Robert Koslover
Certified Consultant
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Posted:
2 years ago
2022年8月17日 GMT-4 17:56
Updated:
2 years ago
2022年8月17日 GMT-4 18:01
There are published papers about graphene. A quick web search finds, among others:
https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6474003/
Just type "electrical conductivity of graphene" into a search engine. Once you identify the value (or values) for its electrical conducticity in your circumstances, plus any other important/needed physical properties of graphene in your model, then you can then define your own material as (for example) "MyGraphene," just as you would any other user-defined material in Comsol Multiphysics.
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Scientific Applications & Research Associates (SARA) Inc.
www.comsol.com/partners-consultants/certified-consultants/sara
There are published papers about graphene. A quick web search finds, among others:
https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6474003/
Just type "electrical conductivity of graphene" into a search engine. Once you identify the value (or values) for its electrical conducticity in your circumstances, plus any other important/needed physical properties of graphene in your model, then you can then define your own material as (for example) "MyGraphene," just as you would any other user-defined material in Comsol Multiphysics.
Please login with a confirmed email address before reporting spam
Posted:
2 years ago
2023年1月10日 GMT-5 11:04
The conductivity is depending on direction, in one direction its metallic, and in the other its semiconducting (x and y along the surface directions). In the conducting direction, lets say x we have as the attached figure says. Number of quantum conductance 2e^2/hN, where N=aD, and a=0.01nm, and D=diameter of graphene flake/ribbon.
Tried simple model with isotropic resistivity (not as I mention above) to use the Contact Impedance, using surface impedance with: surface resistance=Ac/sigG, where sigG=Nc2e_const^2/h_const and Nc=2a/0.01[nm]. It should be better than silver, but it seems comsol only sort of add this resistivity to the bulk resistivity, and nothing interesting happens. rhoBulk=1 and Ac=pia^2, a=0.1 in the model.
To see a more realistic effect i used floating potential on the circle flake instead. The potatial of a metallic flake should be constant over the flake. This works fine. Havn't foond a way to "fool" comsol to do it in the right way. I guess it has to be done with weak formulation...
The conductivity is depending on direction, in one direction its metallic, and in the other its semiconducting (x and y along the surface directions). In the conducting direction, lets say x we have as the attached figure says. Number of quantum conductance 2e^2/h*N, where N=a*D, and a=0.01nm, and D=diameter of graphene flake/ribbon.
Tried simple model with isotropic resistivity (not as I mention above) to use the Contact Impedance, using surface impedance with: surface resistance=Ac/sigG, where sigG=Nc*2*e_const^2/h_const and Nc=2*a/0.01[nm]. It should be better than silver, but it seems comsol only sort of add this resistivity to the bulk resistivity, and nothing interesting happens. rhoBulk=1 and Ac=pi*a^2, a=0.1 in the model.
To see a more realistic effect i used floating potential on the circle flake instead. The potatial of a metallic flake should be constant over the flake. This works fine. Havn't foond a way to "fool" comsol to do it in the right way. I guess it has to be done with weak formulation...