a diffraction grating, constructive interference produces maxima when the path difference between light from adjacent slits equals a whole number of wavelengths.
Checked against the OCR H556 specification (opens in a new tab) on .
- Point 8 of 11
- 4 key terms
Study notes
From the checked teaching notes for this specification point.
The idea
For a diffraction grating, constructive interference produces maxima when the path difference between light from adjacent slits equals a whole number of wavelengths. This condition is d sin θ = nλ, where d is the grating spacing (distance between adjacent slit centres), θ is the angle from the zero-order direction, n is the order (0, 1, 2, ...) and λ is the wavelength. The zero-order maximum (n = 0) occurs at θ = 0° for all wavelengths. Higher orders spread out more, so the grating separates wavelengths, which is why it is used in spectrometry. The maximum possible order is limited because sin θ cannot exceed 1.
What earns the marks
- Constructive interference occurs when the path difference between adjacent slits is a whole number of wavelengths.
- The condition for maxima is d sin θ = nλ, where d is the grating spacing.
- n is the order of the maximum and takes integer values 0, 1, 2, ...
- The zero-order maximum occurs at θ = 0° for all wavelengths.
- The maximum observable order is limited by sin θ ≤ 1, so n ≤ d / λ.
Common mistakes and how to put them right
Treating d as the slit width rather than the distance between adjacent slit centres.
Using degrees in the sine calculation when the calculator is set to radians, or vice versa.
Forgetting that n must be an integer.
Put it right: Non-integer values do not give maxima.
Assuming the zero-order maximum occurs at different angles for different wavelengths.
Put it right: It occurs at θ = 0° for all wavelengths.
Exam tips
- Check that your calculator is in the correct angle mode before evaluating sin θ.
- Rearrange d sin θ = nλ carefully: to find θ use sin θ = nλ / d, then take the inverse sine.
- Remember that the maximum order is the largest integer n for which nλ / d ≤ 1.
Try the lesson
The start of the Electromagnetic radiation from stars: (h) the condition for maxima d sin θ = nλ, where d is the grating spacing lesson, made from checked teaching notes for this specification point.
Listen
For a diffraction grating, constructive interference produces maxima when the path difference between light from adjacent slits equals a whole number of wavelengths. This condition is d sin θ = nλ, where d is the grating spacing (distance between adjacent slit centres), θ is the angle from the zero-order direction, n is the order (0, 1, 2, ...) and λ is the wavelength. The zero-order maximum (n = 0) occurs at θ = 0° for all wavelengths. Higher orders spread out more, so the grating separates wavelengths, which is why it is used in spectrometry. The maximum possible order is limited because sin θ cannot exceed 1. A strong answer earns marks for these points. Constructive interference occurs when the path difference between adjacent slits is a whole number of wavelengths. The condition for maxima is d sin θ = nλ, where d is the grating spacing. n is the order of the maximum and takes integer values 0, 1, 2, ... The zero-order maximum occurs at θ = 0° for all wavelengths. Exam tip: Check that your calculator is in the correct angle mode before evaluating sin θ.
See it
Key words
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Constructive interference condition for multiple slits
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Path difference and order of maxima
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Wavelength separation by a grating
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Limits on observable orders
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See every definition
- Constructive interference condition for multiple slits
- Maxima are produced when the path difference between light from adjacent slits equals a whole number of wavelengths.
- Path difference and order of maxima
- The condition for maxima is d sin θ = nλ, where n is the order and takes integer values 0, 1, 2, ...
- Wavelength separation by a grating
- Higher orders spread out more, so the grating separates wavelengths, which is why it is used in spectrometry.
- Limits on observable orders
- The maximum possible order is limited because sin θ cannot exceed 1, so n ≤ d / λ.
Label the diagram
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