Matches in SemOpenAlex for { <https://semopenalex.org/work/W1994977932> ?p ?o ?g. }
- W1994977932 endingPage "105" @default.
- W1994977932 startingPage "95" @default.
- W1994977932 abstract "Nonlinear free vibration analysis of curved double-walled carbon nanotubes (DWNTs) embedded in an elastic medium is studied in this study. Nonlinearities considered are due to large deflection of carbon nanotubes (geometric nonlinearity) and nonlinear interlayer van der Waals forces between inner and outer tubes. The differential quadrature method (DQM) is utilized to discretize the partial differential equations of motion in spatial domain, which resulted in a nonlinear set of algebraic equations of motion. The effect of nonlinearities, different end conditions, initial curvature, and stiffness of the surrounding elastic medium, and vibrational modes on the nonlinear free vibration of DWCNTs is studied. Results show that it is possible to detect different vibration modes occurring at a single vibration frequency when CNTs vibrate in the out-of-phase vibration mode. Moreover, it is observed that boundary conditions have significant effect on the nonlinear natural frequencies of the DWCNT including multiple solutions." @default.
- W1994977932 created "2016-06-24" @default.
- W1994977932 creator A5004732985 @default.
- W1994977932 creator A5024847591 @default.
- W1994977932 date "2014-11-01" @default.
- W1994977932 modified "2023-10-14" @default.
- W1994977932 title "Nonlinear free vibrations of curved double walled carbon nanotubes using differential quadrature method" @default.
- W1994977932 cites W1966286680 @default.
- W1994977932 cites W1968167977 @default.
- W1994977932 cites W1977423049 @default.
- W1994977932 cites W1979168707 @default.
- W1994977932 cites W1984690065 @default.
- W1994977932 cites W1988772146 @default.
- W1994977932 cites W1996600746 @default.
- W1994977932 cites W1997524944 @default.
- W1994977932 cites W1998015748 @default.
- W1994977932 cites W1999899167 @default.
- W1994977932 cites W2015939267 @default.
- W1994977932 cites W2018479136 @default.
- W1994977932 cites W2018858346 @default.
- W1994977932 cites W2028843445 @default.
- W1994977932 cites W2031272029 @default.
- W1994977932 cites W2040275887 @default.
- W1994977932 cites W2042212373 @default.
- W1994977932 cites W2045270332 @default.
- W1994977932 cites W2050660530 @default.
- W1994977932 cites W2050687049 @default.
- W1994977932 cites W2062854755 @default.
- W1994977932 cites W2063580670 @default.
- W1994977932 cites W2072087150 @default.
- W1994977932 cites W2072235684 @default.
- W1994977932 cites W2077138637 @default.
- W1994977932 cites W2080261365 @default.
- W1994977932 cites W2080290920 @default.
- W1994977932 cites W2082036529 @default.
- W1994977932 cites W2084316166 @default.
- W1994977932 cites W2084818100 @default.
- W1994977932 cites W2085049030 @default.
- W1994977932 cites W2091858626 @default.
- W1994977932 cites W2094963548 @default.
- W1994977932 cites W2098523098 @default.
- W1994977932 cites W2158812288 @default.
- W1994977932 cites W340223933 @default.
- W1994977932 cites W4237347820 @default.
- W1994977932 doi "https://doi.org/10.1016/j.physe.2014.07.010" @default.
- W1994977932 hasPublicationYear "2014" @default.
- W1994977932 type Work @default.
- W1994977932 sameAs 1994977932 @default.
- W1994977932 citedByCount "24" @default.
- W1994977932 countsByYear W19949779322015 @default.
- W1994977932 countsByYear W19949779322016 @default.
- W1994977932 countsByYear W19949779322018 @default.
- W1994977932 countsByYear W19949779322019 @default.
- W1994977932 countsByYear W19949779322020 @default.
- W1994977932 countsByYear W19949779322021 @default.
- W1994977932 countsByYear W19949779322022 @default.
- W1994977932 countsByYear W19949779322023 @default.
- W1994977932 crossrefType "journal-article" @default.
- W1994977932 hasAuthorship W1994977932A5004732985 @default.
- W1994977932 hasAuthorship W1994977932A5024847591 @default.
- W1994977932 hasConcept C120665830 @default.
- W1994977932 hasConcept C121332964 @default.
- W1994977932 hasConcept C134306372 @default.
- W1994977932 hasConcept C158622935 @default.
- W1994977932 hasConcept C159985019 @default.
- W1994977932 hasConcept C182310444 @default.
- W1994977932 hasConcept C192562407 @default.
- W1994977932 hasConcept C195065555 @default.
- W1994977932 hasConcept C198394728 @default.
- W1994977932 hasConcept C24890656 @default.
- W1994977932 hasConcept C2524010 @default.
- W1994977932 hasConcept C2781355719 @default.
- W1994977932 hasConcept C32758168 @default.
- W1994977932 hasConcept C33923547 @default.
- W1994977932 hasConcept C48265008 @default.
- W1994977932 hasConcept C513720949 @default.
- W1994977932 hasConcept C57879066 @default.
- W1994977932 hasConcept C62520636 @default.
- W1994977932 hasConcept C62869609 @default.
- W1994977932 hasConcept C73000952 @default.
- W1994977932 hasConcept C74650414 @default.
- W1994977932 hasConcept C78736273 @default.
- W1994977932 hasConceptScore W1994977932C120665830 @default.
- W1994977932 hasConceptScore W1994977932C121332964 @default.
- W1994977932 hasConceptScore W1994977932C134306372 @default.
- W1994977932 hasConceptScore W1994977932C158622935 @default.
- W1994977932 hasConceptScore W1994977932C159985019 @default.
- W1994977932 hasConceptScore W1994977932C182310444 @default.
- W1994977932 hasConceptScore W1994977932C192562407 @default.
- W1994977932 hasConceptScore W1994977932C195065555 @default.
- W1994977932 hasConceptScore W1994977932C198394728 @default.
- W1994977932 hasConceptScore W1994977932C24890656 @default.
- W1994977932 hasConceptScore W1994977932C2524010 @default.
- W1994977932 hasConceptScore W1994977932C2781355719 @default.
- W1994977932 hasConceptScore W1994977932C32758168 @default.
- W1994977932 hasConceptScore W1994977932C33923547 @default.
- W1994977932 hasConceptScore W1994977932C48265008 @default.
- W1994977932 hasConceptScore W1994977932C513720949 @default.