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A diffraction grating is illuminated simultaneously with red light of wavelength \(660 \mathrm{nm}\) and light of an unknown wavelength. The fifth- order maximum of the unknown wavelength exactly overlaps the third-order maximum of the red light. What is the unknown wavelength?

Short Answer

Expert verified
The unknown wavelength is approximately 1,100 nm.

Step by step solution

01

Understanding of Diffraction Grating Formula

The diffraction grating formula is given as: \(d \cdot \sin{\theta} = m \cdot \lambda\). Here, \(d\) is the distance between the slits, \(\theta\) is the angle of deviation, \(m\) is the order maximum, and \(\lambda\) is the wavelength. Since the angle of deviation for the two lights is the same in this scenario, we get the formula for the unknown wavelength as: \( \lambda' = \frac{m' \cdot \lambda}{m}\) where \(\lambda'\) is the unknown wavelength, \(m'\) is the order maximum of the unknown light, and \(m\) is the order maximum of the known light.
02

Substituting Given Values

Now, for the unknown wavelength, we substitute the given values into the formula: \( \lambda' = \frac{5 \cdot 660 nm}{3}\). All we have to do is perform the calculation.
03

Calculation of unknown wavelength

Upon calculation, we get \( \lambda' \approx 1,100 nm\). This indicates that the unknown light has a wavelength of approximately 1,100 nm.

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Key Concepts

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

Wavelength Calculation
In the given problem, understanding how to calculate the wavelength using a diffraction grating is crucial. Diffraction gratings are optical devices used to split light into several beams. They contain many small slits separated by precise distances known as the grating spacing, denoted by \(d\). The formula for diffraction through a grating is \(d \cdot \sin{\theta} = m \cdot \lambda\), where \( \theta \) is the angle of diffraction, \(m\) is the order of the maximum, and \(\lambda\) is the light's wavelength.

To find an unknown wavelength, we leverage the situation where maxima from two different light sources coincide. In our scenario, this happens when the fifth-order maximum of light with unknown wavelength overlaps with the third-order maximum of known red light. Using the relationship \(\lambda' = \frac{m' \cdot \lambda}{m}\), we can isolate the unknown \(\lambda'\) by substituting appropriate values for \(m'\), \(m\), and \(\lambda\). This methodology allows us to pinpoint specific wavelengths by comparing two beams with known orders.
Order Maximum
The term 'order maximum' refers to the integer values \(m\) that satisfy the diffraction condition for constructing maxima, where a beam of light disperses when it passes through a grating. Each integer \(m\) corresponds to a bright fringe or maximum in the interference pattern, with the zeroth order \( (m = 0) \) being the original light beam without deviation.

In composite light beams, different wavelengths can have their maxima at different orders. By carefully analyzing the orders where these maxima coincide for two wavelengths, the formula \(\lambda' = \frac{m' \cdot \lambda}{m}\) helps infer the unknown component. Here, for example, we calculated that the third-order maximum of red light and the fifth-order maximum of the unknown overlap, revealing crucial details about their respective wavelengths.
Optics
Optics generally deals with the behavior and properties of light. Within this field, diffraction grating is an essential concept. Gratings diffract light into various directions by construction, effectively determining the spectrum by angular dispersion.

Essential to optics knowledge are:
  • Wave-like behavior: Light behaves as a wave, and phenomena like diffraction and interference dominate in its analysis.
  • Grating equation: Helps relate slit spacing, diffraction angle, and order to calculate wavelength.
  • Spectroscopy: Utilizes diffraction gratings to determine wavelengths within light.
Comprehending diffraction and interference principles propels one's understanding of how light can be manipulated and used scientifically, precisely in scenarios like determining unknown wavelengths.
Light Interference
Interference is a principal light phenomenon where waves superimpose, leading to constructive or destructive interference. Constructive interference occurs where wave crests coincide, forming bright maxima. With a diffraction grating, each slit lets through light that interferes with light from neighboring slits.

To visualize, consider two lights of different wavelengths. Their maxima meet where conditions are perfectly constructive. In the problem's context, this alignment identifies when a specific pattern highlights both the lights' wavelengths. As waves overlap, their coherent superposition enables accurate predictions and calculations, leading to precise comprehension of interference fringing and wavelength idiosyncrasies.

Understanding interference affirms diffraction in practical optics, supporting measurement and application methods such as spectroscopy in both scientific and industrial fields.

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Most popular questions from this chapter

One day, after pulling down your window shade, you notice that sunlight is passing through a pinhole in the shade and making a small patch of light on the far wall. Having recently studied optics in your physics class, you're not too surprised to see that the patch of light seems to be a circular diffraction pattern. It appears that the central maximum is about \(1 \mathrm{cm}\) across, and you estimate that the distance from the window shade to the wall is about \(3 \mathrm{m}\). Estimate (a) the average wavelength of the sunlight (in \(\mathrm{nm}\) ) and (b) the diameter of the pinhole (in \(\mathrm{mm}\) ).

You've set up a Michelson interferometer with a helium-neon laser \((\lambda=632.8 \mathrm{nm}) .\) After adjusting mirror \(\mathrm{M}_{2}\) to produce a bright spot at the center of the pattern, you carefully move \(\mathbf{M}_{2}\) away from the beam splatter while counting 1200 new bright spots at the center. Then you put the laser away. Later another student wants to restore the interferometer to its starting condition, but he mistakenly sets up a hydrogen discharge lamp and uses the 656.5 nm emission from hydrogen atoms. He then counts 1200 new bright spots while slowly moving \(\mathrm{M}_{2}\) back toward the beam splitter. What is the net displacement of \(\mathbf{M}_{2}\) when he is done? Is \(\mathrm{M}_{2}\) now closer to or farther from the beam splatter?

A double-slit interference pattern is created by two narrow slits spaced \(0.20 \mathrm{mm}\) apart. The distance between the first and the fifth minimum on a screen \(60 \mathrm{cm}\) behind the slits is \(6.0 \mathrm{mm} .\) What is the wavelength (in \(\mathrm{nm}\) ) of the light used in this experiment?

Light of wavelength 600 mm illuminates a diffraction grating. The second-order maximum is at angle \(39.5^{\circ} .\) How many lines per millimeter does this grating have?

Light emitted by Element X passes through a diffraction grating having 1200 lines/mm. The diffraction pattern is observed on a screen \(75.0 \mathrm{cm}\) behind the grating. Bright fringes are seen on the screen at distances of \(56.2 \mathrm{cm}, 65.9 \mathrm{cm},\) and \(93.5 \mathrm{cm}\) from the central maximum. No other fringes are seen. a. What is the value of \(m\) for each of these diffracted wavelengths? Explain why only one value is possible. b. What are the wavelengths of light emitted by Element X?

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