/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 54 A soap film \((n=1.33)\) is \(46... [FREE SOLUTION] | 91Ó°ÊÓ

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A soap film \((n=1.33)\) is \(465 \mathrm{nm}\) thick and lies on a glass plate \((n=1.52) .\) Sunlight, whose wavelengths (in vacuum) extend from 380 to \(750 \mathrm{nm},\) travels through the air and strikes the film perpendicularly. For which wavelength(s) in this range does destructive interference cause the film to look dark in reflected light?

Short Answer

Expert verified
Destructive interference occurs for 492.0 nm.

Step by step solution

01

Identify the conditions for destructive interference

In general, destructive interference occurs when the path difference is an odd multiple of half-wavelengths. The condition for destructive interference in a film of thickness \( t \) is given by \( 2nt = (m + \frac{1}{2})\lambda' \), where \( n \) is the refractive index of the film, \( \lambda' \) is the wavelength of light in the film, and \( m \) is an integer. For no phase change upon reflection, we apply the condition directly.
02

Calculate the wavelength in the film

The wavelength of light in the film \( \lambda' \) is related to the wavelength in vacuum \( \lambda \) by \( \lambda' = \frac{\lambda}{n} \). Therefore, let \( \lambda_\text{air} = \lambda \) be the wavelength in air; we substitute into the condition: \( 2nt = (m + \frac{1}{2}) \frac{\lambda}{n} \).
03

Rearrange the equation for wavelength in vacuum

Rearrange the expression to find \( \lambda \):\[ \lambda = \frac{2nt}{(m + \frac{1}{2})} \]Substitute given values: \( n = 1.33 \), \( t = 465\ \mathrm{nm} \), to find specific wavelengths.
04

Substitute and solve for permissible wavelengths

Substitute \( n = 1.33 \), \( t = 465 \) nm into the equation:\[ \lambda = \frac{2 \times 1.33 \times 465}{(m + \frac{1}{2})} \]Calculate for different values of \( m \) to find those wavelengths within the range 380 nm to 750 nm.
05

Find admissible wavelengths

Calculate the values:- For \( m = 0 \), \( \lambda = \frac{2 \times 1.33 \times 465}{0.5} = 2465.4 \) nm (out of range).- For \( m = 1 \), \( \lambda = \frac{2 \times 1.33 \times 465}{1.5} = 821.8 \) nm (out of range).- For \( m = 2 \), \( \lambda = \frac{2 \times 1.33 \times 465}{2.5} = 492.0 \) nm (in range).- For \( m = 3 \), \( \lambda = \frac{2 \times 1.33 \times 465}{3.5} = 351.7 \) nm (out of range).Thus, only \( 492.0 \) nm is in the visible range (380 nm - 750 nm).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Destructive Interference
Destructive interference occurs when two waves combine to create a smaller amplitude wave, or cancel each other out. This happens when the waves are out of phase. In thin films like soap, particular conditions determine when this occurs.
- For a thin film interference, destructive interference appears when the optical path difference between two reflective light waves is an odd multiple of half the wavelength - The formula is given by \( 2nt = (m + \frac{1}{2})\lambda' \), - \( t \) is the thickness of the film. - \( n \) is the refractive index. - \( \lambda' \) is the wavelength in the film. - \( m \) is an integer.
This condition allows the film to appear darker where specific wavelengths are canceled out. In our soap film problem, the condition ensures that some wavelengths vanish, rendering dark spots visible in reflected light.
Wavelength Calculation
Calculating the wavelength for thin film interference involves understanding how light behaves in different mediums. Since destructive interference requires specific conditions, calculating which wavelengths will cause this effect is crucial.
Here's how: - The wavelength of light in a film \( \lambda' \) is modified from its vacuum value \( \lambda \) by the film's refractive index \( n \). - It changes by the relation \( \lambda' = \frac{\lambda}{n} \). - The equation to find specific wavelength in air for destructive interference is rearranged to: \[ \lambda = \frac{2nt}{(m + \frac{1}{2})} \]
In our soap film example, values from the formula are substituted to determine acceptable wavelengths that lead to destructive interference. By trying different integer values of \( m \), wavelengths \( \lambda \) within the observable spectrum are identified.
Refractive Index
The refractive index \( n \) of a material is key to understanding how light changes speed when it enters a medium. It is defined by the ratio of the speed of light in vacuum to that in the medium.
- In optics, \( n \) quantifies how much a material can bend light or slow it down.- It directly affects the wavelength of light within the medium. - In our problem, the refractive index of the soap film was given as 1.33. - A higher refractive index means the light travels slower, shortening its wavelength inside the material.
A proper comprehension of the refractive index helps in precisely calculating which wavelengths result in destructive interference in a thin film.
Optical Path Difference
Optical path difference (OPD) is the difference in the path traveled by two light waves as they exit a medium like a thin film. In our case, it determines where light waves either constructively or destructively interfere.
- It accounts for both the physical distance and the change in phase that occurs to light within the film.- Two waves reflect from different interfaces in a film and their phase shift upon reflection adds to the OPD. - The effective extra length the wave travels is \( 2nt \), due to the film walls being traversed twice.- Ensuring the optical path difference matches an integer multiple plus half of wavelengths is crucial for causing destructive interference.
In our scenario, this calculated OPD helps identify the right conditions for when wavelengths are completely canceled out, making the film appear dark when viewed against reflected light.

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Most popular questions from this chapter

A transparent film \((n=1.43)\) is deposited on a glass plate \((n=1.52)\) to form a nonreflecting coating. The film has a thickness that is \(1.07 \times 10^{-7} \mathrm{m} .\) What is the longest possible wavelength (in vacuum) of light for which this film has been designed?

Late one night on a highway, a car speeds by you and fades into the distance. Under these conditions the pupils of your eyes have diameters of about \(7.0 \mathrm{mm}\). The taillights of this car are separated by a distance of \(1.2 \mathrm{m}\) and emit red light (wavelength \(=660 \mathrm{nm}\) in vacuum). How far away from you is this car when its taillights appear to merge into a single spot of light because of the effects of diffraction?

Two parallel slits are illuminated by light composed of two wavelengths. One wavelength is \(\lambda_{\mathrm{A}}=645 \mathrm{nm} .\) The other wavelength is \(\lambda_{\mathrm{B}}\) and is unknown. On a viewing screen, the light with wavelengthV \(\lambda_{\mathrm{A}}=645 \mathrm{nm}\) produces its third-order bright fringe at the same place where the light with wavelength \(\lambda_{\mathrm{B}}\) produces its fourth dark fringe. The fringes are counted relative to the central or zeroth-order bright fringe. What is the unknown wavelength?

The wavelength of the laser beam used in a compact disc player is \(780 \mathrm{nm}\). Suppose that a diffraction grating produces first-order tracking beams that are \(1.2 \mathrm{mm}\) apart at a distance of \(3.0 \mathrm{mm}\) from the grating. Estimate the spacing between the slits of the grating.

In a Young's double-slit experiment, two rays of monochromatic light emerge from the slits and meet at a point on a distant screen, as in Figure \(27.6 a .\) The point on the screen where these two rays meet is the eighth-order bright fringe. The difference in the distances that the two rays travel is \(4.57 \times 10^{-6} \mathrm{m} .\) What is the wavelength (in \(\mathrm{nm}\) ) of the monochromatic light?

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