The following sections of this BookRags Literature Study Guide is offprint from Gale's For Students Series: Presenting Analysis, Context, and Criticism on Commonly Studied Works: Introduction, Author Biography, Plot Summary, Characters, Themes, Style, Historical Context, Critical Overview, Criticism and Critical Essays, Media Adaptations, Topics for Further Study, Compare & Contrast, What Do I Read Next?, For Further Study, and Sources.
(c)1998-2002; (c)2002 by Gale. Gale is an imprint of The Gale Group, Inc., a division of Thomson Learning, Inc. Gale and Design and Thomson Learning are trademarks used herein under license.
The following sections, if they exist, are offprint from Beacham's Encyclopedia of Popular Fiction: "Social Concerns", "Thematic Overview", "Techniques", "Literary Precedents", "Key Questions", "Related Titles", "Adaptations", "Related Web Sites". (c)1994-2005, by Walton Beacham.
The following sections, if they exist, are offprint from Beacham's Guide to Literature for Young Adults: "About the Author", "Overview", "Setting", "Literary Qualities", "Social Sensitivity", "Topics for Discussion", "Ideas for Reports and Papers". (c)1994-2005, by Walton Beacham.
All other sections in this Literature Study Guide are owned and copyrighted by BookRags, Inc.
The strain energy is the potential energy stored in a body when that body is elastically deformed. It is equal to the amount of work required to produce this deformation. A body deforms elastically until the applied stress reaches some maximum value, beyond which the body exhibits permanent deformation. The body need not break at this maximum stress; it will simply not return to its original dimensions if stressed any more. As long as the elastic limit is not exceeded, the strain is directly proportional to the stress. Familiar examples of bodies that behave elastically includ e rubber bands, diving boards, and springs.
If a uniform rod is stretched slowly and elastically, energy will be stored in the rod as elastic energy. The elastic energy stored per unit volume, or strain energy density, is equal to one-half the stress raised to the second power divided, in general, by the Young's modulus. The Young' s modulus is defined as the longitudinal stress divided by the longitudinal strain in the elastic region of deformation; strain is defined as the relative change in dimensions or shape in a body as the result of an applied stress, and is a dimensionless quantity; and stress is the magnitude of the applied force per unit area, usually measured in units of pounds per square inch or pascals.