Sidnei Paciornik

Prof. Dr. Sidnei Paciornik

Department of Chemical and Materials Engineering, Pontifical Catholic University of Rio de Janeiro (PUC-Rio), Rio de Janeiro 22451-900, Brazil
orcid

Research Focus & Metrics

Academic Career Length

41Years (1986-Present)

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

Representative Publications

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1 November 2008 in Journal of Endodontics
Verified
Journal Article
Closed access
GDGustavo De-Deus
Gustavo De-Deus
CRClaudia Reis
Claudia Reis
DBDenise Beznos
Denise Beznos
AAAlice Maria Gruetzmacher de Abranches
Alice Maria Gruetzmacher de Abranches
TCTauby Coutinho-Filho
Tauby Coutinho-Filho
Sidnei PaciornikSidnei Paciornik
Sidnei Paciornik

2 March 2006 in International Endodontic Journal
Verified
Journal Article
Closed access
PDF file
GDG. De‐Deus
G. De‐Deus
Sidnei PaciornikSidnei Paciornik
Sidnei Paciornik
MMM. H. P. Mauricio
M. H. P. Mauricio

1 December 2015 in Brazilian Dental Journal
Verified
Journal Article
Open access
PDF file
GDGustavo De-Deus
Gustavo De-Deus
FBFelipe G. Belladonna
Felipe G. Belladonna
ESEmmanuel Silva
Emmanuel Silva
JMJuliana Roter Marins
Juliana Roter Marins
ESErick Miranda Souza
Erick Miranda Souza
ANAline de Almeida Neves
Aline de Almeida Neves
The aim of this study was to compare the percentage of non-instrumented area of root canals prepared with different enlargements using single-file reciprocating systems (Reciproc and WaveOne) and a conventional multi-file rotary (BioRaCe) system by micro-computed tomographic analysis. Thirty mesial roots of mandibular molars with moderate curvature (10° to 20°) presenting a type II Vertucci canal configuration and similar internal volume were chosen and scanned at an isotropic resolution of 14.16 µm. The sample was assigned to 3 groups (n=10) according to the system used for root canal preparation: Reciproc, WaveOne, and BioRaCe groups. Second and third scans were taken after the canals were prepared with instruments sizes 25 and 40, respectively. The recorded images of the surface area voxels of the canals, before and after preparation were examined from the furcation level to the apex to quantify the non-instrumented surface. Statistical data were compared using GLM for repeated-measures with a significance level set at 5%. Instrumentation systems did not influence the percentage of untouched root canal surfaces (p=0.690) whilst a significant reduction in the percentage of static voxels was observed after the enlargement of the root canal (p=0.010) in all groups (p=0.507). None of the systems was able to prepare the entire surface area of the mesial root canal of mandibular molars. The increased final apical size resulted in a significant positive effect on the shaping ability of the tested systems.

1 January 2008 in Journal of Endodontics
Verified
Journal Article
Closed access
GDGustavo De-Deus
Gustavo De-Deus
MZMatthias Zehnder
Matthias Zehnder
CRClaudia Reis
Claudia Reis
SFSandra Fidel
Sandra Fidel
RFRivail Antonio Sergio Fidel
Rivail Antonio Sergio Fidel
Sidnei PaciornikSidnei Paciornik
Sidnei Paciornik

1 October 2011 in Oral Surgery Oral Medicine Oral Pathology Oral Radiology and Endodontology
Verified
Journal Article
Closed access
GDGustavo De-Deus
Gustavo De-Deus
CRClaudia Reis
Claudia Reis
Sidnei PaciornikSidnei Paciornik
Sidnei Paciornik

20 January 1997 in Physical Review Letters
Verified
Journal Article
Closed access
PDF file
UDU. Dahmen
U. Dahmen
SXSq. Xiao
Sq. Xiao
Sidnei PaciornikSidnei Paciornik
Sidnei Paciornik
EJE. Johnson
E. Johnson
AJA. Johansen
A. Johansen
We show that the equilibrium shapes of small solid Pb inclusions embedded in an Al matrix are size dependent. Using high resolution electron microscopy we have observed that small inclusions a few nanometers in size adopt equilibrium shapes with smooth {111} facets. Inclusion dimensions follow preferred sizes shown to result from the nature of the residual strain which oscillates and decreases with size. As a result, the inclusion shape is controlled by the residual strain energy at small sizes and by the interface energy at larger sizes.