Matches in SemOpenAlex for { <https://semopenalex.org/work/W76650907> ?p ?o ?g. }
- W76650907 abstract "The small wavelength elastic vibration often termed as ultrasonic are of widespread use today. It found wide implementation in non-destructive testing, geometric measurements, vibroageing processes. The ultrasonic measurements have won the strong position providing the reasonable amounts of information at comparatively low price in comparison with other alternative methods. By virtue, the ultrasonic measurements in solids and composite bodies of complicated geometrical shape often require to develop the case oriented equipment and image processing software basing upon the knowledge of the physical essence of the wave propagation in the environment under investigation. As powerful tools for modeling of the ultrasonic measurement process the finite element method (FEM) and/or boundary integral equation method (BIEM) can be used. The modeling of the ultrasonic wave propagation can be considered as the general small displacement transient structural dynamic problem the solution techniques of which has been perfectly described in the early 1980s by numerous researchers and implemented today in practically all the FEM software available on the market. However, the practical application of FEM or BIEM is not always easy and efficient. As a rule, FEM requires highly refined meshes for proper representation of the strain and displacement field taking place in a body the dimensions of which are of considerably larger size than the length of the elastic wave propagating in a body. In this way even simple academic problems often require huge amounts of computational resource and for many practical applications the real price of finite element modeling is prohibitive. BIEM does not have such restrictions on element meshes but the computational time required is huge. This work deals with the FEM approach by developing the mass matrix modification method already introduced in [5] trying to find ways for efficient numerical simulation of the above mentioned problems in 2D case. The efficiency of the method is understood as its speed and accuracy by using moderate computational resources. Solid body is considered as a body the material properties of which (Young’s modulus, density, Poison’s ratio) are close to metals. The wavelength of interest is defined basing on the ratio of the wavelength to dimensions of the body and might vary from the length comparable to the size of the body to the wavelength making only 1/1000 part of the body size. Investigation" @default.
- W76650907 created "2016-06-24" @default.
- W76650907 creator A5017984689 @default.
- W76650907 creator A5031113840 @default.
- W76650907 date "1998-01-01" @default.
- W76650907 modified "2023-09-24" @default.
- W76650907 title "Modelling techniques for ultrasonic wave propagation in solids: 2D case" @default.
- W76650907 cites W2048574034 @default.
- W76650907 cites W2062156211 @default.
- W76650907 hasPublicationYear "1998" @default.
- W76650907 type Work @default.
- W76650907 sameAs 76650907 @default.
- W76650907 citedByCount "2" @default.
- W76650907 crossrefType "journal-article" @default.
- W76650907 hasAuthorship W76650907A5017984689 @default.
- W76650907 hasAuthorship W76650907A5031113840 @default.
- W76650907 hasConcept C10138342 @default.
- W76650907 hasConcept C107551265 @default.
- W76650907 hasConcept C111919701 @default.
- W76650907 hasConcept C120665830 @default.
- W76650907 hasConcept C121332964 @default.
- W76650907 hasConcept C127413603 @default.
- W76650907 hasConcept C134306372 @default.
- W76650907 hasConcept C135628077 @default.
- W76650907 hasConcept C15744967 @default.
- W76650907 hasConcept C162324750 @default.
- W76650907 hasConcept C17744445 @default.
- W76650907 hasConcept C182310444 @default.
- W76650907 hasConcept C198082294 @default.
- W76650907 hasConcept C199360897 @default.
- W76650907 hasConcept C199539241 @default.
- W76650907 hasConcept C202444582 @default.
- W76650907 hasConcept C24890656 @default.
- W76650907 hasConcept C2776359362 @default.
- W76650907 hasConcept C2777904410 @default.
- W76650907 hasConcept C33923547 @default.
- W76650907 hasConcept C41008148 @default.
- W76650907 hasConcept C44886760 @default.
- W76650907 hasConcept C542102704 @default.
- W76650907 hasConcept C66938386 @default.
- W76650907 hasConcept C78519656 @default.
- W76650907 hasConcept C81288441 @default.
- W76650907 hasConcept C94625758 @default.
- W76650907 hasConcept C9652623 @default.
- W76650907 hasConcept C98045186 @default.
- W76650907 hasConceptScore W76650907C10138342 @default.
- W76650907 hasConceptScore W76650907C107551265 @default.
- W76650907 hasConceptScore W76650907C111919701 @default.
- W76650907 hasConceptScore W76650907C120665830 @default.
- W76650907 hasConceptScore W76650907C121332964 @default.
- W76650907 hasConceptScore W76650907C127413603 @default.
- W76650907 hasConceptScore W76650907C134306372 @default.
- W76650907 hasConceptScore W76650907C135628077 @default.
- W76650907 hasConceptScore W76650907C15744967 @default.
- W76650907 hasConceptScore W76650907C162324750 @default.
- W76650907 hasConceptScore W76650907C17744445 @default.
- W76650907 hasConceptScore W76650907C182310444 @default.
- W76650907 hasConceptScore W76650907C198082294 @default.
- W76650907 hasConceptScore W76650907C199360897 @default.
- W76650907 hasConceptScore W76650907C199539241 @default.
- W76650907 hasConceptScore W76650907C202444582 @default.
- W76650907 hasConceptScore W76650907C24890656 @default.
- W76650907 hasConceptScore W76650907C2776359362 @default.
- W76650907 hasConceptScore W76650907C2777904410 @default.
- W76650907 hasConceptScore W76650907C33923547 @default.
- W76650907 hasConceptScore W76650907C41008148 @default.
- W76650907 hasConceptScore W76650907C44886760 @default.
- W76650907 hasConceptScore W76650907C542102704 @default.
- W76650907 hasConceptScore W76650907C66938386 @default.
- W76650907 hasConceptScore W76650907C78519656 @default.
- W76650907 hasConceptScore W76650907C81288441 @default.
- W76650907 hasConceptScore W76650907C94625758 @default.
- W76650907 hasConceptScore W76650907C9652623 @default.
- W76650907 hasConceptScore W76650907C98045186 @default.
- W76650907 hasLocation W766509071 @default.
- W76650907 hasOpenAccess W76650907 @default.
- W76650907 hasPrimaryLocation W766509071 @default.
- W76650907 hasRelatedWork W1480956510 @default.
- W76650907 hasRelatedWork W1484382378 @default.
- W76650907 hasRelatedWork W160679457 @default.
- W76650907 hasRelatedWork W1608006674 @default.
- W76650907 hasRelatedWork W1621261933 @default.
- W76650907 hasRelatedWork W1631802412 @default.
- W76650907 hasRelatedWork W1648837387 @default.
- W76650907 hasRelatedWork W1658814312 @default.
- W76650907 hasRelatedWork W1666207584 @default.
- W76650907 hasRelatedWork W1990448585 @default.
- W76650907 hasRelatedWork W1998079649 @default.
- W76650907 hasRelatedWork W2015027389 @default.
- W76650907 hasRelatedWork W2032957838 @default.
- W76650907 hasRelatedWork W2093256704 @default.
- W76650907 hasRelatedWork W2093819315 @default.
- W76650907 hasRelatedWork W2112397170 @default.
- W76650907 hasRelatedWork W2121276258 @default.
- W76650907 hasRelatedWork W2355258976 @default.
- W76650907 hasRelatedWork W2364803911 @default.
- W76650907 hasRelatedWork W288757733 @default.
- W76650907 isParatext "false" @default.
- W76650907 isRetracted "false" @default.
- W76650907 magId "76650907" @default.