Vesselin Shanov

Dr. Vesselin Shanov

orcid

Research Focus & Metrics

Academic Career Length

22Years (2005-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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5 January 2017 in Small
Verified
Journal Article
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LZLu Zhang
Lu Zhang
DDDerek DeArmond
Derek DeArmond
NANoe T. Alvarez
Noe T. Alvarez
RMRachit Malik
Rachit Malik
NONicholas Oslin
Nicholas Oslin
VSVesselin Shanov
Vesselin Shanov

1 October 2008 in Composites Science and Technology
Verified
Journal Article
Closed access
Jandro AbotJandro Abot
Jandro Abot
YSYi Song
Yi Song
MSM.J. Schulz
M.J. Schulz
VSVesselin Shanov
Vesselin Shanov

28 February 2011 in Journal of Materials Research
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Journal Article
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CJChaminda Jayasinghe
Chaminda Jayasinghe
Supriya ChakrabartiSupriya Chakrabarti
Supriya Chakrabarti
MSMark J. Schulz
Mark J. Schulz
VSVesselin Shanov
Vesselin Shanov

27 March 2019 in Nanoscale
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Journal Article
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YHYu-Yun Hsieh
Yu-Yun Hsieh
YZYu Zhang
Yu Zhang
LZLu Zhang
Lu Zhang
YFYanbo Fang
Yanbo Fang
SKSathya Narayan Kanakaraj
Sathya Narayan Kanakaraj
VSVesselin Shanov
Vesselin Shanov
Hybrid thermoelectric (TE) nanocomposites containing conducting polymers and nanocarbon materials have been extensively studied in recent years due to their unique advantages over single-phase organic/inorganic TE materials. Nanocarbon materials have been developed as conductive nanofillers to improve the electrical conductivity of the polymer matrix, and to create a strong π–π interfacial interaction with the matrix to enhance the TE performance. However, previous designs of the hybrid TE nanocomposites tend to cause aggregation of nanocarbon materials, which is detrimental to the TE performance. Also, they are limited in their fabrication to thin film technologies with submicron thicknesses, which prevents these composites from being used in practical TE devices. Herein, we present the synthesis and thermoelectric properties of free-standing, three-dimensional graphene (3DG)–polyaniline (PANI) composites with greater than 100 μm thicknesses for high performance flexible p-type thermoelectrics. Our 3DG matrix has been synthesized by Chemical Vapor Deposition (CVD) with particulate nickel catalysts, and used as a scaffold for the polymer composites. This material provides an excellent electrical conductivity and a reasonable Seebeck coefficient along with very good mechanical integrity preserved when bending, thus making it a promising candidate for flexible TE. PANI polymer was electrochemically grown on the 3DG scaffold as a filler to further tune the TE properties. The proposed 3DG–PANI composites showed a maximum power factor of 81.9 μW m−1 K−2 with a PANI loading of 80 wt% and highly reproducible TE performance after repeated mechanical bending tests. This novel material provides a different strategy for simple and scalable fabrication of flexible thermoelectrics with high performance TE energy harvesting and improved mechanical properties.

22 December 2015 in Journal of Materials Chemistry A
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Journal Article
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LZLu Zhang
Lu Zhang
DDDerek DeArmond
Derek DeArmond
NANoe T. Alvarez
Noe T. Alvarez
DZDaoli Zhao
Daoli Zhao
TWTingting Wang
Tingting Wang
VSVesselin Shanov
Vesselin Shanov
Graphene foam (GF) is a three-dimensional (3D) graphene structure that has been intensively studied as an electrode material for energy storage applications. The porous structure and seamlessly connected graphene flakes make GF a promising electrode material for supercapacitors and batteries. However, the electrical conductivity of GF is still unsatisfactory due to the lack of macropore size (∼300 μm) control that hinders its applications. Previously we reported a new seamless 3D graphene structure – graphene pellets (GPs) – with well-controlled mesopore size (∼2 nm), high electrical conductivity (148 S cm−1) and good electromechanical properties that differ substantially from the known GF. Here we demonstrate that the obtained 3D graphene structure is an ideal scaffold electrode for pseudocapacitive materials and redox additive electrolyte systems. For example, after electrochemical coating with MnO2, the GP/MnO2 electrode showed specific and volumetric capacitance up to 395 F g−1 and 230 F cm−3 at 1 A g−1, respectively. When combined with a hydroquinone and benzoquinone redox additive electrolyte, the GPs showed a specific capacitance of 7813 F g−1 at 10 A g−1. Moreover, when the GP/MnO2 electrode was assembled with a GP/polypyrrole electrode, the obtained full cell showed good electrochemical performance with a maximum energy density of 26.7 W h kg−1 and a maximum power density of 32.7 kW kg−1, and a reasonable cycle life for practical application. The ease in material processing combined with the excellent electrical and electromechanical properties makes GPs promising for a variety of energy storage applications.

1 November 2018 in Carbon
Verified
Journal Article
Closed access
YHYu-Yun Hsieh
Yu-Yun Hsieh
LZLu Zhang
Lu Zhang
DDDerek DeArmond
Derek DeArmond
SKSathya Narayan Kanakaraj
Sathya Narayan Kanakaraj
PAPaa Kwasi Adusei
Paa Kwasi Adusei
VSVesselin Shanov
Vesselin Shanov