Elasticity

The Physics Hypertextbook
© 1998-2008 by Glenn Elert -- A Work in Progress
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Discussion

Elasticity is the tendency of objects to return to their original shape and size after a force deforming them has been removed.

Recall Hooke's law from mechanics. First stated formally by Robert Hooke (1635-1703) of England in The True Theory of Elasticity or Springiness (1676). Written in Latin as "ut tensio, sic vis", which translates to "as is the extension, so is the force" or in contemporary language "extension is directly proportional to force". No portrait of Hooke is known to exist.

Hooke's law can be generalized to "stress is proportional to strain"; where "strain" refers to a change in some spatial dimension (length or volume, for example) and "stress" refers to the cause of the change (force or pressure, for example).

A coefficient that relates a particular type of stress to the strain that results is called a modulus (plural, moduli).

Young's Modulus (Y)

F  = Y 
Δ
A 0

Named for Thomas Young (1773-1829) who also first stated the formulas for work and kinetic energy and also demonstrated that light is a wave.


[magnify]

Shear Modulus (S)

F  = S 
Δx
A y

Gases and liquids can not have shear moduli. They have viscosity instead.


[magnify]

Bulk Modulus (B)

F  = B 
ΔV
A V0


[magnify]

elastic limits

From somewhere: Elinvar is a trademark for a kind of nickel-chromium steel used for watch springs because its elasticity is constant over a wide range of temperatures

From New Scientist: When warmed, the alloys barely expand. This rare, 'invar' behaviour is characteristic of some nickel-steel mixes that were discovered in the 1890s and are used in parts of delicate mechanisms such as wristwatches and scientific measuring instruments. This refusal to expand when warmed means that the devices are accurate across a range of temperatures.

The new compounds also show 'elinvar' behaviour - their stiffness remains constant when they are heated. This effect holds over an amazingly wide temperature range - from as low as -194 °C to over 200 °C.

Strengths of Selected Materials (MPa)
material compressive limit tensile limit young's modulus
hard steel 552 827 207,000
rubber 2.1 1
granite 145 4.8 51,700
concrete 21 2.1 16,500
oak 59 117 11,000
porcelain 552 5.5
compact bone 170 120 17,900
trabecular bone 2.2 76
Source: Physics of the Body

Summary

Problems

practice

  1. Write something.
    • Answer it.
  2. Write something else.
    • Answer it.
  3. Write something different.
    • Answer it.
  4. Write something completely different.
    • Answer it.

numerical

  1. problems

Resources


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