Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Normal Strain under Axial Loading01:20

Normal Strain under Axial Loading

911
Normal strain under axial loading is an important concept in the field of mechanics of materials. Axial loading implies the application of a force along the axis of a material, like a column or bar. This force can either compress or stretch the material. In the context of axial loading, normal strain is the deformation experienced by the material in the direction of the loading force. It's calculated as the change in length divided by the original length of the material. This unitless ratio...
911
Temperature Dependent Deformation01:12

Temperature Dependent Deformation

277
In a nonhomogeneous rod made up of steel and brass, restrained at both ends and subjected to a temperature change, several steps are involved in calculating the stress and compressive load. Due to the problem's static indeterminacy, one end support is disconnected, allowing the rod to experience the temperature change freely. Next, an unknown force is applied at the free end, triggering deformations in the rod's steel and brass portions. These deformations are then calculated and added...
277
Stress-Strain Diagram - Ductile Materials01:24

Stress-Strain Diagram - Ductile Materials

1.4K
The stress-strain relationship in ductile materials such as structural steel or aluminium is intricate and progresses through several stages. When a specimen is loaded, it initially exhibits a linear length increase, depicted by a steep straight line on the stress-strain diagram. It indicates the material is elastically deforming and will return to its original shape once unloaded. However, when a critical stress value is reached, plastic deformation begins. This stage sees substantial...
1.4K
Stress: General Loading Conditions01:15

Stress: General Loading Conditions

451
To grasp the intricacy of real-world conditions where multiple loads are applied simultaneously to a structure, one might visualize a section passing through a specific point within a body, aligned parallel to the xy plane. This section is subjected to various forces, including original loads, normal forces, and shearing forces.
The shearing force, possessing potential directionality within the plane of the section, is simplified into two component forces running parallel to the x and y axes....
451
Impact Loading01:19

Impact Loading

469
Impact loading occurs when a moving object collides with a stationary structure, such as a rod with a uniform cross-sectional area fixed at one end. Under these conditions, the rod absorbs the kinetic energy from the striking object, leading to deformation and subsequent stress development. As the rod returns to its original position and reaches maximum stress, the absorbed energy, initially manifested as kinetic energy, transforms entirely into strain energy.
In cases of elastic deformation,...
469
Relation between Poisson's ratio, Modulus of Elasticity and Modulus of Rigidity01:15

Relation between Poisson's ratio, Modulus of Elasticity and Modulus of Rigidity

419
Deformation occurs in axial and transverse directions when an axial load is applied to a slender bar. This deformation impacts the cubic element within the bar, transforming it into either a rectangular parallelepiped or a rhombus, contingent on its orientation. This transformation process induces shearing strain. Axial loading elicits both shearing and normal strains. Applying an axial load instigates equal normal and shearing stresses on elements oriented at a 45° angle to the load axis.
419

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Molecular dynamics simulation of high slip flow of water confined between graphene nanochannels at experimentally accessible shear rates.

The Journal of chemical physics·2026
Same author

Electrically Tunable Friction through Surface Adsorption Layer Restructuring.

ACS applied materials & interfaces·2025
Same author

Equations of state and excess entropy of repulsive inverse power particle potential fluids with variable stiffness.

The Journal of chemical physics·2025
Same author

Genetic Biomarkers for Periodontal Diseases: A Systematic Review.

Journal of clinical periodontology·2025
Same author

Three-dimensional, multimodal synchrotron data for machine learning applications.

Scientific data·2025
Same author

Molecular Insights into the Adsorption of Deposit Control Additives from Hydrocarbon Fuels.

Langmuir : the ACS journal of surfaces and colloids·2025

Related Experiment Video

Updated: Nov 21, 2025

A Novel Method for In Situ Electromechanical Characterization of Nanoscale Specimens
07:15

A Novel Method for In Situ Electromechanical Characterization of Nanoscale Specimens

Published on: June 2, 2017

9.5K

Normal Load and Counter Body Size Influence the Initiation of Microstructural Discontinuities in Copper during

F Ruebeling1,2, Y Xu3,4, G Richter5

  • 1Institute for Applied Materials (IAM), Karlsruhe Institute of Technology (KIT), Kaiserstrasse 12, 76131 Karlsruhe, Germany.

ACS Applied Materials & Interfaces
|January 14, 2021
PubMed
Summary

The study reveals a dislocation trace line forms beneath sliding copper surfaces, influencing microstructure evolution. This phenomenon occurs across various loads and contact pressures, impacting tribological behavior.

Keywords:
copperelectron microscopylattice rotationmicrostructuresapphiretribology

More Related Videos

Full-field Strain Measurements for Microstructurally Small Fatigue Crack Propagation Using Digital Image Correlation Method
07:37

Full-field Strain Measurements for Microstructurally Small Fatigue Crack Propagation Using Digital Image Correlation Method

Published on: January 16, 2019

9.9K
Knowledge Based Cloud FE Simulation of Sheet Metal Forming Processes
11:05

Knowledge Based Cloud FE Simulation of Sheet Metal Forming Processes

Published on: December 13, 2016

12.5K

Related Experiment Videos

Last Updated: Nov 21, 2025

A Novel Method for In Situ Electromechanical Characterization of Nanoscale Specimens
07:15

A Novel Method for In Situ Electromechanical Characterization of Nanoscale Specimens

Published on: June 2, 2017

9.5K
Full-field Strain Measurements for Microstructurally Small Fatigue Crack Propagation Using Digital Image Correlation Method
07:37

Full-field Strain Measurements for Microstructurally Small Fatigue Crack Propagation Using Digital Image Correlation Method

Published on: January 16, 2019

9.9K
Knowledge Based Cloud FE Simulation of Sheet Metal Forming Processes
11:05

Knowledge Based Cloud FE Simulation of Sheet Metal Forming Processes

Published on: December 13, 2016

12.5K

Area of Science:

  • Materials Science
  • Tribology
  • Solid Mechanics

Background:

  • Tribological behavior is governed by microstructural changes at the interface of sliding metallic bodies.
  • The fundamental mechanisms driving these tribologically induced microstructural changes remain poorly understood.

Purpose of the Study:

  • To investigate the influence of normal load and counter body size on the initiation of tribologically induced microstructures in copper after a single sliding pass.
  • To elucidate the early stages of subsurface deformation and microstructural evolution under sliding contact.

Main Methods:

  • Systematic variation of normal load and sphere diameter to achieve contact pressures from 530 MPa to 1953 MPa.
  • Utilized Scanning Electron Microscopy (SEM), Focused Ion Beam (FIB), and Transmission Electron Microscopy (TEM) to analyze subsurface deformation.
  • Employed Transmission Kikuchi Diffraction (TKD) to assess microstructural misorientation.

Main Results:

  • A consistent dislocation trace line was identified in the subsurface region (100-400 nm depth) across all tested conditions.
  • Below 6.75 N, dislocation features formed beneath the trace line; above this load, evolution was confined between the surface and the trace line, which moved deeper.
  • Misorientation was concentrated at the dislocation trace line, indicating material rotation.

Conclusions:

  • The dislocation trace line is a general phenomenon in sliding contacts, occurring over a wide range of loads and pressures.
  • Microstructure evolution is complex and depends on load, with the dislocation trace line acting as a key feature.
  • This research provides a foundation for modeling early-stage microstructural changes in tribological contacts.