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AP · AP 2 · extended response

A diffraction grating with an impossible order

AP Physics 2: Algebra-Based · Original GioPhysics question with a detailed, mark-by-mark answer guide.

Demand
discriminating
Marks
6
Topics
1
Answer
Complete
Explore the question data

Diffraction orders

Supplied question data. Read the labelled axes and use the observations to test the physical model.

Vertical axis (y): sin θ

Diffraction ordersSupplied question data. Read the labelled axes and use the observations to test the physical model. Horizontal axis: Order n. Vertical axis: sin θ. Exact values are available in the data table below.00.2250.450.6750.900.751.52.253xy

Horizontal axis (x): Order n

Reading 1Order n: 0sin θ: 0
Read the exact data as a table
Diffraction orders — supplied values
Order nsin θ
00
10.3
20.6
30.9

These are the supplied values, not a worked answer. No fitted trend is drawn.

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extended response6 marks

Monochromatic light falls normally on a grating with 500 lines per millimetre. Measured sine of the diffraction angle against order is supplied below. Use c = 3.0×10⁸ m s⁻¹. Angles are measured from the central direction, not from the grating surface. Supplied model: Use d sinθ = nλ and spacing d = 1/(lines per unit length). Supplied data (Order n; sin θ): (0, 0), (1, 0.3), (2, 0.6), (3, 0.9).

  1. (a)

    Find grating spacing, wavelength, frequency and the largest possible order.

    3 marks
  2. (b)

    Explain how to distinguish an aperture's diffraction envelope from the grating's narrow interference maxima, and improve an angle measurement.

    3 marks
Ready to self-mark?Reveal the detailed answer guide
Answer overview(a) d = 2.0 μm; λ = 600 nm; f = 5.0×10¹⁴ Hz; maximum order = 3. (b) Diffraction spreads each slit contribution; interference between the many coherent slit contributions selects the narrow orders.
01

(a)

3 marks

Find grating spacing, wavelength, frequency and the largest possible order.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    500 lines mm⁻¹ is 5.0×10⁵ lines m⁻¹, so d = 1/(5.0×10⁵) = 2.0×10⁻⁶ m.

  2. 2

    From d sinθ = nλ, λ/d is the graph gradient, 0.30; therefore λ = 6.0×10⁻⁷ m and f = c/λ = 5.0×10¹⁴ Hz.

  3. 3

    The condition sinθ≤1 requires n≤d/λ = 3.33. Integer orders stop at n = 3; a fourth order would require sinθ = 1.2.

02

(b)

3 marks

Explain how to distinguish an aperture's diffraction envelope from the grating's narrow interference maxima, and improve an angle measurement.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    The grating equation predicts directions of principal maxima, while finite slit width determines their broad intensity envelope.

  2. 2

    Measure both +n and −n peaks; half their angular separation reduces an offset in the estimated central direction.

  3. 3

    Repeat and use higher visible orders where practical, while avoiding weak peaks and confusion between order number and wavelength. Never view a laser directly.

Complete marking guidance

Use these worked steps alongside the part-by-part answers. They explain the method and mark allocation; they do not add extra marks.

  1. 500 lines mm⁻¹ is 5.0×10⁵ lines m⁻¹, so d = 1/(5.0×10⁵) = 2.0×10⁻⁶ m.
  2. From d sinθ = nλ, λ/d is the graph gradient, 0.30; therefore λ = 6.0×10⁻⁷ m and f = c/λ = 5.0×10¹⁴ Hz.
  3. The condition sinθ≤1 requires n≤d/λ = 3.33. Integer orders stop at n = 3; a fourth order would require sinθ = 1.2.
  4. The grating equation predicts directions of principal maxima, while finite slit width determines their broad intensity envelope.
  5. Measure both +n and −n peaks; half their angular separation reduces an offset in the estimated central direction.
  6. Repeat and use higher visible orders where practical, while avoiding weak peaks and confusion between order number and wavelength. Never view a laser directly.

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Your self-assessment

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