39 Works

Ni36.67Co30Fe16.67Ti16.67 0% strain (initial surface)

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of bi-axial compression of a single crystal Ni36.67Co30Fe16.67Ti16.67 solid solution. The initial configuration was a Ni36.67Co30Fe16.67Ti16.67 cube with side length 100 nm. The x- and y-directions of the simulation cell were parallel to the [-34-1] and [-5-27] directions of the crystal, respectively. The z-direction was parallel to the [111] crystal direction. The x- and y-directions were periodic, but the z-direction was free, hence the crystal...

CuZr biaxial compression 10% engineering strain

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of bi-axial compression of a CuZr (50% Cu, 50% Zr) metallic glass. The initial configuration was a CuZr cube with side length 100 nm. The glass had been produced by quenching from the melt at a rate of 1e11 K/s under fully periodic boundary conditions. In the compression simulation, the x- and y-directions were periodic, but the z-direction was free, hence the glass had free...

CuZr biaxial compression 30% engineering strain

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of bi-axial compression of a CuZr (50% Cu, 50% Zr) metallic glass. The initial configuration was a CuZr cube with side length 100 nm. The glass had been produced by quenching from the melt at a rate of 1e11 K/s under fully periodic boundary conditions. In the compression simulation, the x- and y-directions were periodic, but the z-direction was free, hence the glass had free...

CuZr biaxial compression 0% strain (initial surface)

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of bi-axial compression of a CuZr (50% Cu, 50% Zr) metallic glass. The initial configuration was a CuZr cube with side length 100 nm. The glass had been produced by quenching from the melt at a rate of 1e11 K/s under fully periodic boundary conditions. In the compression simulation, the x- and y-directions were periodic, but the z-direction was free, hence the glass had free...

Au uniaxial compression in x-direction 20 % engineering strain

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of uni-axial compression of single crystal Au. The initial configuration was an Au cube with side length 100 nm. The x- and y-directions of the simulation cell were parallel to the [-110] and [-1-12] directions of the crystal, respectively. The z-direction was parallel to the [111] crystal direction. The x- and y-directions were periodic, but the z-direction was free, hence the crystal had free surfaces...

Ni36.67Co30Fe16.67Ti16.67 30% engineering strain

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of bi-axial compression of a single crystal Ni36.67Co30Fe16.67Ti16.67 solid solution. The initial configuration was a Ni36.67Co30Fe16.67Ti16.67 cube with side length 100 nm. The x- and y-directions of the simulation cell were parallel to the [-34-1] and [-5-27] directions of the crystal, respectively. The z-direction was parallel to the [111] crystal direction. The x- and y-directions were periodic, but the z-direction was free, hence the crystal...

Ultrananocrystalline Diamond TEM cross-section

Subarna R. Khanal, Abhijeet Gujrati, Sai Bharadwaj Vishnubhotla, Pawel Nowakowski, Cecile S. Bonifacio, Lars Pastewka & Tevis D. B. Jacobs
Cross-section UNCD surfaces for TEM from publication: S. R. Khanal, A. Gujrati, S. B. Vishnubhotla, P. Nowakowski, C. S. Bonifacio, L. Pastewka, T. D. B. Jacobs, "Characterization of small-scale surface topography using transmission electron microscopy", Surf. Topogr.: Metrol. Prop. 6 045004 (2018) See publication for details.

Ultrananocrystalline diamond (UNCD)

Abhijeet Gujrati, Subarna R. Khanal, Lars Pastewka & Tevis D. B. Jacobs
UNCD surface from A. Gujrati, S.R. Khanal, L. Pastewka, T.D.B. Jacobs, "Combining TEM, AFM, and profilometry for quantitative topography characterization across all scales", ACS Appl. Mater. Interfaces 10(34), 29169-29178 (2018)

Rough sphere

Antoine Sanner & Lars Pastewka
Example illustrating the contact of a rough sphere that behaves as a nominally flat rough surface at small normal forces while it follows the Hertzian theory of smooth spheres at large normal forces. This dataset is similar to the simulations in https://doi.org/10.1063/1.4950802 The topographies were generated with the following Python code: ``` from SurfaceTopography.Generation import fourier_synthesis from SurfaceTopography.Special import make_sphere import numpy as np a0 = 1 # Pixel size radius = 10000 n =...

Au biaxial compression 0% strain (initial surface)

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of bi-axial compression of single crystal Au. The initial configuration was an Au cube with side length 100 nm. The x- and y-directions of the simulation cell were parallel to the [-110] and [-1-12] directions of the crystal, respectively. The z-direction was parallel to the [111] crystal direction. The x- and y-directions were periodic, but the z-direction was free, hence the crystal had free surfaces...

Self-affine synthetic surface

Tevis D. B. Jacobs, Till Junge & Lars Pastewka
This surface contains virtual measurements taken out of a large self-affine synthetic surface with Hurst exponent 0.8. The original surface had 50,000 x 50,000 data points and was created using a Fourier filtering algorithm. The surface was "measured" in block containing 500 x 500 data points with a variety of scan sizes ranging from almost the full surface with 100 μm width to 10 μm to 1 μm, with pixel sizes scaling accordingly. This surface...

Neural Implant, Nanoparticle-coated, Top Surface, SEM Cross-section

Nathaniel Miller
Associated publication: Ruikang Ding, Nathaniel C. Miller, Kevin M. Woeppel, Xinyan T. Cui, Tevis D. B. Jacobs “Surface area and local curvature: Why roughness improves the bioactivity of neural implants” Langmuir 2022 “Accepted” Material: Nanoparticle-coated neural implant; Make and model: A1×16-3 mm-100-703, NeuroNexus, Ann Arbor, MI, USA. Subsequently coated with thiolated silica nanoparticles; Surface: Top cross-sectioned by focused ion beam; For more details: See Associated Publication.

Uncoated Bottom Surface of a Brain Implant Probe

Ruikang Ding, Nathaniel C. Miller, Kevin M. Woeppel, Xinyan T. Cui & Tevis D. B. Jacobs
Associated publication: Ding, R.; Miller, N. C.; Woeppel K. M.; Cui X. T.; Jacobs T. D. B. Surface area and local curvature: Why roughness improves the bioactivity of neural implants. Langmuir 2022, Accepted. Material: Neural Implant, Uncoated, Bottom Surface Make and model: A1×16-3 mm-100-703, NeuroNexus, Ann Arbor, MI, USA. Subsequently modified by mercaptopropyl trimethoxysilane; For more details: See Associated Publication.

Nanoparticle-Coated Top Surface of a Brain Implant Probe

Ruikang Ding, Nathaniel C. Miller, Kevin M. Woeppel, Xinyan T. Cui & Tevis D. B. Jacobs
Associated publication: Ding, R.; Miller, N. C.; Woeppel K. M.; Cui X. T.; Jacobs T. D. B. Surface area and local curvature: Why roughness improves the bioactivity of neural implants. Langmuir 2022, Accepted. Material: Neural Implant, Nanoparticle-coated, Top Surface; Make and model: A1×16-3 mm-100-703, NeuroNexus, Ann Arbor, MI, USA. Subsequently coated with thiolated silica nanoparticles; For more details: See Associated Publication.

Unpolished UNCD (measured with 10.11 nm AFM tip)

Antoine Sanner, Wolfram G. Nöhring, Luke A. Thimons, Tevis D. B. Jacobs & Lars Pastewka
Substrate material – Unpolished Ultrananocrystalline Diamond. Substrate Manufacturer – Advanced Diamond Technologies Inc.

Synthetic self-affine topography scanned with a virtual spherical probe

Tevis D. B. Jacobs, Till Junge & Lars Pastewka
This surface contains a self-affine topography that has been scanned with a spherical virtual probe of radius 40 nm. The probe was lowered normal to the surface on each point of the reference topography (that is also included here) and the center of the probe was taken as the "measured" value of the topography. The reference topography has a Hurst exponent of 0.8 and was generated with a Fourier-filtering algorithm. This surface was used to...

Au uniaxial compression in x-direction 10 % engineering strain

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of uni-axial compression of single crystal Au. The initial configuration was an Au cube with side length 100 nm. The x- and y-directions of the simulation cell were parallel to the [-110] and [-1-12] directions of the crystal, respectively. The z-direction was parallel to the [111] crystal direction. The x- and y-directions were periodic, but the z-direction was free, hence the crystal had free surfaces...

Unpolished ultrananocrystalline diamond

Luke A. Thimons, Abhijeet Gujrati, Antoine Sanner, Lars Pastewka & Tevis D. B. Jacobs
unpolished UNCD film on silicon wafer Substrate Manufacturer : Advanced Diamond Technologies, Inc.

Unpolished ultrananocrystalline diamond

Luke A. Thimons, Abhijeet Gujrati, Antoine Sanner, Lars Pastewka & Tevis D. B. Jacobs
unpolished UNCD film on silicon wafer Substrate Manufacturer : Advanced Diamond Technologies, Inc.

Microcrystalline Diamond

Abhijeet Gujrati, Subarna R. Khanal, Lars Pastewka & Tevis D. B. Jacobs
MCD surface topography measured using TEM, AFM, and Stylus Profilometry

Ceramic Floor Tile

Ruikang Ding, Abhijeet Gujrati, Matthew M. Pendolino, Kurt E. Beschorner & Tevis D. B. Jacobs
These are surface profiles of ceramic flooring. The ceramic tile (ADJF250803, ASTM) was a reference tile that was used in the reference standard ASTM F2508-12a. There are 30 profiles generated from image analysis and measured by SEM. 10 profiles are from 250X magnification, 10 profiles are from 5000X magnification, and 10 profiles are from 100kX magnification. There are also 6 profiles measured by stylus profilometry.

Quarry 1 Floor Tile

Ruikang Ding, Abhijeet Gujrati, Matthew M. Pendolino, Kurt E. Beschorner & Tevis D. B. Jacobs
These are surface profiles of quarry 1 smooth flooring. The quarry 1 (0T01881P, Daltile, Dallas, TX, USA) and quarry 2 (01 010 SM 1, Summitville, OH, USA) were commercial tiles, where the full composition was a trade secret, but they were known to include 15-25 wt% quartz, and quarry 2 also included abrasive grits on the surface, presumably to improve slip resistance. There are 30 profiles generated from image analysis and measured by SEM. 10...

Au biaxial compression 30% engineering strain

Wolfram G. Nöhring, Adam R. Hinkle & Lars Pastewka
This surface is the result of a Molecular Dynamics simulation of bi-axial compression of single crystal Au. The initial configuration was an Au cube with side length 100 nm. The x- and y-directions of the simulation cell were parallel to the [-110] and [-1-12] directions of the crystal, respectively. The z-direction was parallel to the [111] crystal direction. The x- and y-directions were periodic, but the z-direction was free, hence the crystal had free surfaces...

Polished ultrananocrystalline diamond

Luke A. Thimons, Abhijeet Gujrati, Antoine Sanner, Lars Pastewka & Tevis D. B. Jacobs
polished UNCD on silicon wafer Substrate Manufacturer : Advanced Diamond Technologies, Inc.

Spherical Ruby tip (500 micron)

Luke A. Thimons, Abhijeet Gujrati, Antoine Sanner, Lars Pastewka & Tevis D. B. Jacobs
polished ruby tips used in adhesion testing material: Ruby manufacturer: Swissjewel

Registration Year

  • 2022
    39

Resource Types

  • Dataset
    39

Affiliations

  • Cluster of Excellence livMatS, Freiburg Center for Interactive Materials and Bioinspired Technologies, University of Freiburg, Georges-Köhler-Allee 105, 79110 Freiburg, Germany
    30
  • Department of Microsystems Engineering, University of Freiburg, Georges-Köhler-Allee 103, 79110 Freiburg, Germany
    30
  • Department of Mechanical Engineering and Materials Science, University of Pittsburgh, Pittsburgh, PA 15261, USA
    18
  • Material, Physical and Chemical Sciences Center, Sandia National Laboratories, Albuquerque, NM 87123, USA
    14
  • Institute for Applied Materials, Karlsruhe Institute of Technology, 76131 Karlsruhe, Germany
    14
  • Department of Bioengineering, University of Pittsburgh, Pittsburgh, PA 15261, USA
    3
  • Department of Mechanical Engineering, École Polytechnique Fédérale de Lausanne, 1015 Lausanne, Switzerland
    2
  • Department of Mechanical Engineering and Materials Science, University of Pittsburgh, Pittsburgh, Pennsylvania 15261, United States
    1
  • Mechanical Engineering and Materials Science, University of Pittsburgh, Pittsburgh, Pennsylvania 15261, United States
    1
  • Department of Microsystems Engineering, University of Freiburg, 79110 Freiburg, Germany
    1