Book cover for Materials Science and Engineering: An Introduction

Materials Science and Engineering: An Introduction

William D. Callister, Jr. David G. Rethwisch

ISBN #9780471736967

7th Edition

771 Questions

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65,043 Students Helped

Homework Questions

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Summary

Learning Objectives

Key Concepts

Example Problems

Explanations

Common Mistakes

Summary

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Learning Objectives

Key Concepts

CONCEPT

DEFINITION

Ceramics Fabrication Techniques

The methods and processes used for shaping, forming, and consolidating ceramic materials into final products with desired properties.

Example Problems

Example 1

Calculate the fraction of atom sites that are vacant for copper at its melting temperature of $1084^{\circ} \mathrm{C}(1357 \mathrm{K}) .$ Assume an energy for vacancy formation of $0.90 \mathrm{eV} /$ atom.

Example 2

Calculate the number of vacancies per cubic meter in gold at $900^{\circ} \mathrm{C}$. The energy for vacancy formation is 0.98 eVlatom. Furthermore, the density and atomic weight for Au are $18.63 \mathrm{g} / \mathrm{cm}^{3}$ (at $\left.900^{\circ} \mathrm{C}\right)$ and $196.9 \mathrm{g} / \mathrm{mol}$, respectively

Example 3

Calculate the energy for vacancy formation in silver, given that the equilibrium number of vacancies at $800^{\circ} \mathrm{C}(1073 \mathrm{K})$ is $3.6 \times 10^{23} \mathrm{m}^{-3}$. The atomic weight and density (at $\left.800^{\circ} \mathrm{C}\right)$ for silver are, respectively, $107.9 \mathrm{g} / \mathrm{mol}$ and $9.5 \mathrm{g} / \mathrm{cm}^{3}$

Example 4

Below, atomic radius, crystal structure, electronegativity, and the most common valence are tabulated, for several elements; for those that are nonmetals, only atomic radii are indicated. Which of these elements would you expect to form the following with nickel (a) A substitutional solid solution having complete solubility (b) A substitutional solid solution of incomplete solubility (c) An interstitial solid solution

Example 5

For both $\mathrm{FCC}$ and $\mathrm{BCC}$ crystal structures there are two different types of interstitial sites. In each case, one site is larger than the other, and is normally occupied by impurity atoms. For FCC, this larger one is located at the center of each edge of the unit cell; it is termed an octahedral interstitial site. On the other hand, with BCC the larger site type is found at $0 \frac{1}{2} \frac{1}{4}$ positions - that is, lying on \{100\} faces, and situated midway between two unit cell edges on this face and one-quarter of the distance between the other two unit cell edges; it is termed a tetrahedral interstitial site. For both $\mathrm{FCC}$ and $\mathrm{BCC}$ crystal structures, compute the radius $r$ of an impurity atom that will just fit into one of these sites in terms of the atomic radius $R$ of the host atom.

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