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    • https://phys.libretexts.org/Bookshelves/College_Physics/College_Physics_1e_(OpenStax)/05%3A_Further_Applications_of_Newton's_Laws-_Friction_Drag_and_Elasticity/5.03%3A_Elasticity_-_Stress_and_Strain
      A change in shape due to the application of a force is a deformation. Even very small forces are known to cause some deformation. For small deformations, two important characteristics are observed. Fi...A change in shape due to the application of a force is a deformation. Even very small forces are known to cause some deformation. For small deformations, two important characteristics are observed. First, the object returns to its original shape when the force is removed—that is, the deformation is elastic for small deformations. Second, the size of the deformation is proportional to the force—that is, for small deformations, Hooke’s law is obeyed.
    • https://phys.libretexts.org/Courses/Prince_Georges_Community_College/PHY_2040%3A_General_Physics_III/02%3A_Sound/2.1%3A_Introduction
      Sound is a longitudinal wave of pressure that travels through compressible medias, which can be solid, liquid, gaseous, or made of plasma.
    • https://phys.libretexts.org/Courses/Prince_Georges_Community_College/PHY_2040%3A_General_Physics_III/01%3A_Waves_and_Vibrations/1.2%3A_Hookes_Law
      Hooke’s law of elasticity is an approximation that states that the extension of a spring is directly proportional to the load applied to it.
    • https://phys.libretexts.org/Bookshelves/University_Physics/Physics_(Boundless)/15%3A_Waves_and_Vibrations/15.2%3A_Hookes_Law
      Hooke’s law of elasticity is an approximation that states that the extension of a spring is directly proportional to the load applied to it.
    • https://phys.libretexts.org/Courses/Joliet_Junior_College/JJC_-_PHYS_110/05%3A_Book-_Physics_(Boundless)/5.09%3A_Sound/5.9.01%3A_Introduction
      Sound is a longitudinal wave of pressure that travels through compressible medias, which can be solid, liquid, gaseous, or made of plasma.
    • https://phys.libretexts.org/Courses/Prince_Georges_Community_College/General_Physics_I%3A_Classical_Mechanics/50%3A_Elasticity
      We have generally been treating solid bodies as if they are infinitely rigid, and do not deform when forces are applied to them, and this is often not a bad approximation. But in the real world, solid...We have generally been treating solid bodies as if they are infinitely rigid, and do not deform when forces are applied to them, and this is often not a bad approximation. But in the real world, solid bodies do deform somewhat, and we sometimes need to allow for these deformation effects. Elasticity refers to the ability of a material to be deformed somewhat, then return to its original state
    • https://phys.libretexts.org/Bookshelves/University_Physics/Physics_(Boundless)/16%3A_Sound/16.1%3A_Introduction
      Sound is a longitudinal wave of pressure that travels through compressible medias, which can be solid, liquid, gaseous, or made of plasma.
    • https://phys.libretexts.org/Courses/Joliet_Junior_College/JJC_-_PHYS_110/05%3A_Book-_Physics_(Boundless)/5.08%3A_Waves_and_Vibrations/5.8.02%3A_Hookes_Law
      Hooke’s law of elasticity is an approximation that states that the extension of a spring is directly proportional to the load applied to it.
    • https://phys.libretexts.org/Courses/Prince_Georges_Community_College/General_Physics_I%3A_Classical_Mechanics/50%3A_Elasticity/50.01%3A_Introduction_to_Elasticity
      where \(\sigma\) is the stress, \(\varepsilon\) is the strain, and \(E\) is the elastic modulus, which takes the place of the spring constant in Hooke's law. In Eq. \(\PageIndex{1}\), the stress \(\si...where \(\sigma\) is the stress, \(\varepsilon\) is the strain, and \(E\) is the elastic modulus, which takes the place of the spring constant in Hooke's law. In Eq. \(\PageIndex{1}\), the stress \(\sigma\) and elastic modulus \(E\) both have units of \(\mathrm{N} / \mathrm{m}^{2}\); the strain \(\varepsilon\) is dimensionless. In all cases, the stress \(\sigma\) is defined as the force \(F\) applied to the body, divided by the area \(A\) over which the force acts:

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