Ingo Alig

Dr. Ingo Alig

orcid

Research Focus & Metrics

Academic Career Length

34Years (1993-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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14 June 2022 in Polymers
Verified
Journal Article
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MTMaximilian Thuy
Maximilian Thuy
Miquel Pedragosa RincónMiquel Pedragosa Rincón
Miquel Pedragosa Rincón
UNUte Niebergall
Ute Niebergall
HOHarald Oehler
Harald Oehler
IAIngo Alig
Ingo Alig
MBMartin Böhning
Martin Böhning
The crack propagation rate of environmental stress cracking was studied on high-density polyethylene compact tension specimens under static loading. Selected environmental liquids are distilled water, 2 wt% aqueous Arkopal N100 solution, and two model liquid mixtures, one based on solvents and one on detergents, representing stress cracking test liquids for commercial crop protection products. The different surface tensions and solubilities, which affect the energetic facilitation of void nucleation and craze development, are studied. Crack growth in surface-active media is strongly accelerated as the solvents induce plasticization, followed by strong blunting significantly retarding both crack initiation and crack propagation. The crack propagation rate for static load as a function of the stress intensity factor within all environments is found to follow the Paris–Erdogan law. Scanning electron micrographs of the fracture surface highlight more pronounced structures with both extensive degrees of plasticization and reduced crack propagation rate, addressing the distinct creep behavior of fibrils. Additionally, the limitations of linear elastic fracture mechanisms for visco-elastic polymers exposed to environmental liquids are discussed.

18 May 2017 in Materials
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MMMichael Thomas Müller
Michael Thomas Müller
KHKonrad Hilarius
Konrad Hilarius
Marco LiebscherMarco Liebscher
Marco Liebscher
DLDirk Lellinger
Dirk Lellinger
IAIngo Alig
Ingo Alig
Petra PötschkePetra Pötschke
Petra Pötschke
The influence of the morphology of industrial graphite nanoplate (GNP) materials on their dispersion in polycarbonate (PC) is studied. Three GNP morphology types were identified, namely lamellar, fragmented or compact structure. The dispersion evolution of all GNP types in PC is similar with varying melt temperature, screw speed, or mixing time during melt mixing. Increased shear stress reduces the size of GNP primary structures, whereby the GNP aspect ratio decreases. A significant GNP exfoliation to individual or few graphene layers could not be achieved under the selected melt mixing conditions. The resulting GNP macrodispersion depends on the individual GNP morphology, particle sizes and bulk density and is clearly reflected in the composite’s electrical, thermal, mechanical, and gas barrier properties. Based on a comparison with carbon nanotubes (CNT) and carbon black (CB), CNT are recommended in regard to electrical conductivity, whereas, for thermal conductive or gas barrier application, GNP is preferred.

15 August 2005 in Solid State Ionics
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Journal Article
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MMM. Marzantowicz
M. Marzantowicz
JDJ.R. Dygas
J.R. Dygas
WJW. Jenninger
W. Jenninger
IAIngo Alig
Ingo Alig

10 September 2008 in Journal of Polymer Science Part B: Polymer Physics
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JXJianjun Xu
Jianjun Xu
MHMarco Holst
Marco Holst
MWMirko Wenzel
Mirko Wenzel
IAIngo Alig
Ingo Alig
Calorimetric studies on a series of anhydride‐cured epoxy resins, in which the epoxy oligomer is a mixture of diglycidyl ether of bisphenol‐A (DGEBA) and diglycidyl ether of poly(propylene glycol) (DGEPPG) in different mole ratios, were carried out. DGEPPG is a flexible epoxy oligomer that was used to tune glass transition temperature for the fully reacted epoxy resin. Conversion versus time curves for the systems with different DGEBA/DGEPPG mole ratios (not including the neat DGEPPG system) were found to overlap with each other in mass‐controlled reaction regime, indicating similar reactivities of epoxy groups in both epoxy oligomers. Onset of diffusion‐controlled reaction regime for different systems was estimated by fitting the conversion versus time data using a phenomenological kinetic equation, as well as from direct comparison of the conversion versus time curves. For the systems (i.e., 0, 10, and 30% DGEPPG) that vitrify during reaction, the crossover from mass‐controlled to diffusion‐controlled reaction occurs close to the onset of the vitrification, where Tg is about 25–30 K below the reaction temperature. For the system (i.e., 50% DGEPPG system) that does not vitrify during the reaction, such crossover still occurs when the Tg of the mixture reaches a value about 25 K below the reaction temperature. © 2008 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 46: 2155–2165, 2008

1 February 2021 in Polymer Testing
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Journal Article
Open access
MSMarkus Schilling
Markus Schilling
UNUte Niebergall
Ute Niebergall
NMNiklas Marschall
Niklas Marschall
IAIngo Alig
Ingo Alig
MBMartin Böhning
Martin Böhning

1 January 1993 in Polymer
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Journal Article
Closed access
GFG. Fytas
G. Fytas
ARA. Rizos
A. Rizos
IAIngo Alig
Ingo Alig
Friedrich KremerFriedrich Kremer
Friedrich Kremer
JRJ. Roovers
J. Roovers