Non linear properties of Metamaterials

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Discussion Overview

The discussion revolves around the application of Ohm's law in the context of nonlinear metamaterials, specifically focusing on the formulation of equations presented in a research paper. Participants explore the microscopic form of Ohm's law and its implications for nonlinear properties.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant expresses difficulty in understanding how Ohm's law is formulated in the research paper, particularly in relation to nonlinear metamaterials.
  • Another participant proposes a relationship for reactance and impedance, suggesting that Ohm's law can be expressed as j = E/Imp.
  • Further contributions attempt to derive expressions for current density (j) in terms of electric field (E) and impedance, but participants note that these do not yield the required relation.
  • Multiple formulations of j in relation to impedance and resistivity are presented, with variations in the expressions used, indicating different approaches to the problem.
  • One participant mentions the use of impedance and resistivity interchangeably, raising questions about the correct symbols and units involved.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the correct formulation of Ohm's law for nonlinear metamaterials, with multiple competing views and expressions presented throughout the discussion.

Contextual Notes

There are unresolved mathematical steps and dependencies on definitions, particularly regarding the symbols and units used for resistivity and reactance.

Sana5643
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im having diificulty in solving Equations in this research paper
how ohms law has been witten in Eq (1)
how can we write microscopic form of ohms law for non linear meta materials?
 

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Reactance X is proportional to frequency, cross-section and inductance : X = omegaSL. Impedance is Imp = R + iX.
Ohm's law is j = E/Imp.

Agree?
 
j = E / ( R + iωSL)
& by substituting
R = d /ơS
we get
j = EơS / ( d + iωơS2L)
but this is not the required relation ??vj = E / ( R + iωSL)
& by substituting
R = d /ơS
we get
j = EơS / ( d + iωơSSL)
but this is not the required relation ??
 
j=E/impeditivity

j=E/(rho + i X)

j=(sigma/sigma)E/(rho + iX)

j=E/(1 + i(sigma)X)

j=E/(1 + i(sigma)(wSL))
 
... I mean:

j=E/impeditivity

j=E/(rho + iX)

j=(sigma/sigma)E/(rho + iX)

j=sigmaE/(1 + i(sigma)(wSL)
 
i was using relation Z= R +i X with resistance 'R'
it means we can use Z= ρ + i X with resistivity 'ρ' as well
 
Impedance = resistance + i reactance.

multiplying by (cross-section/length) gives:

Impeditivity = resistivity + i reactivity.

(the units are different, so the symbols should also be, but except rho, I'm not sure what they are)
 
Thanks for helping me to understand form of Ohms law given in this paper
 

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