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1. Atom is the basic unit of an element that can undergo physical change.

1. Atom is the basic unit of an element that can undergo physical change.

Introduction to Chemical Engineering Thermodynamics
Introduction to Chemical Engineering Thermodynamics
8th Edition
ISBN:9781259696527
Author:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Publisher:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Chapter1: Introduction
Section: Chapter Questions
Problem 1.1P
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1. Atom is the basic unit of an element that can undergo physical change. (_ 2. Permanent dipole bonds are made of atoms with different electronegativity that are united by covalent bonding. (_ 3. A non-crystalline material has no long-range order, which consists of an amorphous, vitreous, or glassy material. ( 4. Linear density refers to the atomic density in particular crystal directions. 5. Vacancies are an equilibrium defects in metals, which occur about 1 in 10,000 atoms and their energy of formation is about 125 eV. ( 6. Dislocation volume represents the amount of dislocations present. ( 7. The concentration of diffusing species is a function of both time and position C = C(x,t). More likely scenario than non-steady state. (_ 8. Diffusion takes place more rapidly along grain boundaries than in the grain matrix in metals and ceramics.
Transcribed Image Text:1. Atom is the basic unit of an element that can undergo physical change. (_ 2. Permanent dipole bonds are made of atoms with different electronegativity that are united by covalent bonding. (_ 3. A non-crystalline material has no long-range order, which consists of an amorphous, vitreous, or glassy material. ( 4. Linear density refers to the atomic density in particular crystal directions. 5. Vacancies are an equilibrium defects in metals, which occur about 1 in 10,000 atoms and their energy of formation is about 125 eV. ( 6. Dislocation volume represents the amount of dislocations present. ( 7. The concentration of diffusing species is a function of both time and position C = C(x,t). More likely scenario than non-steady state. (_ 8. Diffusion takes place more rapidly along grain boundaries than in the grain matrix in metals and ceramics.
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