Study of Nanomaterials Under Second Order Bulk Modulus

In this study, we analyze the variation of pressure under different values of (𝑽𝑽𝟎) for nanomaterials using secondorder pressure derivative of bulk modulus equation of state. Second order pressure derivative of bulk modulus show fine studies of nanomaterials. The Gupta & Gupta EOS is used to calculate the resultant data of ε-Fe (Hexagonal iron), α-Fe2O3 and Ni-filled MWCNT nanomaterials and compared with other equations of state, like Tait EOS, Mie–Gruneisen EOS, Vinet EOS and experimental data available in literature. The resultant data show good agreement with experimental data and other EOSs.

Authors

Publication Details

Journal
Indian Journal of Advanced Physics
Published
2024-10-28
DOI
https://doi.org/10.54105/ijap.b1054.04021024
Citations
1
Primary Topic
nanoparticles nucleation surface interactions
Type
article
Field-Weighted Citation Impact
0.38
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article

Study of Nanomaterials Under Second Order Bulk Modulus

Vishal Kumar Singh, Mohit Gupta, Rohit Gupta, Brijendra Kumar Sharma
1 citations
Indian Journal of Advanced Physics
nanoparticles nucleation surface interactions
0.38
article

Study of Nanomaterials Under Second Order Bulk Modulus

Vishal Kumar Singh, Mohit Gupta, Rohit Gupta, Brijendra Kumar Sharma
article en
1 citations

Abstract

In this study, we analyze the variation of pressure under different values of (𝑽𝑽𝟎) for nanomaterials using secondorder pressure derivative of bulk modulus equation of state. Second order pressure derivative of bulk modulus show fine studies of nanomaterials. The Gupta & Gupta EOS is used to calculate the resultant data of ε-Fe (Hexagonal iron), α-Fe2O3 and Ni-filled MWCNT nanomaterials and compared with other equations of state, like Tait EOS, Mie–Gruneisen EOS, Vinet EOS and experimental data available in literature. The resultant data show good agreement with experimental data and other EOSs.

Indian Journal of Advanced PhysicsVol. 4(2)
Openalex Percentile: Top 39%
nanoparticles nucleation surface interactions
0.38
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