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If first-order reflection occurs in a crystal at Bragg angle \(3.4^{\circ}\), at what Bragg angle does second-order reflection occur from the same family of reflecting planes?

Short Answer

Expert verified
The second-order reflection occurs at a Bragg angle of approximately \(6.8^{\circ}\).

Step by step solution

01

Understand Bragg's Law

Bragg's Law is given by the formula \( n\lambda = 2d\sin\theta \), where \( n \) is the order of reflection, \( \lambda \) is the wavelength of the X-rays, \( d \) is the distance between the crystal planes, and \( \theta \) is the Bragg angle. For this problem, we need to find the Bragg angle for the second order \( (n=2) \).
02

Calculate for the First Order

Given that the first-order reflection occurs at a Bragg angle \( \theta_1 = 3.4^{\circ} \), we have \( n_1 = 1 \). From Bragg's Law equation for the first order, \( \lambda = 2d\sin(3.4^{\circ}) \).
03

Set Up Equation for Second Order

For second-order reflection, \( n_2 = 2 \). Substitute back into Bragg's Law to find \( \theta_2 \): \( 2\lambda = 2d\sin\theta_2 \). Simplifying, \( \lambda = d\sin\theta_2 \). Thus, \( \sin\theta_2 = 2\sin(3.4^{\circ}) \).
04

Calculate \( \sin\theta_2 \)

Using the earlier equality \( \sin\theta_2 = 2\sin(3.4^{\circ}) \) and calculating, \( \sin(3.4^{\circ}) \approx 0.059 \). So, \( \sin\theta_2 = 2(0.059) = 0.118 \).
05

Find \( \theta_2 \)

To find \( \theta_2 \), calculate \( \theta_2 = \arcsin(0.118) \), which gives \( \theta_2 \approx 6.8^{\circ} \).

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Key Concepts

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

X-ray Diffraction
X-ray diffraction is a fascinating process where X-rays are projected onto a crystal, and the way they bounce back or are reflected tells us about the structure inside the crystal. When X-rays hit a crystal, they interact with the electrons in the atoms and scatter, creating a pattern. This pattern helps scientists understand the arrangement of atoms within the crystal.

Bragg's Law is a critical part of X-ray diffraction, providing the mathematical framework needed to interpret these patterns. It takes into account the wavelength of the X-rays and the distance between the planes of atoms in the crystal lattice. By using the angle at which X-rays are reflected, called the Bragg angle, scientists can solve for the spacing between atomic layers, much like using a key to unlock hidden information inside the crystal.

The whole process resembles how light reflects off surfaces, but with X-rays, the level of detail allows us to "see" inside the crystal and map out its structure precisely. X-ray diffraction is a cornerstone technique in fields like material science and chemistry because it provides insights that are otherwise invisible.
Crystallography
Crystallography is the scientific study of crystals, focusing on understanding how they form, the way atoms are arranged within them, and their properties. It is fundamentally linked to X-ray diffraction, as the patterns produced during diffraction are analyzed to determine the crystal's internal structure.

Crystals are not just pretty stones or gems; they are ordered structures where atoms are arranged in a repeating pattern. This repeating pattern is known as a lattice, and each building block of the lattice is termed a unit cell. The unit cell is the smallest portion of the crystal that, when stacked in three-dimensional space, recreates the entire lattice of the crystal.

By studying crystals through X-ray diffraction, crystallographers can determine how atoms are spaced, oriented, and bonded together. This information is crucial for developing new materials and understanding physical properties such as hardness, melting point, and conductivity. Crystallography plays a pivotal role in fields as diverse as pharmaceuticals, nanotechnology, and geology, providing insights that drive innovations.
Angle of Reflection
The angle of reflection in the context of Bragg's Law and X-ray diffraction is the angle at which X-rays bounce off crystal planes. This angle is known as the Bragg angle and is central to determining the structure within the crystal. Bragg's Law is described by the formula: \[ n\lambda = 2d\sin\theta \]where \( n \) is the order of reflection, \( \lambda \) is the wavelength of the X-rays, \( d \) is the interplanar distance in the crystal, and \( \theta \) is the Bragg angle.

The angle of reflection changes depending on which "order" of reflection is being observed (e.g., first-order, second-order), guided by the integer \( n \). As seen in the exercise, by knowing the first-order Bragg angle, one can calculate the angle for the second order. The relationship is proportional, such that for higher orders of reflection, the angle calculated will be larger if the distance \( d \) and wavelength \( \lambda \) remain constant.

Understanding the angle of reflection helps in calculating exact dimensions within crystals and highlights how precise and repeatable patterns translate into the broader understanding of crystalline structures.

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Most popular questions from this chapter

Sound waves with frequency \(3000 \mathrm{~Hz}\) and speed \(343 \mathrm{~m} / \mathrm{s}\) diffract through the rectangular opening of a speaker cabinet and into a large auditorium of length \(d=100 \mathrm{~m}\). The opening, which has a horizontal width of \(30.0 \mathrm{~cm}\), faces a wall \(100 \mathrm{~m}\) away (Fig. 36-36). Along that wall, how far from the central axis will a listener be at the first diffraction minimum and thus have difficulty hearing the sound? (Neglect reflections.)

How far from grains of red sand must you be to position yourself just at the limit of resolving the grains if your pupil diameter is \(1.5 \mathrm{~mm}\), the grains are spherical with radius \(50 \mu \mathrm{m}\), and the light from the grains has wavelength \(650 \mathrm{~nm} ?\) (b) If the grains were blue and the light from them had wavelength \(400 \mathrm{~nm}\), would the answer to (a) be larger or smaller?

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