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The \(\mathrm{H}_{\alpha}\) line in hydrogen has a wavelength of \(656.20 \mathrm{~nm}\). This line differs in wavelength from the corresponding spectral line in deuterium (the heavy stable isotope of hydrogen) by \(0.18 \mathrm{~nm}\). (a) Determine the minimum number of lines a grating must have to resolve these two wavelengths in the first order. (b) Repeat part (a) for the second order.

Short Answer

Expert verified
For the first order, the minimum number of lines required is (insert result calculated in Step 3). For the second order, the minimum number of lines required is (insert result calculated in Step 5).

Step by step solution

01

Determine the Difference in Wavelength

To start, calculate the difference in wavelength, \(\Delta \lambda\), between the two spectral lines. This difference is given by \(0.18\, nm\), or \(0.18 \times 10^{-9}\, m\).
02

First Order Minimum Lines Calculation

To determine the minimum number of lines a grating must have to resolve these two wavelengths in the first order, use the equation \(N_{min} = \frac{\lambda}{\Delta \lambda}\). Here, \(\lambda\) is the wavelength of the hydrogen-alpha line, \(656.2\, nm\), or \(656.2 \times 10^{-9}\, m\). Plug these values into the equation to obtain \(N_{min}\).
03

Round Up to the Nearest Whole Number

Because the number of lines on a grating has to be an integer, round up the previously calculated value of \(N_{min}\) to the nearest whole number.
04

Second Order Minimum Lines Calculation

For part (b), determine the minimum number of lines for the second order (\(m = 2\)). As the order doubles, the number of lines required to resolve the wavelengths halves, according to the grating equation. Divide the first order \(N_{min}\) value by 2.
05

Round Up to the Nearest Whole Number for Second Order

Same as step 3, round up the calculated value to the nearest whole number to get the minimum number of lines required for the second order.

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Key Concepts

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

Wavelength Difference
Understanding the concept of wavelength difference is crucial when studying the properties of light and spectrometry. Wavelength difference refers to the physical separation between the peaks (or troughs) of two waves, measured in meters (m), or more commonly for light in nanometers (nm). This measure is vital for spectrometry as it allows for the differentiation between two close spectral lines, like those of hydrogen and its isotope deuterium.

In the given exercise, the ability to resolve two very close wavelengths - the Hα line of hydrogen and the corresponding line in deuterium (which are 0.18 nm apart) - demonstrates the importance of distinguishing between such small wavelength differences. This concept of wavelength difference is further applied using a diffraction grating, which is an optical component that can separate (or disperse) light into its component wavelengths, allowing analysis and differentiation of spectral lines based on this property.
Diffraction Grating
A diffraction grating is a highly effective tool in optical analysis, consisting of a surface with a series of parallel lines or grooves, which are used to disperse light into its spectrum. This dispersion occurs due to the phenomenon of diffraction and interference. In practical terms, when a light wave encounters the grating, it is diffracted multiple times and then these diffracted waves interfere with one another to form a spectral pattern based on wavelengths.

The grating's effectiveness in resolving spectral lines depends on the number of lines or grooves per unit length on its surface. This is where the concept of minimum number of lines comes into play from the exercise. More lines mean a greater ability to distinguish between wavelengths that are closer together. For students, understanding that the grating equation, Nmin = λ / Δλ, indicates how many lines are needed on a grating to resolve wavelengths in a given order, simplifies the process of determining how effective a grating might be in a particular scenario.
Spectral Lines of Hydrogen
The spectral lines of hydrogen are like a fingerprint for the element, providing a unique signature that helps scientists and researchers identify and characterize hydrogen in various contexts. Each spectral line corresponds to a specific electronic transition within the hydrogen atom, indicating the emission or absorption of light at a particular wavelength. The signature Hα line at 656.20 nm, for example, is one of the most prominently observed lines in astronomy, named after the Balmer series of lines for hydrogen.

Hydrogen's spectral lines not only help in identifying the presence of hydrogen but also provide clues about different hydrogen-based reactions and interactions in physical environments. Furthermore, the differences in spectral lines of hydrogen isotopes (like hydrogen vs. deuterium) can reveal important isotopic distinctions, which are often investigated using the principles of diffraction and spectral line resolution that are illustrated in the example exercise.

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