Math Problem Statement

A 627-nm-thick soap film (n = 1.49) in air is illuminated with white light in a direction perpendicular to the film. For how many different wavelengths in the 300 to 700 nm range is there (a) fully constructive interference and (b) fully destructive interference in the reflected light?

Solution

To solve the problem:

We are working with a soap film of thickness t=627nmt = 627 \, \text{nm}, refractive index n=1.49n = 1.49, and light in the wavelength range 300nm300 \, \text{nm} to 700nm700 \, \text{nm}.


(a) Fully Constructive Interference

Constructive interference in the reflected light occurs when:

2nt=mλ2 n t = m \lambda

Where:

  • nn is the refractive index (1.491.49),
  • tt is the thickness (627nm627 \, \text{nm}),
  • mm is the interference order (m=1,2,3,m = 1, 2, 3, \dots),
  • λ\lambda is the wavelength of light.

Rewriting for λ\lambda:

λ=2ntm\lambda = \frac{2 n t}{m}

The range for λ\lambda is 300nmλ700nm300 \, \text{nm} \leq \lambda \leq 700 \, \text{nm}. Substituting 2nt=21.49627=1868.46nm2 n t = 2 \cdot 1.49 \cdot 627 = 1868.46 \, \text{nm}:

m=1868.46λm = \frac{1868.46}{\lambda}

To find valid mm, compute mm for the extremes of λ\lambda and round to the nearest integers:

  • At λ=300nm\lambda = 300 \, \text{nm}: mmax=1868.463006.23m=6m_{\text{max}} = \frac{1868.46}{300} \approx 6.23 \rightarrow m = 6,
  • At λ=700nm\lambda = 700 \, \text{nm}: mmin=1868.467002.67m=3m_{\text{min}} = \frac{1868.46}{700} \approx 2.67 \rightarrow m = 3.

Thus, m=3,4,5,6m = 3, 4, 5, 6, giving 4 wavelengths for fully constructive interference.


(b) Fully Destructive Interference

Destructive interference in the reflected light occurs when:

2nt=(m+12)λ2 n t = \left( m + \frac{1}{2} \right) \lambda

Rewriting for λ\lambda:

λ=2ntm+12\lambda = \frac{2 n t}{m + \frac{1}{2}}

Substituting 2nt=1868.46nm2 n t = 1868.46 \, \text{nm}:

m+12=1868.46λm + \frac{1}{2} = \frac{1868.46}{\lambda}

Compute m+12m + \frac{1}{2} for the extremes of λ\lambda:

  • At λ=300nm\lambda = 300 \, \text{nm}: mmax+12=1868.463006.23m=5m_{\text{max}} + \frac{1}{2} = \frac{1868.46}{300} \approx 6.23 \rightarrow m = 5,
  • At λ=700nm\lambda = 700 \, \text{nm}: mmin+12=1868.467002.67m=2m_{\text{min}} + \frac{1}{2} = \frac{1868.46}{700} \approx 2.67 \rightarrow m = 2.

Thus, m=2,3,4,5m = 2, 3, 4, 5, giving 4 wavelengths for fully destructive interference.


Final Answer:

(a) 4 wavelengths for fully constructive interference,
(b) 4 wavelengths for fully destructive interference.


Would you like further clarification or step-by-step details? Here are some related questions:

  1. How does the thickness of the film affect interference patterns?
  2. Can this calculation be extended to non-visible wavelengths?
  3. What happens if the film is illuminated at an angle?
  4. How does a change in the refractive index nn modify results?
  5. What is the role of the phase shift in thin-film interference?

Tip: Always verify the interference condition equations with the boundary conditions of the system!

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Math Problem Analysis

Mathematical Concepts

Wave Interference
Thin-Film Optics
Wavelength Calculation

Formulas

2 n t = m λ for constructive interference
2 n t = (m + 1/2) λ for destructive interference

Theorems

Thin-Film Interference Theorem

Suitable Grade Level

College-level Physics