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A grating has 400 lines/mm. How many orders of the entire visible spectrum \((400-700 \mathrm{~nm})\) can it produce in a diffraction experiment, in addition to the \(m=0\) order?

Short Answer

Expert verified
The grating can produce 6 additional orders for the visible spectrum.

Step by step solution

01

Understand the Grating Equation

The grating equation is given by \( d \sin \theta = m \lambda \), where \( d \) is the grating spacing, \( \theta \) is the diffraction angle, \( m \) is the order number, and \( \lambda \) is the wavelength.
02

Calculate Grating Spacing (d)

The grating spacing \( d \) is the reciprocal of the number of lines per millimeter. Since there are 400 lines/mm, convert it to meters: \( d = \frac{1}{400,000} \text{ meters}.\)
03

Determine Maximum Possible Value of m

The maximum order \( m \) is determined by the condition that \( \sin \theta \leq 1 \). Hence, \( m = \frac{d}{\lambda_{min}} \), where \( \lambda_{min} = 400 \text{ nm} = 400 \times 10^{-9} \text{ meters} \).
04

Calculate Maximum m for \( \lambda=400 \text{ nm} \)

Substitute \( d = \frac{1}{400,000} \) and \( \lambda = 400 \times 10^{-9} \) into \( m = \frac{d}{\lambda} \): \[m = \frac{1}{400,000 \times 400 \times 10^{-9}} = \frac{1}{0.16} \approx 6.25 \].
05

Determine Integral Orders

The largest integer \( m \) is \( 6 \), as the order must be an integer. Since \( m=0 \) is already accounted for, the number of additional visible orders is \( 6\).

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Key Concepts

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

Diffraction Experiment
The diffraction experiment is a fundamental procedure for observing the wave nature of light. When light passes through a diffraction grating, it is split into several beams traveling in different directions. This is because the spacing between the grating lines is comparable in size to the wavelength of light, causing the light waves to interfere with one another.
During a diffraction experiment, a beam of light, such as visible light, is directed towards a grating, which consists of many equally spaced lines. As the light waves pass through these slits, they diffract, or spread out. This splitting of light creates patterns of constructive and destructive interference that can be observed on a screen or detected with sensors.
Key elements to note in a diffraction experiment include:
  • The Source of Light: Usually a monochromatic or a spectrum of light that contains multiple wavelengths.
  • The Grating: A series of parallel lines etched onto a surface. The density of lines is measured in lines per millimeter (lines/mm).
  • The Observation Screen: Where the light pattern is observed, showing various orders of maxima and minima indicating interference.
Grating Equation
The grating equation is an essential formula used to predict the angles at which light will diffract in a diffraction grating setup. It is given by the formula:
\[d \sin \theta = m \lambda\]Here:
  • \(d\): This represents the distance between adjacent lines on the grating, also known as the grating spacing.
  • \(\theta\): The angle of diffraction, which is the angle that a particular order of light is observed.
  • \(m\): The order number, an integer that represents the nth bright fringe in the diffraction pattern.
  • \(\lambda\): The wavelength of light being used, typically measured in nanometers for visible light.
Understanding the grating equation helps us determine the angle at which each wavelength of light is steered, allowing us to calculate how many orders of a spectrum like the visible spectrum can be observed in an experiment.
Order of Diffraction
The order of diffraction, represented by the variable \(m\), is an integer that signifies the series of similar light patterns formed due to diffraction through the grating. Each order corresponds to a different angle where bright and dark fringes appear.
To determine the highest possible order for a given wavelength, the grating equation sets the condition: \(\sin \theta \leq 1\). Therefore, the maximum order observed is given by:
\[m_{\text{max}} = \frac{d}{\lambda_{\text{min}}}\]where \(\lambda_{\text{min}}\) is the shortest wavelength in the spectrum. In practical terms, only those orders where \(m\) is an integer will create visible patterns, and footage can be complex to observe if \(m\) becomes too high due to overlapping patterns.
Visible Spectrum
The visible spectrum covers a range of wavelengths that can be detected by the human eye, approximately from 400 nm to 700 nm. This spectrum includes all the colors from violet to red.
In a diffraction experiment, the visible spectrum allows us to perceive different orders of color patterns. When light diffracts through a grating, each different wavelength (color) bends at a slightly different angle. This separation leads to the beautiful array of spectral colors that can be seen on a screen.
Understanding the visible spectrum is crucial when performing calculations to determine how many orders of diffraction can be observed. Given that each wavelength from violet (400 nm) to red (700 nm) behaves uniquely in a grating setup, it is possible to calculate the range of orders visible to the human eye, making practical observations more versatile and insightful.

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Most popular questions from this chapter

Entoptic halos. If someone looks at a bright outdoor lamp in otherwise dark surroundings, the lamp appears to be surrounded by bright and dark rings (hence halos) that are actually a circular diffraction pattern as in Fig. \(36-10\), with the central maximum overlapping the direct light from the lamp. The diffraction is produced by structures within the cornea or lens of the eye (hence entoptic). If the lamp is monochromatic at wavelength \(550 \mathrm{~nm}\) and the first dark ring subtends angular diameter \(2.5^{\circ}\) in the observer's view, what is the (linear) diameter of the structure producing the diffraction?

Estimate the linear separation of two objects on Mars that can just be resolved under ideal conditions by an observer on Earth (a) using the naked eye and (b) using the 200 in. \((=5.1 \mathrm{~m})\) Mount Palomar telescope. Use the following data: distance to Mars \(=8.0 \times 10^{7} \mathrm{~km}\), diameter of pupil \(=5.0 \mathrm{~mm}\), wavelength of light \(=550 \mathrm{~nm} .\)

A diffraction grating illuminated by monochromatic light normal to the grating produces a certain line at angle \(\theta .(\mathrm{a}) \mathrm{What}\) is the product of that line's half-width and the grating's resolving power? (b) Evaluate that product for the first order of a grating of slit separation \(900 \mathrm{~nm}\) in light of wavelength \(600 \mathrm{~nm}\).

Monochromatic light with wavelength \(538 \mathrm{~nm}\) is incident on a slit with width \(0.025 \mathrm{~mm}\). The distance from the slit to a screen is \(3.5\) \(\mathrm{m}\). Consider a point on the screen \(1.1 \mathrm{~cm}\) from the central maximum. Calculate (a) \(\theta\) for that point, (b) \(\alpha\), and (c) the ratio of the intensity at that point to the intensity at the central maximum.

A slit \(1.00 \mathrm{~mm}\) wide is illuminated by light of wavelength \(589 \mathrm{~nm}\). We see a diffraction pattern on a screen \(3.00 \mathrm{~m}\) away. What is the distance between the first two diffraction minima on the same side of the central diffraction maximum?

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