1967
DOI: 10.1007/bf02327001
|View full text |Cite
|
Sign up to set email alerts
|

On the definitions of strain and their use in large-strain analysis

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
12
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 27 publications
(12 citation statements)
references
References 1 publication
0
12
0
Order By: Relevance
“…Elastic deformation is one of the most common phenomena in materials. Experimentally, a one-dimensional elastic bar will be stretched or shortened (i.e., from the initial length L 0 to the final length L 1 ) along the axis direction when an axial tensile or compressive force is applied (Figure a). In this case, the local deformation capacity of an elastic bar can be described by the normal strain, which is simplistically defined as ( L 1 – L 0 )/ L 0 when the change of length is very small. , Although strain is one of the most difficult physical parameters to accurately evaluate, the important influence of strain on the properties from the microdomain to the macrodomain is commonly acknowledged . In particular, with reducing the size of a material to the micro/nanoscale, the strain effect will be further magnified due to the enhanced tolerance of deformation. ,, In the field of electrolysis, catalysts are generally at the nanometer scale and possess high surface energies.…”
Section: Strain Engineeringmentioning
confidence: 99%
See 1 more Smart Citation
“…Elastic deformation is one of the most common phenomena in materials. Experimentally, a one-dimensional elastic bar will be stretched or shortened (i.e., from the initial length L 0 to the final length L 1 ) along the axis direction when an axial tensile or compressive force is applied (Figure a). In this case, the local deformation capacity of an elastic bar can be described by the normal strain, which is simplistically defined as ( L 1 – L 0 )/ L 0 when the change of length is very small. , Although strain is one of the most difficult physical parameters to accurately evaluate, the important influence of strain on the properties from the microdomain to the macrodomain is commonly acknowledged . In particular, with reducing the size of a material to the micro/nanoscale, the strain effect will be further magnified due to the enhanced tolerance of deformation. ,, In the field of electrolysis, catalysts are generally at the nanometer scale and possess high surface energies.…”
Section: Strain Engineeringmentioning
confidence: 99%
“…The atomic spacing at the subsurface or surface can be either larger or smaller compared to that in the bulk state, that is, the generation of tensile or compressive strain in the lattice, respectively (Figure b). Similar to the calculation method for the elastic bar we mentioned earlier, the lattice strain can be determined by the following formula associated with the lattice spacing: , ε = false( ( d strained d bulk ) / italicd normalbulk false) × 100 % where d strained and d bulk represent the lattice spacings in the strained and bulk states, respectively. Essentially, the lattice strain originates from the discrepancy in lattice parameters.…”
Section: Strain Engineeringmentioning
confidence: 99%
“…As another consequence of introducing secondary metals, surface strain in Pt‐based electrocatalysts arises because surface Pt atoms have lower coordination numbers or more dangling bonds than the inner atoms, causing lattice changes to minimize the surface energies . We can define the strain in Pt‐based electrocatalysts, namely s catalyst , simply as the distorted percentage of the Pt lattice between its original and final states . It is calculated as follows by Equation …”
Section: Theoretical Mechanisms Of Tuning Catalytic Propertiesmentioning
confidence: 99%
“…[69,39,40] Such a strain can be defined in several forms, which corresponds to a particular circumstance. [70] In the case of small strains, for example, the definition of the strain along a line is (l f − l i )/l i , where l f and l i refer to the atomic bond length in the final state and the initial state, respectively. However, the accurate evaluation of atomic bond length remains a challenge.…”
Section: Strainmentioning
confidence: 99%