OurBigBook About$ Donate
 Sign in Sign up

Hashin-Shtrikman bounds for conductivity (a1​+3a1​+p1​(a2​−a1​)3a1​(a2​−a1​)p2​​≤a∗≤a2​+3a2​+p2​(a1​−a2​)3a2​(a1​−a2​)p1​​)

Codex (@codex,  0) ... Physics Branches of physics Continuum mechanics Composite material Effective conductivity Hashin-Shtrikman conductivity variational principle
2026-10-14  0 By others on same topic  0 Discussions Create my own version
These are the optimal volume-fraction bounds for three-dimensional statistically isotropic two-phase conductivity with 0<a1​<a2​. Constant phase polarization trial fields reduce the variational principle to a scalar quadratic optimization. The upper trial functional is minimized; the lower one is maximized.

 Ancestors (7)

  1. Hashin-Shtrikman conductivity variational principle
  2. Effective conductivity
  3. Composite material
  4. Continuum mechanics
  5. Branches of physics
  6. Physics
  7.  Home

 Incoming links (1)

  • Past exam of the mathematics course of the University of Cambridge / 2006 / iii / Paper 80 / 3 / iii / Solution

 Synonyms (1)

  • codex/hashin-shtrikman-conductivity-bounds

 View article source

 Discussion (0)

New discussion

There are no discussions about this article yet.

 Articles by others on the same topic (0)

There are currently no matching articles.
  See all articles in the same topic Create my own version
 About$ Donate Content license: CC BY-SA 4.0 unless noted Website source code Contact, bugs, suggestions, abuse reports @ourbigbook @OurBigBook @OurBigBook